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© 2009 Guy Holt ------- All Rights Reserved ------- May not be reproduced without written permission.
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Introduction
Given the wide variety of generators manufactured for different markets, it is important to understand the benefits and drawbacks to each when it comes to their use in
motion picture production. Especially, given that the increasing use of personal computers and microprocessor-controlled recording equipment in HD production has created
an unprecedented demand for clean, reliable power on set at a time when the trend in lighting is toward light sources that generate dirty power.
The power waveform below left is typical of what results
from the operation of a couple of 1200W HMIs with non-power factor corrected ballasts on a conventional portable generator. The adverse effects
of the harmonic distortion exhibited here, can take the form of overheating and failing equipment, efficiency losses, circuit breaker trips, excessive
current on the neutral wire, and instability of the generator voltage and frequency. Harmonic noise of this magnitude can also damage HD digital cinema
production equipment, create ground loops, and possibly create radio frequency (RF) interference.

Left: Distorted power waveform created by Non-PFC 1200W HMI ballasts on conventional generator.
Right: Near perfect power waveform created by the same lights as part of a new production system.
Why is harmonic distortion suddenly an issue in motion picture electrical distribution systems? First, one must appreciate that the power generation and electrical
distribution systems developed for motion picture production were never designed to deal with an abundance of non-linear loads like the electronic HMI and Fluorescent
lighting ballasts prevalent today. In the past, attention was given to portable generator features such as automatic voltage regulation and speed regulation. But, given the
increasing prevalence
of harmonic currents and the problems they cause, an increasingly more important feature today is the quality of the generated power waveform and how well it interacts
with today's light sources.
As production gets more electronically sophisticated, a thorough understanding of the demands placed on portable generators by such production equipment is necessary in
order to generate power that is clean and reliable. To generate power safely, it is important to understand the grounding requirements of the different types of portable generators.
It is the intent of this article to establish a foundation of knowledge that will enable us to build a new production
system that generates the clean stable set power (seen in the waveform above right) capable of operating larger lights (HMIs up to 6kw or Quartz lights up to 5kw),
or more smaller lights, off of portable gas generators than has ever been possible before. But, before we can begin to build the edifice of this new production system (pictured below),
we must first lay a foundation with the basics of power generation.

Our modified Honda EU6500is with our Transformer/Distro can power the PFC 2.5 & 1.8 HMI Pars, PFC 400w
Lighthouse HMI, 2 ParaBeam 400, 2 ParaBeam 200s, and 2 Tegra 400s of our HD P&P Pkg.
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Table of Contents
(Click to jump to subject. Use "Back Button" to return to Table of Contents)
Generator Basics
Lighting Load Types
Harmonics
Interpreting the Sines
Inverter Generators
A Production System for a New Age
Conclusion
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Generator Basics
Principles of Operation
An electric generator is a device or machine that is used to convert mechanical energy into electrical energy. It is based on the principle of electromagnetic
induction, a scientific law that was discovered by British scientist Michael Faraday and American scientist Joseph Henry in 1831. The principle states that when
an electric conductor, such as a copper wire, is moved through a magnetic field, electric current will flow through the conductor. The mechanical energy of the
moving wire is converted into the electric energy. Faraday and Henry also found that when you move a magnet in a coil of wire, electric current is generated.

A rudimentary electrical generator with static magnets and rotating current carrying coils
A generator produces an Electromotive Force (emf) by changing the number of Magnetic Flux Lines (Lines of Force), passing through a Wire Coil. In the rudimentary
electrical generator illustrated above and below, when the Coil is rotated between the Poles of the Magnet by cranking the handle, an AC Voltage Waveform is produced.

A generator operates on the principle of Electromagnetic Induction, which is defined by Faraday’s Law, which states:

Faraday's Law
The Electromotive Force, (emf) induced in a Coil is proportional to the number of turns, N, in the Coil and the Rate of Change of the number of Magnetic Flux Line passing through the surface (A) enclosed by the Coil. In the rudimentary generator illustrated here, the Coil is under a Stationary Magnetic Field. The Magnetic Flux Density, B, is constant and so Lines of Force is proportional to the Effective Area, Aeff, of the Loop (Lines of Force = B x Aeff.) As the Loop rotates at different angles, there is a change in Aeff which is shown in the illustration below.

Effective Area of the Wire Loop at Different Rotational Angle
The Rate of Change of the Lines of Force is the largest at the zero points of the Waveform and is the smallest at the peaks of the Waveform. Since, an Induced
Effect is always opposed to the cause that produced it, the Induced emf is maximum at the zero points and minimum at the peaks as illustrated below. To see why that is, let’s look more closely at what happens as the loop rotates.

Different Rates of Change of the Magnetic Flux at Various Rotational Angles
In the loop diagrams below, the loop is rotating in a clockwise direction. At position A, the top leg (black) is moving toward the south pole, and the lower leg (white) toward the north pole. In position A, no flux lines are being cut since both legs are moving parallel to the lines of flux. Since no flux is cut, no voltage is induced. In position B, the loop has rotated 1/4 of a turn (90°). The black leg is now moving downward, and the white leg is moving upward. In this position, both legs are cutting across a maximum number of lines of flux, and the emf is maximum. At position C the loop has rotated 1/2 of a turn. The two legs are once more moving parallel to the lines of flux, and again no voltage is induced. At position D, the black leg is moving upward, and white leg downward. Both legs are again cutting a maximum number of lines of force, but in the direction opposite to that of position B. Since the legs are cutting the field in the opposite direction, the emf induced causes the current to flow in the opposite direction. The next 1/4 turn brings the loop back to position A, and the cycle starts over again.

Position of the Rotating Wire Coil Plane to the Magnetic Field Direction and the Induced Electromotive Force
If we were to plot on a graph this induced emf against coil rotation, we would get the sinusoidal waveform that appears below the loop diagrams in the illustration above.
Line X-X' is the zero line. All the area above this line is positive (+), and the area below is negative (-). A careful plotting of induced emf through one rotation of the
coil reveals that a sinusoidal voltage waveform is the natural result of the mechanical motion of a generator’s coils. For example, in position A on the illustration of the
coil rotation, the loop is cutting no lines of force so the induced emf is zero (point 1 on the graph.) One quarter turn later, the loop is in position B. It is cutting a
maximum number of lines of force, so the emf is maximum (point 2 on the graph). At position C, the loop has completed 1/2 of a turn, and no lines of flux are being cut, so
the emf is back to zero at point 3 on the graph. In position D, the loop is cutting the field in the direction opposite to that of position B. The emf induced in the coil i
s maximum, but in the opposite direction (point 4 on the graph). Position E is the same as A, so the loop is ready to start over again. If we were to summarize what happens
during one full rotation of the coil: it starts at zero, rises to maximum in one direction (+), falls back to zero, rises to maximum in the opposite direction (-), and then
comes back to zero. Since, an alternating emf causes the current to flow first in one direction and then the other it is called, Alternating Current, or just plain A.C. A c
omplete rotation is called a Cycle. If the generator coil is made to turn 60 complete rotations in one second, the Frequency of rotation is 60 Cycles per second. If we plot
induced emf against coil rotation at 60 Cycles per second we get the familiar AC voltage sine wave - the Alternating Current (AC) used in commercial electrical power systems.
Generator Anatomy
In order to obtain a larger emf, modern generators use stronger rotating Electromagnets instead of the fixed permanent magnet of our illustration.
The electromagnets are mounted on a shaft (called the Rotor) and rotated within electrical coils (called the Stator.) DC power is used to Excite the electromagnets
of the Rotor. The voltage of the AC output is a function of the level of the excitation of the Rotor’s electromagnets, and controlled by the Exciter.
Illustrated below is the anatomy of a Honda conventional generator. It consists of a stationary Stator and a two pole Rotor that spins inside the Stator.

The Rotor contains magnetic fields which are established and fed by the Exciter. When the Rotor is rotated, electrical current is induced in the armature coils of the Stator.
The voltage of the electrical current generated is proportional to the strength of the magnetic fields, the number of coils (and number of windings of each coil),
and the speed at which the Rotor turns. And, since the Rotor rotation produces different directions to the +/- poles of the magnetic field at different points in
time, the voltage generated is sinusoidal (AC), and each full engine rotation produces one complete AC sine wave. Consequently, the engine must spin the generator
Rotor 3600 RPM to produce the 60Hz AC frequency required in North America (60 cycles/second x 60 seconds/minute = 3600RPM). If, because of varying loads, the
Rotor spins faster or slower, the voltage and frequency of the output vary in step. The quality of the electricity a conventional generator puts out then
is determined by the quality of the engine, how smoothly it runs, and how well the engine is capable of maintaining a constant speed.
The Stator assembly consists of insulated windings (armature coils) positioned near an air gap in the Stator core in which the Rotor rotates. The number and the way the
armature coils are connected determine the phase of the power generated. The Stator of a single phase generator, like the Honda EX5500 illustrated above, has two
sets of armature coils which are spaced 180 degrees apart (a three phase generator has three sets of coils spaced 120 degrees apart.) As illustrated in the wiring schematic below, one end of each coil is
connected to a common neutral terminal. The other end of each coil is connected to separate terminals. Conductors attached to the three terminals (hot, hot,
neutral) carry the current to the generator’s distribution panel (load bus) and on to the electrical load.

Generator Wiring Schematic
As such a single phase generator, like the EX5500, has two separate main power producing circuits. These two circuits supply equal power to the receptacles shown below when the voltage selector switch is in the "120/240V" position. With single phase generators, when the distribution panel has two or more receptacles, you must balance the total load on the generator by dividing the individual loads between the two main power circuits.

For example, the Honda EX5500 is rated for a continuous load of 5000W (41.7A total or 20.8A/main circuit). Now, if receptacle 2 (R2) in the illustration above has a 2k light (a 16.8A load) connected to it and receptacle 3 (R3) has a 1k light (a 8.4A load) connected to it, the total power draw on Main Circuit 1 is 25.2A (greater than the 20.8A capacity of Main Circuit 1). This is a substantial overload to this circuit. Main Circuit 1 is substantially overloaded because both receptacles (R2 & R3) are powered by Main Circuit 1. To eliminate the excessive power draw on Main Circuit 1, the load from receptacle 3 (R3) should be switched to receptacle 1 (R1). Now Main Circuit 1 is powering a 16.8A load (less than 20.8A) and Main Circuit 2 is powering a 8.4A load (less than 20.8A).
In addition to the rotor and stator, a conventional generator has an excitation circuit (illustrated below) that consists of slip rings and brushes attached to the engine shaft (not illustrated.) DC flows from the Exciter, through the negative brush and slip ring, to the rotor field poles to establish the magnetic fields. The return path to the exciter is through the positive brush and slip ring.

Rotor Electromagnet Excitation Circuit
Higher quality portable gas generators, like the Honda EX5500, use an automatic voltage regulator (AVR) as an Exciter. The AVR is an electronic device that
ensures constant voltage output regardless of the load applied to the generator (up to the rated load capacity). The AVR accomplishes this by sensing the
voltage in the stator coils and adjusts the DC excitation current, carried to the rotor electromagnets via the slip rings and brushes, to regulate the field pole
flux to maintain constant voltage at the AC output receptacles.

ILLUSTRATION COURTESY OF HONDA POWER PRODUCTS
In small portable gas generators the generator end (called the alternator) is direct-coupled to the engine to provide smooth operation. Alternator housings are bolted directly to the engine providing precise rotor and
stator alignment.
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Portable Generator Types
What differentiates generators is how they go about regulating the voltage and frequency (Hz) of the AC power they generate through magnetic induction. A generator that is intended to power only the universal motors found in power tools and the incandescent lights found on construction sites requires very little power regulation because their intended loads are very forgiving. Where as, a generator that is intended to power sophisticated electronic equipment that is voltage and frequency sensitive, requires sophisticated and costly power regulation. Where there is a direct trade-off between cost and power quality, the degree to which a generator regulates its power depends upon the requirements of the loads it is intended to power.
For example, since it is less expensive to make a relatively simple generator that will satisfactorily operate most construction equipment and RV appliances (but not sophisticated electronics), there is not the cost/benefit return to warrant the incorporation of the more expensive power regulation controls in generators manufactured for these markets. This explains why there are basically four types of generators available on the market to this day. Given this variety of generators manufactured for different markets, it is important to understand the benefits and drawbacks to each when it comes to their use in motion picture production.
Where what differentiates one type of generator from another is the quality of its’ power it is important to understand the AC power waveform. AC Power is depicted using a sine wave.
The sine wave is a way for us to graphically represent how electricity works. The sine wave is measured using an oscilloscope. The vertical axis represents amplitude (this may be represented in Volts.) The horizontal axis (degrees) represents time and is also known as wavelength. Notice how the voltage sine wave above starts at 0. It then reaches its peak at 90º. This is where the voltage is at its positive maximum. The wave then crosses 0 volts again at 180º (this is called the zero crossover) before peaking again at 270º in the negative and returning to 0 volts at 360º. This process is called a cycle. The frequency of cycles per minute is measured in Hz (Hertz). The standard in North America is 60Hz.

Pure Sinusoidal Power Waveform
A pure sinusoidal voltage, like the one represented above, is a conceptual quantity produced by an ideal AC generator built with finely distributed stator and field windings that operate in a uniform magnetic field. Since in reality neither the winding distribution nor the magnetic field can be uniform in a working AC generator, voltage waveform distortions are created, and the voltage-time relationship deviates from our conceptual pure sine function. The smoother the curve of the sine wave, the more stable the power. Any spikes or "blips" in the curve are caused by a fluctuation in the power. These can be bad for both your generator and the equipment being powered.
Here are the representative waveforms, and brief descriptions, of the four types of generators available on the market today. Given the importance of understanding the benefits and drawbacks to each when it comes to their use in motion picture production we will examine each type of generators, as well as the typical loads they will power on a set, in more detail latter.
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Brushless Generators: Among the most common because of their inexpensive construction, brushless generators have the least reliable voltage control. Brushless generators can't react
quickly to changing loads, either producing low power (a brownout) or high power. Fluctuations of this nature will cause voltage sensitive equipment like HMI lights
to shut off, or will damage sensitive electronics. With a substantual voltage waveform distortion of 23%, brushless generators do not interact well with HMI and Kino Flo ballasts. For this reason brushless generators are only suitable for powering incandescent lighting.
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AVR Generators:
AVR generators feature an Automatic Voltage Regulator designed to consistently control voltage. The AVR keeps the output voltage more or less constant,
regardless of the load. With no large fluctuations in voltage resulting from changing loads, AVR generators will for the most part operate HMI lights
reliably. With older magnetic HMI ballasts, AVR generators require frequency governors to eliminate flicker on film and scrolling in video. With an
appreciable voltage waveform distortion of 19.5%, AVR generators do not interact well with non-power factor corrected HMI and Kino Flo ballasts.
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MSW Inverter Generators:
“CycloConverter”, “Modified Sine Wave”, “Psuedo Sine Wave” are different manufacturer’s trade names for modified square wave inverter generators. These generators
use inverters to produce not a sine wave, but a modified square wave that, depending on their cost, more or less resembles a sine wave. Where the modified square wave is generated from
switching DC power that is converted from the AC power the alternator generates, the power MSW Inverter generators generate is cleaner and more stable than
AVR generators. With a slight voltage waveform distortion, MSW Inverter Generators will interact reasonably well with HMI and Kino Flo ballasts. However,
a modified square wave will cause sensitive electronic equipment (computers, hard drives, video cameras) to overheat. While, equipment that depends on peak
voltage (battery chargers) will not operate as effectively on a modified square wave. For these reasons MSW Inverter Generators are less than ideal for HD
digital cinema productions.
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PWM Inverter Generators:
PWM Inverter Generators operate like MSW Inverter Generators, but use a sophisticated pulse width modulation (PWM) logic to control a micro processor to switch IGBTs at high
speeds to produce a near pure sine wave from the DC power that is converted from the AC power of the generator alternator. With a negligible voltage waveform distortion of 2.5%
(less than grid power), PWM Inverter Generators interact well with HMI and Kino Flo ballasts. These units are ideal for sensitive electronics, such as computers, audio, and
video recording equipment. PWM Inverter Generators offer a number of other benefits, including less noise, lower weight, and greater fuel efficiency as compared to conventional
AVR Generators.
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WAVEFORMS COURTESY OF HONDA POWER EQUIPMENT
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Conventional Portable Generators
A conventional generator rotates two electro-magnets (energized wire coils) inside its stator core. Since the rotation produces different directions to
the +/- poles of the magnetic field at different points in its circular motion, the voltage generated is sinusoidal (AC), and each full engine
rotation produces one complete ac sine wave. By design, the engine must spin the generator rotor 3600 RPM to produce an AC frequency of 60 Hz
(60 cycles/second x 60 seconds/minute = 3600RPM). If, because of varying loads, the generator spins faster or slower, the voltage and frequency of the output
vary in step. The quality of the electricity a conventional generator puts out then is determined by the quality of the engine, how smoothly it runs, and how well
the engine is capable of maintaining a constant speed.
Brushless Generators
Among the most common because of their inexpensive construction, brushless generators have the least reliable voltage control of all generators. The drawback to brushless generators in motion picture lighting applications is that they don't react quickly to changing loads. When a new load (light) is switched on, a brushless generator will alternately produce low voltage (a brownout) and then high voltage (a surge) as the engine slows down under the additional load, and then speeds ups again, before stabilizing under the greater load.
Fluctuations of this nature can result in the following scenario we have all probably experienced at one time or another when trying to run multiple HMI lights with conventional portable generators. After turning on the first HMI light, you switch on a second light. The striking of the HMI arc creates a surge in the power load, this causes momentary engine instability, which results in a dip in output voltage. The dip in voltage causes both HMI lamps (the one already running and the one striking) to cut out. When, within seconds, the engine stabilizes again, the power comes back up to full, which causes the HMI light that cut out to hot-restrike (because the ignition switch is still on.) But, because the lamp is hot, the strike doesn’t take. The striking voltage returns to the ballast and fries delicate electrical components in the ballast. As this nightmare scenario demonstrates, the voltage fluctuation of brushless generators are sufficient to cause voltage sensitive equipment, like HMI lights to shut off, for this reason brushless generators are really only suitable for powering incandescent lighting and not much else.
Another problem with brushless generators is that the power they generate exhibits significant voltage waveform distortion (see waveform above). With an applied voltage waveform distortion of upwards of 23%, brushless generators do not interact well with HMI and Kino Flo ballasts, causing harmonic currents to be thrown back into the power stream, which results in a further degradation of the voltage waveform (more on that latter.)
Automatic Voltage Regulated (AVR) Generators
To be suitable for filming with all types of HMI ballasts, conventional generators must employ governor systems to maintain constant voltage (V) and AC Frequency (Hz).
To avoid the nightmare scenario described above when striking multiple small HMIs (less than 1200W), a portable generator must have an Automatic Voltage Regulator or AVR. An AVR keeps the output voltage more or less constant, regardless of the load. It accomplishes this by first monitoring the output voltage. It then compares it with the desired set value and corrects any error by suitably changing the field excitation current. By constantly adjusting the excitation to the brushes to increase or decrease the output voltage, the AVR ensures a more or less consistent flow of power regardless of the load. Under normal circumstances an AVR system can ensure a voltage that is within ±3% of the mean voltage. In this fashion, AVR systems eliminate surges and brown-outs that would otherwise occur when switching on and off small movie lights (both HMI & Quartz.)
Unfortunately, given the size of portable generators (usually less than 7000W) relative to common motion picture lighting loads (upwards of 2000W),
even the best AVR systems are still not responsive enough to always handle the changes in load created when switching on larger motion picture lights.
Where the load placed upon the generator by a 1200W HMI (which draws anywhere from 13.5-19 Amps depending on the type of ballast), or a 2000W Quartz
light (which draws 16.8 Amps) can account for 30-60 percent of the capacity of the generator, the generator’s AVR system is more often than not simply
overwhelmed. For this reason (and others), the general rule of thumb when using conventional AVR generators is to oversize the generator by a factor
of 2 to 1 relative to your total load. It also helps to use more small lights than just a few large lights.
The second type of governor system a portable generator must have to be suitable for lighting with all HMI ballasts, as well as sophisticated electronic production equipment like laptops, hard drives, and HD monitors, is a AC Frequency governor.
Broadly speaking, HMI ballasts now come in two varieties. They are magnetic ballasts and electronic square wave ballasts, also called flicker free ballasts. For the purpose of this discussion, I will not refer to electronic square wave ballasts as flicker free, because that implies that magnetic ballasts generate flicker, which they do not under controlled circumstances. To avoid “flicker” with magnetic HMI ballasts operating on conventional generators, the generator speed must be tightly governed. The need for such tight control of the AC frequency has to do with the fact that HMI lights are inherently arc lights whose output pulsates.
If you were to look at an HMI globe, instead of a coiled tungsten filament glowing, you would find an electrical arc spanning the gap between two opposing electrodes. On the most fundamental level, a magnetic HMI ballast is simply a variable transformer choke between the power supply and the lamp electrodes. The transformer provides the start-up charge for the igniter circuit, rapidly increasing the potential between the electrodes of the head’s arc gap until an electrical arc jumps the gap and ignites an electrical arc between the lamp electrodes. The transformer then shifts gear and acts as a choke, regulating current to the lamp to maintain the pulsating arc once the light is burning.
As such, the light intensity of a HMI powered by a magnetic ballast follows the waveform of the supply power and increases and decreases 120 times a second, twice every AC cycle. This fluctuation in the light output is not visible to the eye but will be captured on film or video if the frequency (Hz) of the AC power is not precisely synchronized with the film frame rate or video scan rate. If the AC Frequency of the power were to vary, a frame of film or video scan, would receive more or less exposure depending upon the exact correspondence of the film/video exposure interval to the cycling power waveform because the light intensity is pulsating at twice the AC frequency.

ILLUSTRATION COURTESY OF HARRY BOX
The normal sinusoidal 60Hz current of a magnetic ballast (left) creates a fluctuating light output (right) requiring that the camera frame rate be synchronized with the light fluctuations to obtain even exposure frame to frame.
In film production with magnetic HMI ballasts (as opposed to video), to avoid this flicker, you must also use a crystal controlled camera, run the camera at one of a number of safe frame rates (those that can be divided into 120 and result in a whole number), and use power that is regulated at exactly 60 Hz +/- a quarter cycle (59.75 Hz - 60.25 Hz).

The problem one encounters when operating magnetic HMI ballasts on conventional generators is that by design the AC frequency they generate is a function of engine speed and their speed fluctuates. As the generator spins faster or slower, the frequency of the output varies in step. For this reason, when filming with magnetic HMI ballasts, a separate governor is required to ensure that the engine spins its’ core at a near constant 3600 RPM to produce the desired AC Frequency of 60 Hz (60 cycles/second x 60 seconds/minute = 3600RPM).

A Barber Coleman AC Frequency Governor in a Honda EX5500
An AC Frequency governor accomplishes this by first monitoring the engine speed, it then compares that reference signal with an internal quartz crystal reference, and corrects any error by adjusting the engine throttle through a mechanical linkage (see picture above.) By constantly adjusting the engine speed in this fashion the governor ensures a more or less stable 60 Hz AC Frequency. It is worth noting here, for the purpose of our latter discussion regarding the adverse effects of power waveform distortion, how the governor system obtains its’ engine speed reference.
Larger generators that are designed to take AC frequency governors, have a magnetic pick up that senses the rotation of the core. However, since the AC frequency governors for portable gas generators are after market modifications, the engine speed reference signal is obtained by measuring the frequency of the output voltage inside the AVR unit. By sensing the zero-crossing information from the waveform, the AC frequency governor can precisely regulate the engine speed and in theory eliminate erratic exposure of film frames or video scans.
In practice, AC governor systems work well in small portable generators only if the generator is well maintained, finely tuned, and carefully prepped for each shoot. The carburetors of small generator engines are easily gummed up by old fuel making them run rough. For this reason, it is important to bleed old fuel from the system and replace it if the generator as been sitting idle for an extended period of time. A second maintenance issue is that the generator battery must be at full capacity as well as fully charged. The reason for this requirement is that the battery charging system of the generator was not designed for the additional electrical load of the AC Frequency governor. If the generator battery is not at full capacity and fully charged, the AC Frequency governor eventually runs the battery down to the point that it can no longer regulate the engine because it is underpowered. Unfortunately, more often than not, the generators coming out of rental houses are poorly maintained and inadequately prepped making the AC governor system ultimately unreliable.

ILLUSTRATION COURTESY OF HARRY BOX
The refined square-wave signal of an electronic ballast (left) creates virtually even light output (right)
When electronic square wave HMI ballasts came on the market, they were at first thought to be the solution to all the problems inherent in running HMI lights on small portable generators. By eliminating the flicker problem associated with magnetic ballasts, they also eliminated the need for the expensive and ultimately unreliable AC governors required for flicker free filming with magnetic HMI ballasts and portable gas generators. Electronic square wave ballasts eliminate the potential for flicker by squaring off the curves of the AC sine wave supplying the globe. Squared off, the changeover period between cycles is so brief that the light no longer pulsates but is virtually continuous. Even if the AC Frequency of the power were to vary, a frame of film or video scan, would receive the same exposure because the light intensity is now not pulsating but nearly constant. Electronic square wave HMI ballasts allow you to film at any frame rate and even at a changing frame rate.
Since they are not frequency dependent, it was thought at first that electronic square wave ballasts would operate more reliably on small portable generators – even those without frequency governors. For this reason, as soon as electronic square wave ballasts appeared on the market, many lighting rental houses replaced the more expensive crystal governed portable generators with less expensive non-synchronous portable generators. The theory was that an electronic square wave ballast would operate reliably on a non governed generator and allow filming at any frame rate, where as a magnetic HMI ballast operating unreliably on a AC governed generator allowed filming only at permitted frame rates.
In practice, electronic square wave ballasts turned out to be a mixed blessing. Part of the problem with operating electronic HMI ballasts on portable gas generators in the past has to do with the purity of the power waveform they generate. With an applied voltage waveform distortion of upwards of 19.5%, conventional AVR generators do not interact well with electronic HMI ballasts, causing harmonic currents to be thrown back into the power stream, which results in a further degradation of the voltage waveform and ultimately to equipment failure or damage (more on that latter.)
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Inverter Generators
A conventional generator, one that runs at 3600 RPM, makes a pretty decent sine wave. This is because it generates power by rotating two large coils in a magnetic field, and as discussed above, sine waves are a natural product of rotating machinery. However the power that conventional generators produce is considered “dirty” power.
ILLUSTRATION COURTESY OF KIRK KLEINSCHMIDT

Waveform of power output by conventional generator. Note the frequency error and noticeable distortion
Measured on an oscilloscope (pictured above), its’ sine wave appears jagged. Those small spikes in the sine wave indicate noise that can cause HMI lights to act erratically and cause problems for sophisticated electronics, like video cameras, monitors, computers, and hard drives that need a clean sine wave to operate. With the increasing use of personal computers and microprocessor-controlled recording equipment in motion picture production, the demand for clean, reliable power has reached new heights.

ILLUSTRATION COURTESY OF HARRY BOX
Step 1: Rectifier Bridge converts multi-phase AC power to rectified sine wave. Step 2: rectified sine wave is flattened to DC. Step 3: micro processor switching alternates wave polarity creating a modified square wave.
Inverter generators meet this demand for cleaner power by adding an additional component that completely processes the “dirty” AC power from the generator’s alternator. An inverter
module takes the raw power produced by the alternator and passes it through a microprocessor controlled multi-step process to condition it. But, rather than using simple two pole cores,
the alternators of inverter generators use multi-pole cores and small stators to produce a raw AC power that is multiphase (more than 300 overlapping sine waves), high frequency
(up to 20’000 Hz), and upwards of 200 Volts. This high voltage AC power is then converted to DC. Finally the DC power is converted back to low voltage single phase AC power by an inverter.
In the process the inverter cleans and stabilizes the power.
Not all inverter generators are equal (Modified square wave verses true sine wave inverters.)
There are 3 major types of inverters used in generators - sine wave, modified square wave, and square wave. One might wonder why there are so many types of inverters.
As John De Armond, explains in his informative article "The “Hows” and “Whys” of Inverters and Inverter Generators" the primary reason is cost. To paraphrase John's article,
to make a nice sine wave from DC power is expensive. There is a trade-off between cost and waveform purity. An approximation of a sine wave
may be created by outputting one or more stepped square waves with the amplitudes chosen to approximate a sine (a modified square wave). The more steps, the more like a
sine wave the output is. However, each of the voltage steps requires its own voltage supply, its own transistor switch, plus the necessary control circuitry. The bottom
line is that the more steps, the more expensive the inverter. The two go hand in hand.

ILLUSTRATION COURTESY OF JOHN DE ARMOND
Ideal Sine Wave (black), Single Step Square Wave (blue), Three Step Square Wave (red)
Take a look at the figure above. The black trace is, of course our ideal true sine wave. The blue wave is a single step approximation or square wave. The red wave is a three step wave or modified square wave. As is intuitive, the three step wave produces a closer approximation of a sine wave and thus will satisfactorily operate more devices than the single step one. The tradeoff is cost and complexity

ILLUSTRATION COURTESY OF JOHN DE ARMOND
Switch sequence of three step output stage of a modified square wave inverter.
The figure above is a line drawing of a typical three step output stage of a modified square wave inverter. The voltages V1 through V3 are increasingly higher DC voltages
converted from the AC power generated by magnetic induction. A microprocessor generates the pseudo sine wave (modified square wave) by sequentially switching S1 through
S3 on, S3 through S1 off, S4 through S6 on, S6 through S4 off. It repeats this 60 times a second. Where each of the voltage steps requires its own voltage supply, its
own transistor switch, plus the necessary control circuitry, one can intuit that the more steps in the modified square wave, the more complicated and thus more expensive
the inverter is.
Where it is less expensive to make a modified square wave that will satisfactorily operate most construction equipment and RV appliances, than it is to make a true sine
wave there is not the cost/benefit return to warrant the incorporation of the more expensive true sine wave inverters in generators manufactured for these markets. This is
why there are still three types of inverter generators available on the market to this day.
Advantages and Disadvantages:
Square Wave Generators
While a square wave inverter will run simple things like tools with universal motors with no problem, they will not operate much else. For this reason, generators with square wave
inverters are now found only in the construction trades, where they offer the benefit of being cheaper, smaller, lighter, and running longer on a gallon of gas than conventional
generators. For reasons I will explain below, square wave inverter generators have no application in motion picture production.
Modified Square Wave Generators
“Modified Sine Wave”, “Psuedo Sine Wave”, and “Cycloconverter” are all sales terms used for a modified square wave type of AC power. Modified square wave inverters are low in cost, slightly more efficient than conventional generators, and will satisfactorily operate almost all common household appliances and power tools. For this reason, they are typically used in the economy RV/Residential Standby and Industrial lines of generator manufacturers.
Where the modified square wave is generated from switching DC power that is converted from the AC power the alternator generates, the power MSW Inverter generators generate is cleaner
and more stable than AVR generators. With a slight voltage waveform distortion, MSW Inverter Generators will interact reasonably well with HMI and Kino Flo ballasts. However, a
modified square wave will cause sensitive electronic equipment (computers, hard drives, video cameras) to overheat. While, equipment that depends on peak voltage (battery chargers)
will not operate as effectively on a modified square wave. For these reasons MSW Inverter Generators are less than ideal for HD digital cinema productions. John De Armond, clearly explians
why that is the case using one of the more rudimentary inverter generators, the simple three step modified square wave discussed above, as an example in his article
"The “Hows” and “Whys” of Inverters and Inverter Generators".

ILLUSTRATION COURTESY OF JOHN DE ARMOND
Output waveform of a Honda EX350 square wave inverter generator
The photo above is an oscilloscope shot of the actual output of an older Honda EX350 modified square wave inverter generator. Notice the RMS voltage indication on the right side - 120 volts even though the peak voltage is only 142 volts. For a true sine wave, the peak voltage would be 120 * 1.414 = 169 volts. This difference in peak voltage is what makes or breaks the operation of modified square wave inverter generators in motion picture production applications where they work fine on construction sites.

ILLUSTRATION COURTESY OF JOHN DE ARMOND
Voltage and the current output waveforms of a Honda EX350 square wave inverter generator powering 300W incandescent light
The photo above shows a scope shot of both the voltage and the current output of this generator driving a 300 watt incandescent light (a resistive load.) As you see, a modified
square wave works well for a resistive load like an incandescent light. Things get a whole lot more interesting when one connects a fluorescent lamp to the
generator. As you can see in photo below the solid-state ballast of the fluorescent lamp slightly distorts the voltage waveform (creates a spike) and creates
all kinds of current oscillation. This kind of harmonic activity can cause a noticeable audio buzz, equipment to malfunction, or shut off (more on harmonic noise latter.)

ILLUSTRATION COURTESY OF JOHN DE ARMOND
Voltage and the current output waveforms of a Honda EX350 square wave inverter generator powering fluorescent light
Another common problem with modified square wave generators like the Honda EX350 is encountered when they are used to charge batteries on remote sets without grid power. John De Armond
illustrates the problem in his informative article "The “Hows” and “Whys” of Inverters and Inverter Generators" by first examining how the battery charger works on grid power when plugged
into a conventional outlet.
To paraphrase him a battery charger typically consists of a transformer, a rectifier and support electronics like charge control circuitry. On each half-cycle of the 60 hz line voltage, the voltage first increases and then decreases in the shape of a sine. The transformer secondary of the battery charger follows this voltage. Connected to the secondary is the rectifier that converts the AC to DC for battery charging. Only when the instantaneous AC voltage exceeds the battery voltage plus the 0.7 voltage drop of the rectifier does current flow to charge the batteries. Photo 5 illustrates this effect. The two lines at “1” and “2” mark on the voltage sine wave where the rectifier starts conducting and causing current to flow.

ILLUSTRATION COURTESY OF JOHN DE ARMOND
Problems arise when a charger of this type is connected to a modified square wave inverter. Recall from the first photo above that the peak voltage of a modified square wave
does not rise as high as a sine wave (142 volts verses the 169 volts of a true sine wave.) The horizontal line in the photo above shows about where the square wave would reach. In
this particular case, the square wave would never reach a voltage sufficient to make the rectifier conduct and so the battery would never charge even though power is connected, the LED indicators light up, and a true RMS voltmeter would indicate about 120 volts. This is another fundamental problem with modified square wave inverters in production applications.
Audio/video production equipment, computers, and battery chargers require a nearly pure (low distortion) sine wave input. If these devices are to be run from an inverter generator, then the generator’s inverter module must supply a sine wave or something pretty close to it. As discussed, inverters of this sophistication are appreciatively more expensive - from 2 to 3 times - because of the number of and prohibitive cost of high power electronic switch devices and components required. However, recent rapid developments in the field of IGBT (insulated gate bipolar transistors) electronics and miniaturization/mass production of microprocessor based digital control systems have reached the stage that Pulse Width Modulation (PWM) inverter modules are economically viable and affordable. Still not as cheap as modified sine wave inverter modules, generator manufacturers only put Pulse Width Modulation (PWM) inverter modules in their deluxe or Super Quiet product lines. For instance, the Honda super quiet EU series of generators employ Pulse Width Modulation (PWM) inverter modules with a waveform distortion factor of less than 2.5% - which is considerably better than conventional generators and quite often better than what you get out of the wall outlet.
True Sine Wave Generators
Pulse width modulation (PWM) inverters provide a more sinusoidal current and for that reason are commonly called true sine wave inverters. Pulse Width Modulation (PWM) inverters use micro-processor control modules to produce AC power with a "true" sine wave (with full width and amplitude) from high voltage DC power converted from the AC power generated by magnetic induction in the core of the generator. PWM inverters are more efficient and typically provide higher levels of performance.

ILLUSTRATION COURTESY OF KIRK KLEINSCHMIDT
Waveform of power output of PWM inverter generator. Note there no discernable distortion or frequency error.
The "true" sine wave these generators deliver is more suitable for computers, solid-state equipment with built-in computer functions or microcomputer-controlled
functions. Unlike the simple two-pole alternators of AVR generators, an inverter generator uses a core that consists of multiple stator coils and multiple rotor magnets.
Each full rotation of the engine produces more than 300 three phase ac sine waves at frequencies up to 20 kHz, which is considerably more electrical energy per
engine revolution than produced in conventional two pole AVR generators.

PHOTO COURTESY OF SUBARU/ROBIN POWER PRODUCTS
Core parts from PWM Inverter Generator. Note the multiple windings of the core stator.
The power generated by the multi-pole core next goes to the inverter module. A basic PWM inverter consists of a converter, DC link, control logic, and an inverter.

Basic wiring schematic of PWM Inverter
The converter section consists of a fixed diode bridge rectifier
which converts the more than 300 three phase ac sine waves at frequencies up to 20 kHz to a DC voltage (about 200 V in at least one unit).

Converter and DC Link
AC Output is then generated from the high voltage DC by the inverter section with voltage and frequency set by a PWM control logic. A
highspeed microprocessor switches IGBTs (insulated gate bipolar transistors) on and off several thousand times a second according to the PWM control logic to
create a variable voltage and frequency.

Control logic and Inverter Section
PWM inverter control logic goes something like this: to generate the positive half cycle of a true AC sine wave, an IGBT connected to the positive value of the DC voltage from the converter is switched on and off by a micro-processor at variable rates and for variable intervals to create current to flow of a variable voltage.
ILLUSTRATION COURTESY OF SIEMENS CORP.

PWM Voltage and Current
In other words, the IGBT is switched on for a short period of time,
allowing only a small amount of current to build up and then is switched off. The IGBT is switched on and left on for progressively longer periods of time, allowing current to build up to higher levels until the current reaches a peak. The IGBT is then switched on for progressively shorter periods of time, decreasing current. The negative
half of the AC sine wave is generated by switching an IGBT connected to the negative value of the converted DC voltage. The fixed DC voltage (200 VDC) is modulated or clipped in this fashion to provide a variable voltage and frequency.
Where IGBTs can turn on in less than 400 nanoseconds and off in approximately 500 nanoseconds, they are ideal for the high switching speed necessary to create a true sine wave in this fashion.
The fixed DC voltage (200 VDC) is modulated or clipped in this fashion to provide a variable voltage and frequency.

ILLUSTRATION COURTESY OF KIRK KLEINSCHMIDT
The three phases of the inverter generator process: high frequency AC converted to DC; DC inverted to stable clean 120V, 60 Hz AC.
To summarize this complex process: the generator's multi-pole core produces high voltage multiphase AC power. The AC power is then converted to DC. Finally the
DC power is converted back to AC by an inverter. Since the inverter completely processes the raw power generated by the alternator, the voltage and frequency of the power it generates is no longer linked to engine speed (RPM) as is the case with conventional AVR generators.
Rather, using microprocessor controlled IGBTs the inverter module switches the high voltage DC according to PWM control logic to provide AC power with a voltage
stability within ± 1%, and frequency stability within ± 0.01 HZ. The end result is a nearly pure sine wave with a wave distortion of only 2.5%; which, is as clean or cleaner than
commercial power.
As discussed above, developments in this direction began a long time ago, but a techno-economical solution could not be found to manufacture true sine wave inverters until recently because of the prohibitive cost of high power electronic devices and components. However, recent rapid developments in the field of IGBT electronics and miniaturization/mass production of microprocessor based digital control systems have reached the stage that Pulse Width Modulation (PWM) inverter modules are economically viable and affordable.
__________________________________________________________________
Lighting Load Types
All loads are not created equal
All lighting loads are not the same. Incandescent, Fluorescent, LED, and HMI lights fall into two broad categories. Those that are linear loads and those that are non-linear
loads. Non-linear loads further break down into two categories: those that exhibit high inductive reactance (magnetic HMI ballasts) and those that exhibit high capacitive
reactance (electronic HM, Fluorescent, & LED ballasts). Because each type of load has an effect (mostly adverse) on the power supply, their individual characteristics are worth
exploring in more detail. Even more so, because they adversely affect generated power more than they do grid power.
Linear Loads
Incandescent Lights (Purely Resistive Loads)
An incandescent light is a simple resistive load. The high resistance of its tungsten filament creates heat until the filament glows - creating light. The current in such a simple
resistive AC circuit increases proportionately as the voltage increases and decreases proportionately as the voltage decreases. Changes in alternating current (AC) and the
relationship between voltage and current in a purely resistive circuit (Incandescent Lights) can be represented graphically by the sine waves below.

Unity Power Factor: Voltage & Current are in Phase.
For a sinusoidal voltage, the current is also sinusoidal. For a purely resistive load like incandescent lights, the current is always proportional to the voltage. The voltage and current are in phase and so have a Power Factor of 1 or unity power factor (power factor will be explained in detail below.)
Non-Linear Loads
HMI Lights with Magnetic Ballasts
The make up of a magnetic HMI ballast is relatively simple by comparison to the newer electronic HMI ballasts. Between the power input and the lamp is a transformer that acts as a choke coil. The transformer provides the start-up charge for the igniter circuit, rapidly increasing the potential between the electrodes of the head’s arc gap until an electrical arc jumps the gap and ignites an electrical arc between the lamp electrodes. The transformer then acts as a choke, regulating current to the lamp to maintain the pulsating arc once the light is burning.
As such, the light intensity of an HMI follows the power waveform and increases and decreases 120 times a second, twice every AC cycle. This fluctuation is not visible to the eye but will be captured on film or video as a steady pulsation if the camera is not in precise synchronization with the AC power frequency. With magnetic HMI ballasts, to avoid this flicker, you must use a crystal controlled camera, run the camera at one of a number of safe frame rates (those that can be divided into 120 and result in a whole number), and use power that is regulated at exactly 60 Hertz (cycles per second.)

Transformers of a 12k Magnetic HMI Balllast
Essentially a large coil of wire that is tapped at several places to provide for various input voltages and a high start-up voltage, the transformers of magnetic HMI ballasts
exhibit high self-inductance. Self-inductance is a particular form of electromagnetic induction that inhibits the flow of current in the windings of the ballast transformer,
pulls the voltage out of phase with the current, and reduces the power efficiency (power factor) of the ballast. Because the high self-inductance inherent in magnetic HMI
ballasts adversely effects the power generated by small portable generators, it is a topic worth exploring in more detail.
Self-Inductance
Self-inductance is defined as the induction of a voltage in a current-carrying wire within a coil when the current in the wire itself is changing as it
alternates. Taking a close look at a simple circuit with a coil will help us to understand how voltage is induced by changing current. The alternating
current running through a coil creates a magnetic field in and around the coil that is increasing and decreasing as the current alternates. The magnetic
field forms concentric loops that surround the wire and join to form larger loops that surround the coil as shown in the image below. When the current
increases in one loop the expanding magnetic field will cut across some or all of the neighboring loops of wire, inducing a voltage in these loops. This
voltage causes a current to flow in the windings of the coil.
ILLUSTRATION COURTESY OF THE NDT RESOURCE CENTER

Magnetic fields created in and around a coil with alternating current running through it.
By studying this image of a coil, it can be seen that the number of turns in the coil will have an effect on the amount of voltage that is induced into our
simple circuit. Increasing the number of turns or the rate of change of magnetic flux thereby increases the amount of current induced. The current induced
by this voltage has a direction such that its magnetic field opposes the change in magnetic field that induced the current. Or, in other words, the current
induced in a conductor will oppose the change in current that is causing the flux to change.
Inductive Reactance
By taking an even closer look at a coil of wire it can be seen how induction reduces the flow of current in our simple circuit. In the image below, the direction of the primary current is shown in red, and the magnetic field generated by the current is shown in blue. It can be seen that the magnetic field from one loop of the wire will cut across the other loops in the coil and this will induce current flow (shown in green) in the circuit.
ILLUSTRATION COURTESY OF THE NDT RESOURCE CENTER

Induced current works against the primary current in a coil.
Note that the induced current flows in the opposite direction of the primary current and accomplishes no actual work other than to create energy circulating back and forth between the coil and the power source. The induced current working against the primary current results in a reduction of current flow in our simple circuit. This opposition to the flow of current is called inductive reactance.
Since inductive reactance reduces the flow of current in a circuit, it appears as an energy loss just like resistance. However, it is possible to distinguish between resistance and inductive reactance in a circuit by looking at the timing between the sine waves of the voltage and current of the alternating current. As we saw above, in AC circuits with resistive loads, the voltage and the current are in-phase, meaning that the peaks and valleys of their sine waves occur at the same time. When there is inductive reactance present in the circuit, the phase of the current will be shifted so that its peaks and valleys do not occur at the same time as those of the voltage. As illustrated below, inductive reactance causes current to lag behind the voltage. The degree to which the two waveforms are put out of phase depends on the relative amount of resistance and inductance offered by the coil.

Poor Power Factor: Voltage & Current are in out of phase.
As we saw in our simple circuit above, the number of turns in the coil will have an effect on the amount of voltage that is induced into the circuit. Increasing the number
of turns increases the amount of induced voltage. In the case of a magnetic HMI ballast, the multiple fine windings of the ballast transformer induces appreciable voltage
and considerable current that is in opposition to the primary current, causing the primary current to lag behind voltage, a reduction of current flow, and an inefficiency
in the use of power supplied by the generator. Put simply, the ballast draws more power than it uses to create light. Capacitors are typically included in the design of
magnetic HMI ballasts to compensate for the high inductance of the transformer and to bring the current back in phase with the voltage.
Apparent Power Verses True Power = Power Factor
If, in this situation, you were to measure the current (using a Amp Meter) and voltage (using a Volt Meter) traveling through the cable supplying the magnetic HMI ballast and multiply
them according to Ohm’s Law (W=VA) you would get the “apparent power” of the ballast. But, if you were to instead, use a wattmeter to measure the actual amount of energy being converted
into real work (light) by the ballast, after the applied voltage overcomes the induced voltage, you would get the “true power” of the ballast. The ratio of “true power” to “apparent power”
is called the “power factor” of the ballast.
The favorite analogy electricians like to use to explain power factor is that if apparent power is a glass of beer, power factor is the foam that prevents you from filling it up all the way.
When lights with a low power factor are used, a generator must be sized to supply the apparent power (beer plus foam), even though only the beer (true power) counts as far as how much actual
drinking is possible. Where a typical 1200W magnetic HMI ballast takes 13.5 Amps at 120 Volts to generate 1200 Watts of light the power factor is .74 (13.5A x 120V= 1620W, 1200W/1620W= .74).
Capacitive Reactance
Electronic HMI, Fluorescent, & LED ballasts belong to a category of power supplies, called Switch Mode Power Supplies (SMPSs), that exhibit another type of opposition to the flow of current that is called Capacitive Reactance. SMPSs utilize electronic components that use only portions of the AC power waveform. These devices then return the unused portions as harmonic currents that stack on top of one another, pull the voltage and current out of phase, and under the wrong conditions create distortion of the voltage waveform.

As illustrated in the wiring schematic above, all SMPSs consist of first a diode-capacitor section (consisting of a Bridge Rectifier and Smoothing
Capacitor) that converts the AC input power to DC power; and then, in the case of HMI & Fluorescent lights, a Switch-mode Converter section that converts the DC power back
to an alternating power waveform that ignites the lamp. In the case of High Output AC LED ballasts, the Switch Mode Converter further conditions the DC power the diode-capacitor section outputs. How HMI and Fluorescent ballasts differ as SMPSs is by the shape and frequency of the alternating power waveform the Switch-mode converter
generates. In the case of electronic HMI ballasts the Switch-mode converter generates a low frequency (60Hz) square wave. In the case of electronic Fluorescent ballasts,
the Switch-mode converter generates a high frequency (>20kHz) sine wave.
Regardless of what circuits are in the green box in the illustration above, all SMPSs utilize a diode-capacitor
section to first convert the AC line input power to DC power. The diode-capacitor section of a SMPS is the source of the capacitive reactance that opposes the flow of current
and contributes to its’ poor power factor.
ILLUSTRATION COURTESY OF HARRY BOX

The capacitive reactance of SMPSs act on power in a way opposite to inductive reactance. It causes current to lead voltage. SMPSs typically have a power
factor less than .6, meaning that the ballast (whether HMI, Fluorescent, or LED) has to draw 40% - 50% more power than it uses. Where capacitive reactance
leads to an inefficient use of power (lots of foam, not much beer), and the harmonic currents generated can have adverse effects on other equipment
operating on the same power, it is worth exploring the cause of capacitive reactance and the source of the harmonic currents in more detail.
To understand the cause of the capacitive reactance of SMPSs, and it’s effect on the power supply, let’s look first at the operation of fluorescent
ballasts in more detail.
Fluorescent Lights (Electronic vs. Electromagnetic Ballasts)
The ballast of a fluorescent light functions very much like an HMI ballast. It provides the lamp with high voltage during start-up to ignite an arc between the lamp electrodes, and then stabilizes the arc by limiting the electrical current to the lamp. As in the case of HMI lights, there are two basic types of fluorescent ballasts: magnetic and electronic.
A magnetic fluorescent ballast works very much like a magnetic HMI ballast. It uses a magnetic transformer of copper windings around a steel core to convert the input line voltage and current to the voltage and current required to start and operate the fluorescent lamp. Like magnetic HMI ballasts, they exhibit high inductive reactance and have a poor power factor. The power factor of magnetic ballasts is usually less than .5 and they typically account for 18% to 35% of total harmonic distortion in the power supply of offices where they are commonly used. Like magnetic HMI ballasts, the output frequency of a magnetic fluorescent ballast is the same as the input AC line frequency (60 Hz), which means that (as was the case with an HMI magnetic ballast) the camera frame rate must be synchronized with the AC frequency of the power supply in order to avoid the appearance of light intensity fluctuation in the image.
For this reason fluorescent lights were seldom used in motion picture production until the advent of high frequency electronic ballasts for fluorescent lamps.
Fluorescent Lights with Electronic Ballasts
Electronic fluorescent ballasts are a Switch-mode Power Supply (SMPS) designed to perform all the same functions as a magnetic ballast but at a higher frequency. They first rectify the 60 Hz AC input to DC and then produce a very high frequency alternating current (20,000 - 50,000 Hz depending on the fixture) using an inverter and power conditioning components.

Kino Flo 4 Bank Select Ballast
The high frequencies at which electronic fluorescent ballasts operate make them a suitable light source for film and television production. By converting the 60 Hz input frequency to between 20,000 - 50,000 Hz, electronic ballasts eliminate the problem of light intensity fluctuation associated with standard magnetic ballasts. At those frequencies the period of time between the off and on pulse of each cycle is so short that the illuminating phosphors do not decay in light output.

Assorted High Frequency Fluorescent Lights Designed for Motion Picture Lighting.
Like the glowing tungsten coil of an incandescent lamp, the fluorescent phosphors become essentially flicker free. Electronic fluorescent ballasts also weigh less and don’t have the characteristic hum of magnetic ballasts. These characteristics of high frequency electronic ballasts make them well suited for motion picture lighting. Developed first by Kino Flo (above), and now available from a number of manufacturers, motion picture fluorescent lights now come in a wide assortment of shapes and sizes.

Assorted CFL Fluorescent Lights Designed for Motion Picture Lighting.
Regardless of its’ shape or size, the ballasts of all high frequency fluorescent lights utilize a Diode-Capacitor circuit to first convert the AC line input to DC. Since it is the Diode-Capacitor circuit of an electronic ballast that generates a high level of capacitive reactance, which leads to an inefficient use of power and the generation of harmonic currents, let us examine how they work in one type of fluorescent light in more detail – the self ballasted Compact Fluorescent Lamp (CFL) pictured below.

CFL Fluorescent Light being tested.
Since the Diode-Capacitor circuit of a self ballasted CFL is similar in design to those in most all fluorescent movie lights (Kino Flo, Lowel, etc.), a close examination of the power factor of CFLs will help us to understand the cause of the capacitive reactance in SMPSs in general, as well as it’s effect on the power supply.

circuit schematic of an Incandescent bulb.
To understand the power factor of a self ballasted CFL bulb it is helpful to compare it to an incandescent bulb. If you will recall from the beginning of
this section, an incandescent light is a simple resistive load (see circuit schematic above.) The high resistance of its tungsten filament creates heat until the filament glows - creating
light. As we see in the oscilloscope shot below, of a 25W incandescent bulb operating on grid power, the current is always proportional to the voltage (current is represented on the scope as the voltage drop on a 1 Ohm resistor.)

Current and Voltage Waveform of a ACEC 25W Incandescent bulb.
If the applied voltage is sinusoidal, the current generated is also sinusoidal. That is, the current increases proportionately as the voltage increases and decreases proportionately as the voltage decreases. Since the peak of the voltage corresponds to the peak in current, the voltage and current are also in phase and so have a unity power factor (Power Factor of 1.)
The voltage and current waveforms, below, of a CFL bulb operating on grid power is very different from that of the incandescent light above. The most
noticeable difference is that the current, generated by the CFL bulb, no longer proportionately follows the nice smooth sinusoidal voltage waveform
supplied to it by the power grid. Rather, it has been distorted by electrical components in the ballast so that it instead consists of sharp spikes
in power that quickly drop off over a short duration. A second distinguishing characteristic is that the peak of the voltage no longer corresponds
to the peak in current. The current now “leads” the voltage by 1.7 milli seconds. The voltage and current are no longer in phase, but instead exhibit
what we call a Leading Power Factor.

Current and Voltage Waveform of a Brelight 25W CFL Bulb.
Like all electronic fluorescent ballasts, the ballasts of CFLs are a Switch-mode Power Supply that converts line-frequency power (60Hz) to a high frequency alternating current.
In the case of self-ballasted CFL bulbs, what is in the green Switch Mode Converter box of the SMPS illustration above, are a pair of MOSFETS (metal–oxide–semiconductor
field-effect transistors) that act as a high frequency DC to AC inverter.
For the purpose of this discussion, what's in the green Switch Mode box, or what the power supply ultimately does with the DC power put out by the diode-capacitor circuit is not
important. What's important is that like all SMPSs, CFL ballasts consist of first a diode-capacitor section that converts the AC input power to DC power. Since, the
capacitive reactance of all SMPSs is caused by this diode-capacitor circuit, how it operates in self-ballasted CFL bulbs and the affect it has on power quality is
representative of SMPSs in general (fluorescent, HMI, & AC LED.)

Typical schematic of CFL electronic ballast: L-to-R consists of half-bridge rectifier, conditioning capacitor, DC/AC Inverter.
The distorted current waveform and Leading Power Factor exhibited by CFLs is caused by the Diode-Capacitor circuit of its’ electronic ballast. To quickly
summarize the cause of this current distortion, the Diode-Capacitor circuit uses only the ascending portion of the supply voltage waveform - which pulls
the current out of phase with the voltage. As seen in this scope shot, it also draws current in quick
bursts, and returns the unused portions as harmonic currents that stack on top of one another creating harmonic distortion of the power waveform.
These harmonic currents, combined with the Leading Power Factor, creates the capacitive reactance that opposes the flow of current in the circuit that
leads to an inefficient use of power by the ballast. Since, the harmonic currents generated can have an adverse effect on other equipment operating on
the same power, it is worth exploring the cause of this capacitive reactance and the source of the harmonic currents in more detail.

Step 1: Rectifier Bridge converts line frequency AC power to rectified sine wave. Step 2: rectified sine wave is flattened to DC by conditioning Capacitor.
Step 3 (not shown): Inverter alternates wave polarity creating a high frequency alternating power to excite lamp gases.
As illustrated above, the diode-capacitor section converts the AC power to DC power by first feeding the AC input current through a bridge rectifier,
which inverts the negative half of the AC sine wave and makes it positive. The rectified current then passes into a conditioning capacitor that
removes the 60 Hz rise and fall and flattens out the voltage - making it essentially DC. The DC is then fed from the conditioning capacitor to the
Switch-mode converter which in the case of a fluorescent ballast is a high frequency inverter that utilizes a pair of MOSFETs to generate the high frequency (20-50kHZ) AC power.

Yellow Trace: Rectifier Bridge converts AC power to rectified sine wave. Blue Trace: Stored Capacitor Voltage. Red Trace: Current drawn by capacitors once input voltage is greater than voltage stored in the capacitor (Blue trace.)
As shown in the illustration above, the diode-capacitor circuit only draws current during the peaks of the supply voltage waveform as it charges the
conditioning capacitor to the peak of the line voltage. Since the conditioning capacitor can only charge when input voltage is greater than its stored
voltage, the capacitor charges for only a very brief period of the overall cycle time. That is because, after peaking, the half cycle from the bridge
drops below the capacitor voltage; which back biases the bridge, inhibiting further current flow into the capacitor. Since, during this very brief
charging period, the capacitor must charge fully, large pulses of current are drawn for short durations. Consequently, electronic fluorescent ballasts
(and SMPSs in general), draw current in high amplitude short pulses. The remaining unused current feeds back into the power stream as harmonic currents.
Given this method of operation, the diode-capacitor circuits of CFLs (and SMPS in general) create two artifacts that can effect power quality adversely. First,
since the conditioning capacitor starts to charge when input voltage is greater than its stored voltage, and stops after the input voltage peaks,
it pulls current out of phase with voltage. As we can see in the oscilloscope shot above, it causes current to lead voltage or creates a "Leading Power Factor."
Second, the unused portions of the voltage waveform that return into the power stream as harmonic currents can have a severe effect on power quality under certain conditions.
Where, it is the combination of a Leading Power Factor and harmonic currents generated by diode-capacitor circuits that constitute the capacitive reactance of SMPS that
opposes the flow of current it is worth exploring the effect of both in CFLs in more detail.

Components of a CFL ballast
These simple diode-capacitor circuits are used in CFL bulbs and in many fluorescent movie lights because they are compact and inexpensive. However, they have a number of
drawbacks. For instance, notice how large the input current spike (red trace above) of the diode-capacitor circuit is. Without power factor correction, the in-put bridge
rectifier requires a large conditioning capacitor at its output. This capacitor results in line current pulses (as seen in our oscilloscope shot above) that are very high
in amplitude. All the circuitry in the ballast as well as the supply chain (the generator, distribution wiring, circuit breakers, etc) must be sized to carrying this high
peak current (the foam in our analogy).

For a rather amusing demonstration of the greater current drawn by SMPSs for the same wattage of light check out this You-Tube video
“Compact Fluorescent
verses The Generator." In this video, lighting designer Kevan Shaw, first operates a 575W ETC Source Four Leko with
Quartz Halogen bulb on an 850W two stroke gas generator without problem. However, when he tries to operate an equivalent wattage of CFLs (30 x 18W bulbs = 540W) the generator goes
berserk. Kevan then turns off the 18W CFL bulbs one at a time until the generator stabilizes. Only after turning off half the CFL Bulbs does the generator operate normally
with a remaining load of 15 - 18W CFLs (270 W.) What accounts for the erratic behavior of the generator in this video under the smaller load of CFLs? It is a combination of the
poor Power Factor of the CFL bulbs and the harmonic currents they generate. Even though the 15 CFL bulbs have a True Power of 270W, the Watt indicator on Kevan's generator
indicates that they draw twice that in Apparent Power (535W), or have a Power Factor of .5 (270W/535W =.504.)
Another drawback to the diode-capacitor circuits used in SMPSs is that when they draw current it is for only a fraction of the half cycle of the voltage waveform.
If we return to the illustration above, we see that the pulses of current are narrow, with fast rise and fall times. Since a diode-capacitor circuit uses only the very
peak of the voltage waveform, they generate high harmonic content as the unused portions of the voltage waveform are returned as harmonic currents (see graph below.)

Distribution of Harmonic Currents generated by CFL bulb
The fast rise time of these current pulses can cause Radio Frequency Interference (RFI) problems. For this reason, Lowel Light warns on their website that their compact fluorescent (CFL) fixture, the Lowel Ego, that: “The lamps may cause interference with radios, cordless phones, televisions, and remote controls. If interference occurs, move this product away from the device or move to a different outlet” (http://www.lowel.com/ego/lamp_info.html.)
Harmonic currents can also stack on top of one another creating excessive current on the distribution system neutral (see below.) And, since the neutral conductor of a distribution system is not fused, it can cause the neutral to overheat and possibly catch fire.

In one study, substituting incandescent lamps with the equivalent wattage of CFLs in a small single phase distribution system substantially increased the current on
the system neutral as a result of the 3rd harmonics generated by the CFL Bulbs.
For this reason, on their website Kino Flo cautions users of their older style fixtures, that the ballasts “will draw double the current on the neutral from what is being drawn on the two hot legs. On large installations it may be necessary to double your neutral run so as not to exceed your cable capacity.” (http://www.kinoflo.com/FYI/FAQs.htm#2"]FAQ “Why is the neutral drawing more than the hot leg.”)
Finally, when the power is supplied by a conventional AVR generator, these harmonic currents can also lead to severe distortion of the voltage waveform in the power distribution
system. When you plug an electronic ballast (fluorescent, HMI, or LED) into a wall outlet you need not be concerned about current harmonic distortion producing voltage distortion.
The impedance of the electrical path from the power plant to the outlet is so low, the distortion of the original applied power waveform so small (less than 3%), and the power
plant generating capacity so large by comparison to the load, that harmonic currents fed back to it will not effect the voltage at the load bus (electrical outlet.) However,
it is an all together different situation when plugging an electronic ballast (fluorescent, HMI, or LED) into a portable generator. In this case, the impedance of the power generating
system (generator and distribution cable) is sufficient enough that a harmonic current will induce a voltage at the same frequency. For example, a 5th harmonic current will
produce a 5th harmonic voltage, a 7th harmonic current will produce a 7th harmonic voltage, etc. Since, as we saw above, a distorted current waveform is made up of the
fundamental plus one or more harmonic currents, each of these currents flowing through an impedance will, result in voltage harmonics appearing at the load bus, a voltage
drop, and distortion of the voltage waveform.
Since electronic ballasts consume current only at the peak of the voltage waveform (to charge the smoothing capacitor), voltage drop due to system impedance occurs only at the peak of the voltage waveform. In this fashion, the pulsed current consumed by electronic ballasts produces voltage distortion in the form of flat-topping of the voltage waveform.

The pulsed current consumed by electronic ballasts produce voltage distortion in the form of flat-topping
The measurement of this distortion is designated as the Total Harmonic Distortion (THD) of the distribution system. While self ballasted CFLs generate the most severe harmonic
noise, all fluorescent ballasts (both magnetic & electronic) generate harmonic noise (see table below.)

The severe voltage waveform distortion exhibited above can cause overheating and failing equipment, efficiency losses, circuit breaker trips, and instability of the generator's
voltage and frequency. In addition to creating the radio frequency interference (RFI) mentioned on the Lowel Light website, harmonic distortion of this magnitude can also
cause component level damage to HD digital cinema production equipment and create ground loops. We will explore how harmonic distortion of the power waveform
adversely effects equipment operating on it in more detail in subsequent sections, but first lets continue our survey of lighting loads with electronic HMI ballasts.
HMI Lights with Electronic Ballasts
Like the development of electronic fluorescent ballasts, the development of electronic HMI ballasts was a major advance in lighting technology because they eliminate the flicker problem associated with magnetic ballasts, as well as the need for expensive frequency governors in small generators. They allow you to film at any frame rate and even at changing frame rates. An electronic HMI ballast eliminates flicker by creating a virtually constant output of light over the AC cycle by squaring off the curves of the AC sine wave. The changeover period is so brief that the light is virtually continuous.

By comparison to magnetic HMI ballasts, electronic HMI ballasts are quite a bit more complicated. As another example of a Switch-mode Power Supply (SMPS),
they, in fact, operate in a very similar fashion to electronic fluorescent ballasts. Like a fluorescent ballast, AC power is first converted into DC.
Then, a high-speed switching device (micro processor controlled IGBTs) turns the DC current into alternating current. The difference between an
electronic HMI ballast and an electronic fluorescent ballast is that the HMI ballast generates a square wave where the electronic fluorescent ballast
generates a high frequency sine wave.

Since an electronic ballast completely processes and regulates the input power they can tolerate fairly wide voltage and Hertz rate discrepancies. A 120V
electronic ballast can take an input from 95V to 132V with out affecting the output signal and the fixture's color temperature, and it will not be
affected by the fluctuations in frequency (Hz) of conventional AVR generators without governors.
Where they are not frequency dependent and will tolerate voltage fluctuations, at first it was thought that electronic square wave ballasts would operate
more reliably on small portable generators – even those without frequency governors. For this reason, as soon as electronic square wave ballasts appeared
on the market, many lighting rental houses replaced the more expensive crystal governed portable generators with less expensive non-synchronous portable
generators. The theory was that an electronic square wave ballast would operate reliably on a non-synchronous generator and allow filming at any frame rate, where as a magnetic HMI ballast operating on a crystal controlled synchronous generator allowed filming only at permitted frame rates. In practice, electronic square wave ballasts turned out to be a mixed blessing.
Like all SMPSs, electronic HMI ballasts without power factor correction draw current in large pulses and return harmonic currents to the power stream. The capacitive
reactance of electronic HMI ballasts also causes current to lead voltage and so they also have a leading power factor. An electronic square wave HMI ballast typically
has a power factor less than .6, meaning the ballast has to draw 40 percent or more power than it uses. For example a 1200W non-power factor corrected electronic HMI
ballast takes 18.5 Amps at 120 Volts to generate 1200 Watts of light and has a power factor of .54 (18.5A x 120V= 2220W, 1200W/2220W= .54).

Above is the nameplate from an Arri 575/1200 Electronic Ballast with DMX Control. You can see that it is marked that it will draw 18A of current ("I") at 125
Volts ("U"). You will also notice that it states that the ballast has a cos@=.6 which mean that the Power Factor is .6. It is important to understand that this greater Apparent Power consists not only of the high amplitude short pulses
of current drawn by the ballast. Like a CFL, a non-PFC electronic HMI ballast also returns the unused portion of the voltage waveform into the distribution system as harmonic currents. That is, when a wattmeter measures the actual
amount of energy being converted into real work (light) by the ballast (the “True Power” of the ballast), it is not measuring the power that goes into the generation of harmonic currents. Before exploring in more detail how the Leading
Power Factor and harmonics generated by electronic HMI ballasts can
adversely effect equipment operating on it, we need to say a few words about the loads placed upon generators by two new light sources: "High Output" AC LEDs and LEPs (Lighting Emitting Plasmas).
High Output AC LEDs

An LED consists of a chip of semiconducting material doped with impurities to create a “p-n junction.” As in other diodes, current flows easily from the p-side, or anode, to
the n-side, or cathode, but not in the reverse direction. As illustrated below, when the opposing electrodes of the p-n junction have different potentials, electrons fall into
the lower energy level, releasing energy in the form of a photons or light. LEDs, by nature, require direct current (DC) with low voltage, as opposed to the mains electricity from the electrical grid that supplies a high voltage with an alternating current (AC).

LED lights used in motion picture lighting applications fall into a category of LED technology called AC LED lighting. The term AC LED lighting refers to illumination generated by High Power LED (HPLED) light engines supplied with a sinusoidal AC voltage source—typically the utility line voltage (e.g., 120 V in the U.S., 100 V in Japan, 220 V in Europe). AC LEDs present many advantages over incandescent light sources including lower energy consumption, longer lifetime, improved robustness, smaller size, faster switching, and greater durability and reliability. For these reasons, but principally because of its high luminous efficacy, AC LED lighting has tremendous potential to become the dominant type of lighting in motion picture production. However, they are relatively expensive and require more precise current and heat management than traditional motion picture light sources.
One of the key advantages of LED-based lighting is its high efficiency, as measured by its light output per unit power input. White LEDs quickly matched and overtook the efficiency of standard incandescent lighting systems. In 2002,
Lumileds made five-watt LEDs available with a luminous efficacy of 18–22 lumens per watt [lm/W]. For comparison, a conventional 60–100 W incandescent light bulb produces around 15 lm/W, and standard fluorescent lights produce up to
100 lm/W. In September 2003, Cree, Inc. introduced a white LED light giving 65 lm/W at 20 mA, becoming the brightest white LED commercially available at the time, and more than four times as efficient as standard incandescent lights.
In 2006 Cree, Inc. demonstrated a prototype with a record white LED luminous efficacy of 131 lm/W at 20 mA, which is even better than standard fluorescent lights. Since then, LEDs have been proven (in lab tests) to surpass the assumed
theoretical limit of 200 lumens per watt. For instance, Cree has claimed to have a laboratory prototype LED achieving 231 lumens per watt (typical of high power LEDs the correlated color temperature was not great, it was reported to
be 4579 K.) However, these efficiencies are for the LED chip only, held at low temperature in a lab. In a lighting application, operating at higher temperature and with drive circuit losses, efficiencies are much lower. In 2009, a
United States Department of Energy (DOE) test of commercial LED lamps showed that average efficacy was about 46 lm/W at a time when manufacturers were claiming levels of 105 lm/W (e.g. the XLamp XP-G LED chip pictured below.)

Cree's high-power LED XLamp 7090 XR-E Q4
Such exaggerated claims on the part of manufacturers is common when a new technology comes to the market. Why should the manufacturers of LEDs be any different? In the marketing of their products, manufacturers of LED luminaries put a little spin on the scientific data, which has a tendency to cloud not only the issue of lumen efficiency, but also, as we shall see, of color rendering, color temperature, useful life, and finally energy savings. While there is truth in the claims as they pertain to single LED diodes, as the US Department of Energy (DOE) study (more details below) clearly demonstrates, it has turned out to be much more difficult for fixture manufacturers to realize anything close to the kind of lumen efficiency, color rendering, and lamp life within the framework of a practical light fixture that the LED manufacturers publish for their emitters. Some fixture manufacturers have made a substantial commitment in R&D and have made enormous progress in addressing some of these issues. For other manufacturers the key to success has been to downplay the limitations and keep the price of their fixtures low. For this reason, to pick the right LED luminary for a particular job it helps to have a little knowledge of the technology.
Manufacturers have come up with many ways to use LED technology in illumination devices. The common types are pads, small panels, lens lights, ring lights, larger panels, and RGB washes. In addition, there are small theatrical lights or entertainment venue lights, and wide variety of architectural lights in various shapes and sizes. Where it is beyond the scope of this article to analyze the advantage and disadvantage to each, I would suggest the 4th Edition of Harry Box’s “Set Lighting Technician’s Handbook” for a comprehensive survey of some of the most promising fixtures currently on the market. I will concentrate instead on the inherent advantages and limitations of this new technology in motion picture applications. Without a doubt LEDs have become one of the most efficient light sources available (Plasma Lamps being the other.) But, before the full potential of High Power AC LED lighting can be realized for motion picture lighting applications, LED manufacturers must overcome some key barriers: color rendering, cost, power quality and versatility. Let’s now explore the issues surrounding each of these in more detail.
The Color Rendering/Cost Trade-Off
A primary problem for manufacturers of LED fixtures for motion picture applications is how to manage the color spectrum of their fixtures. As we will see, this is a complex issue and how it is addressed ultimately determines the suitability of the fixture for
motion picture lighting applications. At this point in time in the manufacture of LED luminaries for motion picture applications there exists a trade-off between color rendering and cost. How a manufacturer trades one off for another depends on what approach
the manufacturer takes to creating "white light."
There are two primary ways of producing high intensity white-light using LEDs. One is to use individual LEDs that emit three primary colors — red, green, and blue — and then mix all the colors to form white light. The other is to use a phosphor material to convert
monochromatic light from a blue LED to broad-spectrum white light, much in the same way a fluorescent light bulb works.
Phosphor White LEDs
A "white' LED comprises a die (diode chip) that creates blue light. A portion of this blue light is used to activate a phosphor layer. Once activated, the phosphors create light of other colors that blend with the blue light to produce a fuller spectrum white light
much in the same way a fluorescent light bulb does. In effect, a fraction of the blue light undergoes what is called a Stokes shift and is transformed from shorter wavelengths to longer. Called remote phosphor technology, a primary benefit to this approach is that
the color spectrum of a given LED can be manipulated to a desired "white light" by applying phosphor layers of distinct colors. Depending on the chemistry of the phosphor used, the color balance of the resulting light can be correlated to daylight, or stretched closer
to a tungsten color balance. The cooler white LEDs use semi-transparent phosphors so the blue "pump" color comes through. In contrast to blue LEDs, the warmer white LEDs are opaque to the pump color, and are therefore much lower in efficiency. This Stokes shift process
reduces the total output , so there is a tradeoff in lumen output with warmer color temperatures and broader spectrum white LEDs.
Even though phosphor based White LEDs have a lower efficiency than normal LEDs due to the heat loss from the Stokes shift (as well as other phosphor-related degradation issues), the remote phosphor method is the most common method for making high intensity white
LEDs for a broad range of applications including home, architectural, industrial, and motion picture lighting. The reason for this is that the design and production of a light source or light fixture using a monochrome emitter with phosphor conversion is simpler
and cheaper than a complex RGB system.
The less expensive motion picture LED lighting instruments are affordable because they use the same White Phosphor LEDs as those mass-produced for home, architectural, and industrial lighting applications. Stamped from the same
semiconductor wafer as the chips used in these other applications, what differentiates the chips used in motion picture lighting instruments is the higher tolerances for flux (output), color (CCT and Green/Magenta bias), and
forward voltage used in the sorting of chips during a process called "binning" (illustrated below.) Put another way, they are simply the cream skimmed off the top of a production run.

Given the irregularities inherent in the manufacture of the semiconductor wafers from which White Phosphor LEDs are stamped, the LEDs in a production batch are all slightly different. In a mechanized testing procedure, they are sorted and grouped together
into bins according to their flux and color. Binning has been refined over the years, and these days the tolerance of the best binning systems allow barely perceptible differences between LEDS from a selected bin. The difference in color between two sources
is quantified using what is called the "MacAdams ellipse." A MacAdams ellipse defines the distance at which two colors that are very close to one another first become distinguishable to the human eye as different colors. As illustrated below, for a given point
of color on the chromaticity diagram, the MacAdams ellipse defines the contour around it, where the colors that surround the point are no longer indistinguishable from that of the point.

Binning has now been refined to the point where LED manufacturers can now bin their LEDs to separate them to within two to four MacAdams "steps." In other words, the LEDs within a single bin may be as much as four distinguishable separations apart from one another,
where one MacAdams step is not visible, two to four steps is barely visible, 5 or more is readily noticeable. Each LED manufacturer has its' own unique bin parameters (one has 15 distinct color bins for "warm white" alone.) It is also generally true that the tighter
the bin parameters (fewer MacAdams Steps), or the higher the flux (output), the higher the cost of the LEDs (as much as 2x-3x.) And, to complicate things even further, LED suppliers charge a high premium to fixture manufacturers who buy from just one bin.

To be cost effective fixture manufacturers must mix LEDs from a range of bins. This has prompted some manufacturers to create recipes using computer modeling. For example, for each LED from a slightly green bin, the recipe compensates with an LED from a magenta bin.
This way the fixture designer can assure that the sum balance of the light from all the LEDs in each fixture falls within their prescribed parameters for color balance and green/magenta shift. For a daylight-balanced LED fixture a well designed system can yield a
light fixture having very respectable tolerance of +/- 50K.
Fixture manufacturers for motion picture lighting generally rely on just such careful binning practices to provide as accurate and consistent color performance as they can. But this approach to white light has an inherent limitation: regardless of how tight the bin
parameters are set, by their nature the spectral distribution of Phosphor White LEDs is less than optimum for motion picture lighting applications.
Spectral Power Distribution
The spectral power distribution of a lamp indicates how much energy is present in each part of the spectrum. Natural sunlight and incandescent lamps have a continuous spectrum. Discharge lamps, like HMIs, have a discontinuous spectrum with a series of emission
lines at different wavelengths. To fill in the missing colors, they contain additives that contribute the absent parts of the spectrum and make it continuous. Given how they produce white light, Phosphor White LEDS have a unique discontinuous spectral quality that
is unlike that of natural daylight, HMI, or incandescent light. In the case of 3200K White LEDs, the phosphors added shape the spectral distribution by enhancing certain colors in the spectrum to simulate the spectral distribution of incandescent light. As a result,
the spectral distribution of Phosphor White LEDs resembles a series of peaks and valleys. If you look at the spectral power distribution of a white LED (below left) you will notice a big spike at about 465nm (the blue LED) and a broader bump between 500 and 700nm
produced by the phosphors. Even though the spectral power distribution has these peaks and valleys, the human eye perceives the light as white light.

The curves shown above are the spectral power distributions for the three approaches to producing white light that we will discuss as well at that of an incandescent lighting instrument. While the discontinuous spectral distribution of Phosphor White LEDS (far left)
may appear white to the eye, and the color of objects illuminated by it appear natural to the eye, to film emulsions and digital imaging systems designed to reproduce accurate color under continuous spectrum light sources (like daylight or incandescent lamps), the
color of the same objects will appear unnatural on screen. That is, the hue of an object being illuminated by this "apparent white light" can be drastically different than expected when it appears on the screen. For example, below is a "Macbeth chart" contrasting
the resulting effect upon different color swatches of studio tungsten light and a representative Phosphor White LED lighting instrument.

Split Macbeth chart: each color patch shows the visible effects of studio tungsten light in the top half of the patch, and a representative Phosphor White LED lighting instrument in the bottom half.
A common test chart used for assessing color performance of motion picture imaging systems, the chart above would be more accurately called a "split Macbeth chart" because each color patch shows the visible effects of the two light sources – studio tungsten in the
top half of the patch, and the Phosphor White LED lighting instrument in the bottom half. Although your computer display is not likely to be a calibrated reference monitor, the wide variations in color patch hue caused by the discontinuous spectral distribution of
the Phosphor White LED lighting instrument should be readily apparent.
What accounts for these results? First, as you can see from its' spectral power distribution above, Phosphor White LEDS, compared to continuous light sources, have no output at wavelengths shorter than about 425nm, which means that violet colors don't render well.
Second, there is minimal output in the medium blue-cyan-turquoise range from about 465-510nm, which is why the aqua-type colors don't render well either. Lacking these complementary colors within the spectrum, skin tones and warm, amber-yellow colors don't stand
out. Third, with the long-wavelengths cutoff in the high-600 nm range, pinks, reds, oranges, and other long wave-length colors tend to look a little dull under Phosphor White LEDs, compared with how they look under continuous spectrum light sources (daylight, HMI,
Tungsten) which extend all the way out on the long-wavelength end. Finally, as you can see from the gray scale at the bottom, this particular Phosphor White LED Luminary has a overall magenta bias.
It is a common mistake to think that a custom camera white balance can correct for the deficiencies of LEDs. While you can white balance out/time out this magenta bias
in digital video cameras/digital film intermediate, the camera/timer is not able to replace the parts of the spectrum that are missing all together. And since gels only
rebalance the spectral distribution of a light source by passing the wavelength of the color that they are, gels cannot correct for these deficiencies either because t
here is not light of those wavelengths to pass in White Phosphor LEDs to begin with.

This inability of LEDs to render color is very visible in tests recently performed by The Academy of Motion Picture Arts and Sciences (AMPAS) as part of their “Solid State Lighting Project Technical Assessment” (see below for details.) In one (above) a model was photographed wearing a dress that had a number of different blue/cyan tints. Footage was shot with both a true tungsten source and a White Phosphor LED source. The tungsten-lit footage displayed all of the subtle differences in blue/cyan tones in the fabric, while the LED-lit footage, lacking cyan output, showed just a nice blue dress, without the same richness of hue. Since the light doesn’t put out much cyan, the camera/film simply can’t record it because those wavelengths are not reflected by the dress.
The same holds true of flesh tones illuminated by LED light. As is also evident in the pictures above, skin tones don’t reproduce well under LED lights because of the steep drop off of high frequency colors (above the 600nm cut off) such as pinks, reds, oranges, and other long wave-length colors. As the illustration below, comparing the reflected spectral distribution of a Caucasian skin tone under theoretical pure white light (an even distribution of all wavelengths) to that of a Phosphor White LED demonstrates, absent these wavelengths the skin tones look pale under LEDs because light reflected by the skin tone is likewise absent these critical long wavelength colors.

Reflected Spectral Distribution of Caucasian skin tone under theoretical White Light and Phosphor White LED Light
In the picture above illuminated by the Phosphor White LED, both the cyan/blue dress and the skin tone, don’t reproduce well because you can't get accurate color reflected from an object unless that color is in the light in the first place. In other words, if the light source doesn’t generate the color (cyan), it is not reflected by the object (the dress) and so the camera/film simply can’t record it. And, as Cinematographer Daryn Okada, ASC, discovered the hard way, color gel packs, camera white balance, or digital intermediate timing can’t bring it out if it isn’t there to begin with.
Like many of us, Daryn Okada uses LEDs as “touch up” lights to add a little something where key lights don’t cover. Needing to touch up a face on one talent mark, he once hid a small LED unit behind a chair, to add some glow to an actress’s face when she reached a mark where the keys had fallen off. “The manufacturer claimed the unit to be a ‘tungsten LED source,’” he recounts. “She stopped right in the doorway, where I had this LED, and looked fine. But when I got the dailies back, her face was totally magenta.” What’s worse, Okada says the image could not be repaired in post, because there wasn’t enough of the right color of light in the scanned negative for a color timer to bring out.
Had Daryn Okada been shooting with a digital video camera, he would have noticed the off color of the LED source immediately. But, given the limited spectral output of LEDs, his ability to remedy the problem would have been limited. If he white balanced the camera for the LED source, the background of the room beyond the doorway that was lit by tungsten lights would turn very green. In a mixed light situation such as this, the only alternative is to match the LED source to the prevalent tungsten source with a custom gel pack on the LED head. But, since gels rebalance the spectral distribution of a light source by passing the wavelength of the color that they are, gels cannot correct for these deficiencies either because there is not light of those wavelengths to pass in White Phosphor LEDs to begin with. In other words, White Phosphor LEDS are so deficit in certain parts of the color spectrum that by the time you came up with a color gel pack to match them to a continuous light source like a tungsten light, the LED panel would put out very little light with all those gels on it.
To understand why this is so, we need only look at a similar situation: the conversion of tungsten light to daylight using full CTB gel. As you can see in the Spectral
Power Distribution graph of tungsten light above, tungsten light is so deficient in the blue part of the spectrum that it takes a quite saturated blue gel to balance it
to daylight (see spectral transmission of Full CTB gel below). In fact, the transmission coefficient of some Full CTB gels is only 24%, which means that it passes only
24% of the source. That is why gelling tungsten lights
is a very inefficient way of creating a daylight source (a tungsten 1000w gelled with CTB becomes a 240W daylight source.)
Spectral transmission of Full CTB gel
A gel pack that would match a White Phosphor LED to tungsten light would have to include violet to extend its’ spectral output below 425nm. It would have to include medium blue, cyan, and turquoise to fill in the missing wavelength from 465-510nm. Finally it would have to include pink, red, and orange to extend its’ spectral output beyond its’ 600nm cut-off. All of these gels would have to be quite saturated, since there is very little, if any, output of these wavelengths in White Phosphor LEDs to begin with. Imagine how much light you will get out of a LED light panel with such a gel pack (LED light panels put out barely enough to begin with, and have no output to waste to such accurate color correction.) Since, under most circumstances it is simply not feasible to completely match LED sources to tungsten sources with a gel pack, in mixed light situations such as these you are left, without recourse, with the off color generated by LEDs.
If the actress in Daryn Okada’s shot were the model in the blue/cyan dress above, you can imagine what would happen when she stepped onto the mark lit only with the LED source by looking closely at the contrasting
photos above. Since, under the circumstances, Daryn Okada could not white balance for the LED source (and it would not be feasible to match the LED source with a gel pack) the rich blue/cyan hue of her dress in
the left photo would turn into the simple blue of the right photo. The vibrant skin tone of the left photo would turn into the flat skin tone of the right photo, and it would have an overall magenta cast to boot.
This example clearly demonstrates that White Phosphor LEDs, simply by nature of their discontinuous spectral distribution, cannot accurately reproduce colors on screen under all circumstances no matter how tightly their bin parameters are set.
While they are less than perfect at reproducing parts of the color spectrum, the color rendering of Phosphor White LEDs may be adequate in certain situations. For a specific application, say where lights must be
operated off of batteries, a LED fixture offers the unique advantage of greater power efficiency over conventional lights, which may out weigh its shortcomings in color rendering.
After all the color spectrum of LEDs is not horrendous. For example if you were to look at the image of the model in the cyan/blue dress lit by Phosphor White LEDs above, you wouldn’t say it looked bad. But, when viewed side-by-side with the same
image lit by a continuous tungsten source, you see what it should have looked like. For that reason whenever color rendition is critical I always opt for a continuous spectrum light source - especially shooting interviews where rendering a realistic
flesh-tone is critical.
For example when I lit Ted Kennedy in his old age, and it was important to convey the impression of a robust and healthy elder statesmen, I fought hard to use a more expensive HMI interview kit consisting of Joker HMIs with Chimera Light Banks, when the show producers wanted me to use a cheaper LED kit. To convince the Producers that there would be a significant difference, I brought the LED kit. After seeing the difference they came up with the extra money for the HMI kit because it was important to render a healthy flesh tone.
I also wouldn’t try to light a table-top food/product shot with LEDs either. Because of their limited color rendering capability, food presentation that will look vibrant and colorful to eye, under LEDs will tend to look a little dull on camera.
By comparison a full spectrum daylight source such as HMI or LEP will capture the vibrant colors. Likewise, I wouldn’t try to mix LEDs with a uniform continuous light source, such as a studio lit with tungsten fixtures. If caught in isolation,
their color deficiencies will be quite noticeable and unacceptable in comparison to the tungsten. And, I would always choose a discontinuous source like high CRI fluorescent tubes over LEDs because the discontinuous color spectrum of Kino Flos can be
easily corrected with gels - where LEDs can not.
Once the green spike of
Kino-Flo’s True Match tubes have been corrected by the application of minus green (magenta) gels, the resulting spectral distribution is nearly continuous and contains a greater proportion of the long wave length colors that
are so critical to rendering flesh-tones accurately (see illustration above.)
Where skin-tones are significantly altered by the steep drop-off of long wavelength colors in LED light sources, Kino-Flo’s high CRI True-Match tubes contain sufficient light in that critical part of the spectrum to render
skin-tones realistically (see illustration above.) In other words, once Kino Flo True Match Tubes have been corrected for their green spike, they provide a nearly full spectrum source. With LEDs, it is nearly impossible to correct for their
deficiencies with gels.
Unfortunately, the limitations inherent in remote phosphor technology make it unlikely that we will ever see a Phosphor White LED with as continuous a color spectrum as the best Flos do today. If you will recall, in the remote phosphor approach to white light with LEDs, the LED designer manipulates the color spectrum of a given LED to a desired "white light" by applying phosphor layers of distinct colors that are activated by the LED’s “Pump” color (usually the 450nm blue of an InGaN LED) to extend the color spectrum by a process called a “Stokes shift.” Depending on the chemistry of the phosphors used, the color balance of light generated by remote phosphor technology can approximate daylight, or stretched closer to a tungsten color balance. The “5500K” white LEDs use semi-transparent phosphors so the blue "pump" color comes through. In contrast to 5500K LEDs, the warmer “3200K” white LEDs have to use more phosphors and so are more opaque to the pump color, and are therefore much lower in efficiency.
There are inherent limitations to the “Stokes shift” process by which a portion of the “pump” color is transformed from shorter wavelengths to longer. First, it works in only one direction – that is why LEDs don’t emit color wavelengths shorter than their pump color and why
Phosphor White LEDS, compared to continuous light sources, have no output at wavelengths shorter than about 425nm (which is why violet colors don't render well under them.) The second inherent shortcoming to this approach to generating “tungsten” light from a LED is that
the Stokes shift process reduces the total lumen output, so there is an inevitable trade-off in lumen output and broader spectrum white LEDs. For that reason LED designers have to cut the high frequency output in the high-600 nm range. The appreciable drop-off of color wavelengths longer than 625nm that results is why pinks, reds, oranges, and other long wave-length colors tend to look dull under 3200K LEDs, compared with how they look under true Tungsten light which is a continuous spectrum light source that extends all the way out on the long-wavelength end.
Finally, given the unavoidable energy loss in the Stokes shift, the remote phosphor approach is not the most efficient method to achieving photographic white light with LEDS. For this myriad of reasons, the remote phosphor approach to generating photographic white light with LEDs has been all but abandoned by the more serious manufacturers of LED luminaries for motion picture production – leaving only manufacturers of LEDs for the general illumination market and those manufacturers that repurpose them for motion picture lighting applications.
No matter how much effort is spent on optimizing Phosphor White LEDS to higher light output and higher CRI ratings for the general illumination market, without a mass market for continuous spectrum remote phosphor LEDs (as opposed to high CRI – they are very different) tuned to our specific needs, there is not much hope of seeing a true “Tungsten” LED. In other words, because our requirements do not coincide with those of the mass general illumination market, LED manufacturers - outside of possibly Osram (see below for details) - are not developing Phosphor White LEDs specifically for motion picture lighting – it is simply too small a market in the larger scheme of things. As long as that is the case, there will be higher CRI LEDs developed but we won’t see a meaningful attempt to address the color rendering deficiencies of Phosphor White LEDs for photographic purposes.
The OSRAM KREIOS LED chip
Since, the color spectrum of LEDs can be manipulated by blending phosphor layers, it is possible to tune their output specifically for the color sensitivity of film emulsions and digital imaging systems. The motion picture lighting division of OSRAM did just this
in the KREIOS LED stage light module that Mole-Richardson uses in their MoleLED 12 Pack.

The OSRAM Kreios stage light LED module
The KREIOS stage light module (pictured above) is a metal core circuit board with 20 high-output blue LEDs each topped with a remote phosphor dome. The phosphor domes are an OSRAM proprietary design, which are blue light activated to produce light that is a very
close approximation of Tungsten and Daylight. While, remote phosphor technology is commonly used to extend short wavelengths to create a fuller color spectrum in Phosphor White LEDs, OSRAM was the first LED manufacturer that set out to use remote phosphor technology to
match the spectral sensitivity of Tungsten and Daylight balanced film stocks.

The spectrum distribution of the Daylight balanced MoleLED clearly shows the blue light emitted by the InGaN-based LED
(peak at about 465 nm) as well as the more broadband light created by phosphors.
And, with the help of Kodak, Panavision, Technicolor, and Shelly Johnson ASC, multiple film tests were shot with the KREIOS stage light module in order to verify the color generated by the MoleLED on set would translate to the color viewed in film dailies.
This attention to detail and strict testing has resulted in a LED fixture that almost seamlessly mixes with existing Tungsten Halogen light sources, natural daylight, or any daylight balanced light source.

The spectrum distribution of the Tungsten balanced MoleLED clearly shows the blue light emitted by the InGaN-based LED
(peak at about 465 nm) as well as the more broadband light created by phosphors.
Even though OSRAM was successful in using remote phosphor technology to closely match the spectral sensitivity curves of Tungsten and Daylight balanced film stocks, this approach has several drawbacks. Since the OSRAM KREIOS stage light module is specifically
designed for motion picture lighting applications, and not mass produced like Phosphor White LEDS, they are considerably more expensive – making the MoleLED 12 Pack (pictured below) one of the more expensive LED light panels on the market.

The MoleLED 12Pack
And, given the seemingly unavoidable energy loss in the Stokes shift, the remote phosphor approach is not the most efficient method to achieving white light with LEDS. And, finally, the consistency of the color output of remote phosphor LEDs is
effected by the binning and manufacturing tolerance of their blue pump (generally optimized between 450nm and 460nm), thermal management in the fixture, the ageing of the phosphors, and even the ambient temperature.
For example, a one degree shift in the junction temperature of the blue InGaN LED (pump color) in remote phosphor LEDs, will cause a +/- 2nm shift in the dominant wavelength. If compounded by the average wavelength variation of +/- 2nm of blue InGaN LEDs, a 5nm divergence from the prescribed 455nm wavelength of the pump color will create color inconsistency of 5 MacAdams ellispses. While not readily apparent to the eye, image capture systems will easily see this variation.
However, much effort is being spent on optimizing these devices to higher light output and higher
operation temperatures. With development ongoing, the efficiency of phosphor based LEDs is sure to rise, but without a mass market for remote phosphor LEDs tuned to our specific needs, there is not much hope of the prices coming down significantly.
Since, market competition often focuses on brightness (lumens/watt), some manufacturers opt for brighter LEDs with unappealing color characteristics, while others select LED chips with better color characteristics and rely on good optical design and drive electronics
to produce reasonably good output. With all these factors in play, it would be quite misleading to judge the quality of an LED fixture strictly on the basis of brightness. Manufacturers using remote phosphor technology are forced to balance these competing priorities, and each approaches it in
their own way.
Tunable Multi-emitters
A more efficient approach to generating white light with LEDS, and one resulting in more lumens/watt, is to use tunable multi-emitters. These lights use multiple LEDs that each emitt light at different wavelengths. The simplest form of a multi-emitter instrument is a
"tri-color panel" using red, green and blue LEDs, also known as an RGB LED. While the RGB approach is capable of delivering not only a vast array of colors as well as tunable white light, the CRI (Color Rendering Index) is quite low. The typical color rendering
achievable for such a system ranges between 40 and 60 depending on the targeted color temperature (3200K or 5500K.) Motion picture lighting typically requires a CRI in excess of 80, and higher the value the better. Therefore, an RGB tunable emitter may be
well suited to color washing applications in stage lighting, it is less suitable for creating white light for motion picture lighting applications.
A variation of the multi-emitter technique that is better suited to motion picture lighting uses "cool white" and "warm white" LEDs within the same fixture, and provides a control to mix the colors as needed. The idea is that by mixing the two sets of LEDs, the user achieves a
nominally correct CCT for any color temperature from tungsten to daylight. While this is an intuitive solution to color balancing that one would think eliminates the need for fractional CTO and CTB color correction gels to achieve an intermediate color
balance, this approach does entail a compromise non-the-less.

If on the chromaticity diagram above, you were to plot the color point of two illuminants, all the colors that are possible by mixing the two colors of light will be located on the straight red line drawn between the two points. However, the line (black line above)
that would be charted by heating a black body radiator (as it turns red, orange, yellow, white, and finally blue as it is heated) is not a straight line, so it is not possible to create light that remains neutral in terms of their green/magenta shift, while mixing
only two colors.
Another variation of the multi-emitter technique that is even better suited to motion picture lighting uses additional LEDs that emit additional wavelengths to create a closer match to natural daylight or studio tungsten light. For instance, the addition of an
amber emitter (creating an RGBA system) significantly enhances the CRI of the light generated while still maintaining the desired color point. The primary advantage to RGBA systems is that color flexibility is still achievable, but more importantly for motion
picture lighting applications, it is possible to walk the white point along the black body line while still maintaining a CRI approaching 90.

RGBA emitters do however present LED lighting manufacturers with some design challenges. Delivering a consistent color across the beam without color fringing or shadowing can be a complicated task. Reducing the optical source size of the LED or LED system can
improve the color mixing. One approach is to create a multichip LED (like the one pictured above), locating the individual colors as close as possible and therefore reducing the mixing distance. Although various multi-chip packages exist, few exist that enable
both high flux density (output) and color mixing. Most multi-chip packages are limited to a low drive current, reducing the flux density and output. Alternatively one may use multiple discrete high output sources, but this increases both the optical source size
and color mixing challenge. Such fixtures typically place a diffusion material immediately over the LEDs to help blend the discrete colors, but this comes at a loss of output.
Another problem is that, while it is relatively easy to put a dimmer on an LED, and blend two different color LED chips to achieve variable color mixing, as we saw above it is quite a different matter to track the color so that it remains on the black body locus
at every point from daylight balance to tungsten balance. Maintaining a specific color temperature at a high CRI while dimming is made even more difficult by virtue of the fact that temperature in the LED changes when they are dimmed. Change in temperature shifts
output wavelength as well as efficiency, and different LED chips change efficiency at different rates and at different temperatures. For these reasons, a more complex approach to dimming is required in order to control all these factors.
Some manufacturers start by incorporating more colors of LED chips into the fixture in order to counter the shift in green/magenta bias as the color tracks along the black body locus. The chips are controlled by microprocessors using algorithms to continuously
regulate the intensities of the different colored LEDs so that the mixed light gives the desired color temperature at any dimmer setting. Using multiple LED colors within a white-light fixture increases the total color space achievable by the light, and in
this way greatly improves on the limited color rendering of Phosphor White LEDs when used alone. Using this approach also allows the manufacturers to calibrate each fixture at the factory to compensate for any difference in the color output of the particular
LEDs. Without a doubt, multi-emitter LED fixtures require a complex set of design considerations to deliver consistent color. These fixtures require intelligent drivers that can ensure Color and CRI consistency over time and temperature through predictive means.
The better multi-emitter designs, like the new Arri L7 LED Fresnels (see below for more details) incorporate a color-feedback system of self-monitoring sensors to ensure stable color across a range of output levels, as well as correcting changes in performance
caused by ambient temperature and component aging, which ensures consistent color temperature. These units use an LED array optimized for film and video image capture, with standard color temperature presets. These arrays can create broad-spectrum white light
and, unlike conventional multi-emitter LED lights, the color temperature remains consistent throughout the full range of dimming, ambient temperature and life of the unit. The drawbacks to this approach are that they are expensive (they require micro-processers)
and their spectral distribution is still discontinuous. Even though they emit additional wavelengths to create a closer match to, say, tungsten lighting, as we can see by their spectral power distribution graph below, the resultant curve is very "spikey". This
has the same noticeable side effects in color reproduction as discussed above. Like remote phosphor LEDs, tunable multi-emitter designs, simply by the nature of their discontinuous spectral distribution still cannot reproduce colors on screen with complete accuracy.

Unfortunately it is very hard to judge with your eye how an LEDs spectrum is going to line up with the sensors in the camera. As we have seen, eye response and camera response can be quite different. Additionally common color meters, like the Minolta III F, are
completely useless with LEDs. The meter makes its calculation of the color temperature based on an assumption that the light source has a continuous spectrum. Color readings of an LED have been shown to be misleading for both correlated color temperature and
green/magenta shift. To make matters worse the CRI ratings published by manufacturers are useless if not downright misleading.
CRI and Color Rendering
Contrary to popular belief, CRI ratings are not a valid measure of judging the color rendering capability of LED luminaries for photographic purposes. First, the CRI Index was not designed for photographic purposes, but simply to provide a reference scale for general
illumination. It is as follows:
- CRI 90 - 100: Retail (merchandise, artwork) and work spaces (design) where faithful color rendering is critical.
- CRI 70 - 90: Most office, retail, school, educational, medical, and other work and residential spaces where good color rendering is required.
- CRI as low as 50: Industrial security and storage lighting where color fidelity is not important.
As you can see the CRI index makes no mention of photographic reproduction. It is simply because there is no means by which to measure for photographic purposes the discontinuous output of LED lights (CCT is for continuous spectrum black body radiators only) that LED
manufacturers use the CRI index.

Second, the CRI index is a measure of the ability of a light source to reproduce a minimum of 8 mid saturated colors faithfully (a different 8 colors are used in Europe.) As such CRI ratings are at best a very limited measure of the color rendering capability of a
light source. And, finally, it is possible for a LED luminary manufacturer to game the system by tuning the output of their LED to the limited color range of the CRI color scale and achieve a high CRI rating while delivering mediocre results on screen. Let’s take up
hese issues one at a time.
What makes CRI an imperfect measure for photographic purposes? It really only tells you how a light source will perform in a narrow band of mid saturated colors, and it is best with sources that lie near to the line of a black body radiator on the Chromaticity diagram and don’t have too high or too low a color temperature. Because CRI wasn’t designed as a measure for “White Light” produced in the way that an LED produces it, it can produce misleading results when applied to LEDs. With a large gap in wavelengths from 465-510nm Phosphor White LEDs
can do a bad job of rendering cyan but still get a respectable CRI because the eight indices for the individual test colors are averaged together to produce the final CRI. In other words, a light source such as LEDs can score well even though they render one or
two colors poorly because the CRI average hides the deficiency.
Additionally, because the eight standard sample colors are all of fairly low saturation, the CRI tells you nothing about how a light source will perform when rendering deeply saturated colors. For instance, saturated colors that fall between the widely separated peaks
of the spectra of Phosphor White LEDs will perform poorly, but the CRI scale won't register that deficiency either.
Finally, it is possible for a LED luminary manufacturer to game the system by tuning the output of their LED to the limited color range of the CRI color scale and achieve a high CRI rating while delivering generally poor results on screen. Since the eight standard
sample colors do not include an orange or red, CRI ratings will not tell you how a light source is at rendering these long wavelength colors that are so critical to rendering an accurate Caucasian flesh-tone. In other words, since it does not measure above the 600nm
cut-off of Phosphor White LEDs, CRI does not tell you how LEDs are at rendering flesh-tones.
These inherent problems with using CRI to measure the color rendering capability of solid state lighting are becoming widely recognized and a new metric, CQs or Color Quality scale, is under development by the national Institute of standards and technology (nIst) to address these and other concerns. Until then, the CRI ratings of manufacturers should be taken with a grain of salt.

The "Tru Color" Foton 33W Single Emitter LED Light
For example, PRG has introduced a White Phosphor LED, the Foton, that boasts a CRI rating greater than 97. In typical marketing hyperbole, PRG claims on their website that “Producing a 97+ CRI … the Foton is the most color accurate digital light source designed specifically for motion picture, broadcast and professional photography.” Given the high CRI indices the Foton is able to achieve on the eight standard CRI colors (see illustration below), that is probably true.

But, if we look instead at the Spectral Power Distribution graph of the Foton (below), we see that the long wavelength colors that are critical to rendering a realistic flesh-tone still drop-off appreciably. Even though the Foton suffers the same inherent limitations of all Phosphor White LEDs to generate colors with long wavelengths, this deficiency is not reflected in its CRI of 97+ because these long wavelength colors are not part of the narrow range of CRI colors. Since the rendering of a realistic flesh-tone is paramount in cinematography (whether for film or Digital), CRI is simply not a valid measure of a LED’s color rendering capability for motion picture lighting.

For these reasons, the best approach to judging the color of a LED luminary is to shoot tests. A side-by-side comparison using a color chip chart and a full spectrum light source, will clearly demonstrate how the camera system will respond to a specific LED
fixture. To see such camera tests of wardrobe, set, and make-up for the different approaches to achieving white light with LEDs that we have discussed, use this link to the
Solid State Lighting Project Technical Assessment generated by the Academy of Motion Picture Arts and Sciences.
Lumen Maintenance/Depreciation
How well a lamp maintains its lumen output over time is referred to as lumen maintenance. Greater lumen maintenance means a lamp will remain brighter longer. The opposite of lumen maintenance is lumen depreciation, which represents the reduction of lumen output
over time.
A number of factors effect lumen maintenance/depreciation. In the case of discharge lamps (HID or HMI) and incandescent lamps (Tungsten), the repeated cycles of heating and cooling that their quartz envelope goes through, cause the molecules to lose their
crystalline structure. As a result, the quartz envelope over time loses some of its transparency and becomes more opaque. This process is called devitrification. As the quartz envelope devitrifies, it blocks more of the light and prevents it from escaping
from the envelope, contributing to the depreciation of the lumen output. Another cause of lumen depreciation in discharge lamps (HID or HMI) and incandescent lamps (Tungsten), is that metal from their filament or electrodes evaporates and condenses on the
inner wall of the quartz envelope, causing blackening. This also contributes to the loss of light output.
A third factor that effects lumen depreciation is the intended use which is reflected in the bulb design. One way to think about HMI lamps is as a metal halide type lamp with a rock-n-roll life philosophy of "live fast, die young." To increase output, improve
luminous efficacy, and color rendering, HMI lamps are designed with comparatively very short electrode gaps. However, their increased luminous efficacy places an increased load on the bulb wall which accelerates the devitrification of their quartz envelope;
which, in turn, leads to increased lumen depreciation. In other words, their brilliance comes at the expense of lamp life. Over their relatively short life of 500-750 hrs, it is not uncommon for HMI lamps to lose 15-20 percent of their initial lumen output
before they fail all together.
Evaluating the lumen maintenance of an LED luminary is more complex because in many ways it is more complex than traditional fixtures. An LED is an electromechanical system: in addition to the essential light emitting source, an LED luminary also includes a
provision for heat transfer, electrical control, optical conditioning, mechanical support, and protection, as well as aesthetic design elements. Because the LEDs themselves are only one part of this elaborate electromechanical system, the affect of these
other components must be taken into account when determining the lumen maintenance of an LED luminary.
For instance, while LEDS do not radiate heat like a tungsten filament, half or more of their input energy may be converted to heat in current carrying components. This heat must be conducted away from the diodes for an LED to operate efficiently. This situation
requires a heat conducting assembly, be it a passive heat sink or active fan cooling, that will operate reliably over an extended period of time - most do not. For proper operation, the power supply and electronics of an LED luminary must provide a well-controlled
DC drive current and other control features - most begin to fail long before the rated life of the product.
Any optical components must also be able to withstand years of exposure to intense light and possibly heat without yellowing, cracking, or other significant degradation. Reflecting materials need to stay in place and maintain their optical efficiencies. Since
it is nearly impossible, even in the best designed LED luminaries, to completely protect against system degeneration of the type described above, the lumen maintenance of an LED luminary is significantly less than that given by manufacturers for a single diode.
For example, recent tests from the Caliper program (US Dept. of Energy) suggest that the lumen output of many LED luminaries depreciate to less than 50% after only 500hrs (see page 27 of the summary for examples of
lumen depreciation after about 500 hours
.) While, this might not be representative of every product, the vast majority of those that were tested fell far short of the manufacturers claims of lumen maintenance.
Color Shift
In addition to losing light output, an aging luminary, also exhibits color shift. With HMI bulbs, color temperature varies significantly with lamp age. A new bulb generally will output at a color temperature close to 15,000 K during its first few hours. After
this short burn-in period, the color temperature reaches its prescribed value of around 5600 K or 6000 K. With age, however, its' arc length becomes larger as more of the electrodes burn away. Greater voltage is required to sustain the arc, and as voltage
increases, color temperature decreases proportionately at a rate of approximately 0.5 -1 Kelvin for every hour it burns. Which means that by the time it fails, after approximately 750 hours of use, its' color temperature will be between 5250 and 4875K.
Determining the color shift of LED luminaries is also complicated. That is because color stability is not exclusively determined by the performance of the LED diode. Other factors that contribute to color shift
in LEDs include LED design, materials, manufacturing processes, optics applied to the LED, and the temperature and time the LED operates. The increase in junction temperatures typical of LEDs over time can cause color shifts as noted above.
Likewise, optical
components in the LED luminary may discolor, crack, or significantly degrade after extended exposure to the intense light the luminary generates. Environmental conditions (including air quality) may cause materials in optical components to deteriorate. Finally,
luminary design my create non-uniform color characteristics such as halos or yellowish, bluish, or greenish hues around the edges of the beam, and these color characteristics may vary over time for the reasons mentioned above.
A new technology also requires a new method of measuring shifts in color. Since LEDs are not "black body" radiators (that turn red, orange, yellow, white, and finally blue as they are heated), the Correlated Color Temperature (CCT) ratings in Kelvin are not
adequate to describe color shifts in LED luminaries over time as it is in conventional lamps. This is another reason why the LED industry uses, instead, the "MacAdam ellipses" discussed earlier.

That samples in the Caliper study cited above (one is illustrated above) exhibited color shifts greater than a 36-step MacAdams ellipses and a 30 percent drop in lumens within 3000 hours, suggests that that LED luminary reached it's usefulness to serve even
as a set practical for motion picture lighting long before 3000hrs (remember one MacAdams step is not visible, two to four steps is barely visible, 5 or more is readily noticeable.) Unfortunately, the manufacturers of LED luminaries for motion picture lighting
purposes do not publish specifications for color shift over time; probably because, as the results of the Caliper study cited above suggests, they are significant and would appreciably shorten their claim of 50'000 hours of "lamp life." The better LED luminaries
for motion picture lighting applications (the Arri L7 and Gekko Kezia) compensate for color shift with active microprocessor controlled color management that involves self testing using internal color sensors (see below for more details.) However, sensors and
controls may themselves shift over time and affect color - so even such methods of color management are not full proof.
Lamp Life
In light of what we now know about LEDs, claims of 50'000 hr lamp life made by manufacturers like Litepanels should be taken as the marketing hyperbole that they are. Determining the "life" of an LED luminary is a very complex matter and how to do so is still
being hotly debated within government and industry regulatory bodies. Until a standard measure of LED lamp life is settled upon, extravagant claims of 50'000 hrs should be taken with a grain of salt.
For conventional lamps (HID, HMI, Incandescent, Fluorescent), the method for determining "rated average lamp life" is well established and easy to calculate: it is simply the point at which half the lamps cease to emit light. For LED luminaries it gets quite a bit
more complicated for several reasons. One complicating factor is that LED luminaries are made up of multiple components and usually have no replacement parts. That means, even though the individual LEDs in a luminary may be rated to last for 50'000 hours, its'
actual life will fall well short of that mark if one of its other key components fails sooner. For example, HMI ballasts are manufactured to outlast their lamps many times over, because those lamps are relatively short lived and easily replaced. But at this
relatively early stage in the development of LED technology, there's very little data available to confirm that LED drivers will last as long as the expected life of a LED diode that carries a 50'000 hr rating.
Another complicating factor is that LEDs have no filament or electrodes to burn out and thus generally keep on producing light, although at declining levels and a gradual shift in color. And, since a well designed LED luminary has a comparatively very long-rated life
(as conventionally defined), over which its' lumen output drops continuously, it also has an appreciatively greater lumen depreciation over that life than does an HMI lamp. To extend the analogy used above, if HMI lamps are "Live Fast, Die Young" Rock-n-Rollers, LED
Luminaries would be suburban Dads working 9-5 jobs. With their best years behind them and a few more pounds around their waist, they now spend their weekends driving the kids to soccer practice in a minivan, and usually fall asleep by 10pm on a Saturday night watching
TV. Given their continuous
lumen depreciation and color shift over time, it is clear that there comes a time when, like a suburban Dad, a motion picture lighting LED luminary has surpassed it working life and should be retired. Since it won't burn out in its' prime, like an HMI lamp, how
do we determine when a light has surpassed its' useable life. Clearly, this new technology requires a new approach to determining useable "lamp life" than that used for conventional lamps like HMIs.
For instance, how useful is a manufacturer's "rated average lamp life" of 50'000 hours when testing has found that complete LED luminaries can depreciate as much as 50% in just 500 hrs. Whatever the stated lifetime of any lighting product, it must reflect a
meaningful statistical measure of the performance of a given fixture design. Clearly, in the case of LED luminaries to be meaningful "lamp life" must include not only the median time to failure of the array of diodes under normal operating conditions, but
"failure" must also be defined as unacceptable lumen depreciation for the particular application rather than complete failure to light.
One such alternative rating system for LED Lamp Life proposed by the Department of Energy (DOE) LED Lifetime and Reliability Working Group
denotes "B" and "L" factors; where B represents the interval of time it takes for half of the diodes to "fail" (called B50), and L is the lumen performance level defining a "low-light failure". For example, the LED luminary that depreciated 50% in just 500
hrs in the Caliper study above would have a B50/L50 Lamp Life rating of 500 hrs. In other words, after 500 hrs, half of the diodes will have considered to have "failed" because their output dropped to 50 percent (low light output.) In this rating system B
represents the time interval in hours in which a percentage of diodes have failed, where L represents failure as defined by an unacceptable lumen performance as a result of lumen depreciation.
One benefit to this rating system, is that each industry can determine a "lamp life" that is meaningful to its' application. For example, a B50/L50 rating of 500hrs (a drop-off of 50 percent of the diodes (B50) to 50 percent of their original value (L50) in
500 hours) may be perfectly acceptable in warehouse illumination. In more demanding applications, like home illumination, more demanding criteria would be required in determining lamp life for it to be meaningful. Most LED manufactures for home illumination
use L70, or the point where lumen output has declined by 30 percent from initial output, to define the end of an LED's life because the average human eye can't detect decreases in light levels up to that point when the light is used intermittently. Once
lumen maintenance has depreciated below that point, we begin to perceive the LED luminary is not as bright as it was when we first bought it and so become dissatisfied with its' use for home illumination. Since an L of 70 (30 percent lumen depreciation)
would be clearly unacceptable in more critical applications, such as traffic signal illumination, an even more stringent definition of low-light failure would be chosen. Whatever level of lumen depreciation is chosen for low-light failure, to be meaningful
to it's users, it should be in line with existing lamp technologies used in that industry.
In the case of motion picture lighting, I would argue that nothing short of a B50/L85 criteria would be appropriate and meaningful, since that has been our experience with both HMI and Tungsten Lamps (as noted above the rated average life is the
interval in which 50% of lamps fail and with an average lumen depreciation of 80-85%.) If we adopt this criteria for motion picture LED lighting luminaries, the rated lamp life in hours would be the interval in which a drop-off of 50 percent
of the diodes (B50) to 85 percent of their original value (L85) occurs. Without a doubt, this is a more meaningful criteria by which to judge the lamp life of an LED array for motion picture lighting applications.
Unfortunately, motion picture lighting manufacturers have not adopted this rating system - possibly because it would expose their exaggerated claims of 50'000 hrs as nothing more than marketing hyperbole. Short of hard data, how can we estimate
the useable life of an LED light-panel? One way would be to apply a B50/L85 criteria to the Caliper test results for similar style architectural LED luminaries - after all their diodes are cut from the same semi-conductor wafer and arrayed in similar style housings. Applying the
B50/L85 criteria to similar White Phosphor Array Type LED architectural luminaries suggests that the useable lamp life of similar type of LED luminaries designed for motion picture lighting applications is probably no more than 1500 hrs.
To put that in perspective, it is the equivalent of burning through two HMI globes. Since these types of LED fixtures have no interchangeable parts that can be replaced after reaching low-light failure, after 1500 hrs the fixture can only be
thrown away while an HMI head can be lamped with another bulb.
The Power Quality of AC LED Lights
Despite improved color rendering and significantly higher energy efficiency than incandescent lighting, the power quality of AC LED lighting has been a much less compelling story because of its reliance on Switch Mode Power. As was true of early electronic HMI ballasts, manufacturers of AC LEDs will have to address the relatively poor power quality generated by the Switch Mode Power Supplies (SMPSs) used in AC LED lighting ballasts before AC LED lighting can replace incandescent lamps in studios and on location sets powered by generators.
High Power AC LEDs use separate power supplies because they require more precise voltage/current management than traditional motion picture light sources. Unlike incandescent light bulbs, which illuminate regardless of the electrical polarity, LEDs will only light with correct electrical polarity. When the voltage across the p-n junction is in the correct direction, a significant current flows and the device is said to be forward-biased. If the voltage is of the wrong polarity, the device is said to be reverse biased, very little current flows, and no light is emitted.

.
While LEDs can operate on direct alternating current, this approach is unsuitable for motion picture lighting applications because it will cause flicker in the image. Since an LED only lights when forward-biased, when powered directly with alternating current they will only light with positive voltage, causing the LED to turn on and off at the frequency of the AC supply. As in the case of magnetic HMI ballasts, these pulsations of light will lead to flicker in the image unless both the power supply and camera shutter are tightly regulated. For this reason, LEDs used as a light source for motion picture production require direct current (DC) be applied to their diodes. To operate on AC mains power, LEDs need not only some type of AC-to-DC converter but also additional regulation of the DC to the diodes.

A small voltage change results in a exponentially large change in current.
LEDs require additional regulation of the DC to the diodes because the current drawn by LEDs is an exponential function of voltage. As illustrated above, a small voltage change results in a large change in current. It is therefore critically important that the right DC voltage be provided to the diodes. If the voltage is below the threshold, or on-voltage, no current will flow and the result is an unlit LED. If the voltage is too high, the current will go above the maximum rating, heating and potentially destroying the LED. To make matters worse, as an LED heats up, its voltage drop decreases, further increasing current. For these reasons, High Power AC LEDs require a high degree of power conditioning unlike incandescent light sources.

Left: The Cool Lights LED 600 Fixture. Right: Schematic diagram for an LED string with series resistor and linear voltage regulator.
Existing AC LEDs employ additional power conditioning in the head that is either a DC-to-DC Switch Mode Power Supply type (SMPS) with “constant current regulation”, or a Resistor Type with “linear voltage regulation.” While a resistor wired in series with a string of LEDs permits a linear voltage regulator to stabilize the LED current, this approach (used by Cool Lights and illustrated above) has several drawbacks. First, considerable energy is wasted in the series resistors. Second, the linear voltage regulator that converts the supply voltage to the desired voltage for the LED strings maintains a constant output by wasting excess electrical energy by converting it to heat. As such, this approach is highly inefficient and not ideal for battery operation. The same function is performed more efficiently by using DC-to-DC switched-mode power supply (SMPS) in conjunction with a constant current regulator in the light head.

Left: The Litepanel 1x1 LED Fixtre. Right: Schematic diagram for an LED string with constant current regulator.
The SMPS/constant current regulator approach, in contrast, regulates output voltage by rapidly switching a pass transistor (typically between 50 kHz and 1 MHz). In this approach (used by Lite Panels, Mole,
& Zylites and illustrated above) voltage regulation is provided by varying the ratio of “on” to “off” time of the transistor. Since transistors have no resistance when "closed" and carry no current when
"open" almost all the input power is delivered to the load; no power is wasted as dissipated heat. This higher efficiency is the chief advantage of switch-mode power supply when compared to a linear power
supply that dissipates excess voltage in the form of heat to regulate its’ output. In addition to enabling the total LED string voltage to be a higher percentage of the power supply voltage, resulting in improved efficiency and reduced power use, the highly regulated power provided by SMPS also stabilize the light output of High Power AC LEDs over the wide range of voltages provided by batteries as they discharge.

Figure 1(a): schematic diagram for a SMPS type AC-to-DC Converter that converts sinusoidal AC voltage to DC voltage to drive a LED.
Since, LEDs used in motion picture lighting require direct current (DC) be applied to their diodes, to operate them on AC mains power requires some type of AC-to-DC converter. Again, because of their higher efficiency AC-to-DC switch-mode power supplies are almost universally used for this purpose.

Litepanel 1x1s use the Cincom TR70A24 SMPSs Type AC-to-DC Converter (above right) which boasts a line regulation of +/- 1%, load regulation of +/- 2%, and an efficiency of 84%..
But, as Figure 2(a) below illustrates, the SMPSs used in AC LED ballasts can draw a very distorted current, and can result in current that is significantly phase-shifted with respect to the sinusoidal voltage waveform.
For instance, the AC power supply that Litepanels uses for their 1x1 panel arrays have a Leading Power Factor of 0.54 and generate high harmonic distortion (THD upwards of 68.1%). As such, the AC power supplies of LEDs can have an
adverse effect on power quality similar to that of CFLs described above.

Figure 2(a): Voltage and Current waveforms generated by SMPS type AC-to-DC Converter used to drive AC LEDs.
Like Fluorescent and HMI electronic ballasts, the power quality of SMPS-based AC LED ballast can be improved, but this comes at the additional cost of adding a power factor correction module to further condition and control the current drawn by the load. Unfortunately, the manufacturers of High Power AC LED Light fixtures for motion picture lighting applications generally do not give Power Factor specifications for their products. But, if the present state of Fluorescent and HMI lights is any indication, it is probably the case that the less expensive LED lights are not Power Factor Corrected, while the more expensive ones are Power Factor Corrected.

Distribution of harmonics generated by the power supply of the Litepanel 1x1 LED Fixtures. Note: predominance of the 3rd, 5th,
7th, and 9th harmonics that don't cancel on neutral returns
Versatility and Control
The final issue LED Manufacturers will have to address, before LEDs will be widely accepted in motion picture production, is their lack of versatility and control. The drawback to existing LED light panels is that their light falls off very rapidly and is hard
to control. These characteristics make LED light panels only suitable as Key sources in documentary interview set-ups where the Keys are typically positioned close to the interview subject. In that capacity LED light panels (with heavy diffusion) can generate
a wonderful soft light that wraps around the interview subject without wilting them. However, in dramatic set lighting, where Key sources must be capable of throwing a distance, LED light panels have only limited applications as fill sources. The broad soft
light they put out drops off too rapidly, and is too difficult to control, for them to be effective as a Key or Backlight source in dramatic set lighting.
However, progress is being made in the development of a LED light with the versatility and control of a traditional Fresnel instrument. In April 2010, Litepanels introduced a prototype for their Sola-Series LED “Fresnels” at NAB.
While definitely a step in the right direction in developing a production LED Fresnel light, the Litepanel Sola fixtures still don’t quite combine the advantages of LED illumination (cool-burning, energy-efficient) with the characteristics
of a traditional Fresnel fixture.

The 75W Liepanel Sola 6 LED "Fresnel"
With the Sola fixtures, Litepanels has not overcome the basic problems of LEDs discussed above. For instance, Litepanels claims the 75W Sola 6 (pictured above) has the output equivalent to a 650W Tungsten, but comparing the photometrics published on their website to those of an Arri 650 Fresnel, the Arri has nearly three times the
output of the Sola 6. Litepanels doesn’t give CRI ratings for the Sola Fresnels on their website, but when asked they say the CRI is in the 80s – which is
still rather anemic compared to other light sources. And, even though, Litepanels has improved the Power Factor of the Sola Fixtures over that of the 1x1s,
at about .75 (the 75W head draws a maximum of 100 Watts according to their technical specs.) it could stand further improvement (a Power Factor Corrected HMI has a Power Factor of .98 and Tungsten lights
have unity power factor.) And, while the Sola 6 has an impressive spot to flood range (10 to 70 degrees), spot/flood capability is not the only characteristic that makes a Fresnel light versatile. Of equal importance is the ability to render
clearly defined shadows and cuts. The ability of Fresnels to render crisp shadows make them ideal for creating gobo effects like window or branch-a-loris patterns. And, the ability of Fresnels to render clearly defined cuts enables their
light to be precisely cut to set pieces and talent. Finally, Tungsten & HMI Fresnels have sufficient output that the crispness of their shadows or the hardness of their cuts can be varied by simply adding one of a variety of diffusion
material to soften their output if desired. These are the characteristics of traditional Fresnels that make them extremely versatile, that the Sola "Fresnels" have not been able to emulate. To understand why it is so hard for LED manufacturers
to produce the qualities of a true Fresnel, let's look at those qualities in more detail and how they are achieved in traditional Fresnel heads.
The Quality of Fresnel Instruments
A Fresnel lens can be regarded as an array of prisms arranged in a circular fashion, with steeper prisms on the edges and a nearly flat convex lens at the center. The prisms near the center of the light source act as "dioptric" lenses that magnify and concentrate
the output of the lamp filament. At the same time, the multiple prisms mounted around the periphery of the lens (above, below, on one side and the other of the filament), act as "catadioptric" lenses that collect and intensify the light and redirect it in the same
plane as the dioptric lenses towards the center. In this fashion, a Fresnel lens bends the light of a source into a column of nearly parallel rays as shown in the illustration below.

Not only does a Fresnel lens refract the diverging rays of light emitted by a point source (lamp filament) into a highly collimated beam of light, but moving the point source toward the lens floods the beam - increasing its spread and decreasing its intensity.
Moving the point source away from the lens spots the beam, making it narrower and more intense.

At full flood, the beam is relatively even across a broad sweep (it has no central hot spot), then falls off quickly toward the edges, making for a very even field. As the lamp is spotted in, the rays become less divergent, more nearly parallel. The beam narrows
and gets brighter at the center, falling off rapidly on either side. At full spot, the usable portion of the beam is narrow, about a 10 degree angle.
A common misunderstanding is that the reflector collimates the light of a Fresnel head. In fact, the purpose of the reflector is to double the intensity of its' output. When the light-emitting filament of the bulb is placed near the center of
curvature of a spherical, concave polished mirror reflector, the reflecting surface creates an image of the filament. That image is located in the same plane, but slightly displaced from the filament itself. This has the effect of doubling the amount of light
forward projected from the locale of the lamp filament

In other words, without the reflector, "this reflector light" (the dashed lines in the illustration above) would have been lost in the back of the lamp housing. With a reflector, these rays of light are collected and sent back to their point of origin where they
emanate forward, parallel with the direct rays of light from the filament (the solid line in the illustration above), towards the back of the Fresnel lens where they are together collimated by the lens (for this reason the filaments of the bulbs used in Fresnel
heads are designed with an open geometry to minimize blocking of the retro-reflected light - making them not quite an ideal point source.) Now that all the light that emanated forward and back, emanates forward from a single point within the fixture (the filament
and its mirror image), the light projected forward is doubled. The efficiency of this lamp/reflector design, the collimated quality of it's light output, and the ability of the Fresnel lens to focus the rays of light quickly and easily to obtain a desired intensity or beam width, is what makes the Fresnel
head one of the most versatile fixtures to work with.
For example, a Fresnel head in spot position will "throw" light a great distance, meaning it will illuminate a subject to the same brightness at a much greater distance. This particular characteristic of Fresnel heads is very useful when they have to be used at a
distance. But, Fresnel heads are useful in the making of motion pictures not only because of its ability to focus the beam brighter than a typical lens. What makes them incredibly versatile is that in flood position they also generate light that is crisp and has
a relatively consistent intensity across the entire width of the beam of light.
Fresnels end up used in flood position a lot because that is where it creates its hardest, most delineated shadows (the flood/spot mechanism is often used for little more than to fine-tune intensity.) The more spotted in the fixture, the less sharp the shadow
lines appear. In full spot position, rays from the Fresnel travel more nearly parallel, but some converge slightly and cross one another. This creates fuzziness to shadows cast from an object. If one wants to project a sharp shadow or make a pattern (e.g. the
classic gag below of venetian blinds cast on a wall), one would want to use the light at full flood.

Another common application of a Fresnel in Flood is to create a consistent wash of light over a large area with multiple fixtures. For example, say that, to light a large room, several lights are required because the spread of one is not large enough. Fresnel
instruments spaced evenly apart along one wall of the room can do the job nicely, if the lamps are set at full flood, and the edge of the beam of each light (the 50% drop-off point) is overlapped slightly so that it feathers into that of the next. Overlapping
the beams in this fashion will create an even 100% intensity seamlessly across the whole room.
The highly collimated light of a Fresnel head will enable you to use barn doors to place the edges of the beam of light so that the light does not spill onto adjacent talent or set elements (if they are very reflective.) By closing the two large leaves of a
barn door into a narrow slit you can make a narrow slash of light. The slash can be horizontal - for an eye light for example - or turned diagonally to make a slash across the background. When a very confined, narrow, circular beam is desired, replace the barn
doors with a snoot. Snoots come in different aperture sizes so that you can adjust the beam width. You might use a snoot, for example, to light a set with small pools of light - lighting tables in a cafe for instance.
As an added bonus, it is fairly easy to calculate the intensity and beam diameter of a Fresnel because it has a focused beam (doing so for soft-lights is not so straightforward.) It is for these reasons, that the Fresnel head is still probably the most commonly
used fixture in motion picture production.
LED Fresnels
There are two big hurdles to manufacturing a LED Fresnel head of a practical size - say, the equivalent of a 650W Tungsten Fresnel. First, Fresnel lenses require a point source of light. Second, they are not very efficient and so require a lot of light.
Unfortunately, at this time there is no single-diode LED with sufficient output to serve as a point source for a Fresnel lens, nor will there likely be one in the near future. To understand why that is, let's look at these hurdles in more detail.
At 15 lumens/watt, a 650W tungsten globe will generate 9'750 lumens. But, given the doubling effect of the Fresnel head's highly polished spherical reflector, nearly 19'500 lumens is forward projected onto the back of the Fresnel lens from a relatively
localized source (given the open geometry design of the bulb's tungsten filament it is not quite a point source.) If we take even the brightest LED that exists today, the newest addition (as of 5/11/2011) to the CREE XLamp LED family that in lab tests
generated 231 lumen/watt, it would require an 84.4 Watt LED of this efficiency to match the forward projection of that achieved by a 650W tungsten filament in front of a highly polished spherical reflector. Even if Cree can maintain that efficiency in
what is presently the largest commercially available single-die component LED available, 10Watts, we are still looking at an LED array of at least nine LEDs to equal the forward projection of a 650W tungsten filament in front of a highly polished spherical reflector.
Another reason we are not likely to see a single diode LED with sufficient output is that it is highly unlikely that Cree can maintain that level of efficiency in practical application as the efficiency was optimized at 350mA in the lab test, and had a
correlated color temperature of 4500K. By the time that technology is scaled up to a 10W single-die component LED, and phosphors are added to extend the color temperature to 3200K, you can be sure the end product will generate no where near the same
lumen/watts. Put in perspective, we are still a long way off from having a single-die LED with sufficient output and correlated color temperature to match a 650W tungsten filament in front of a highly polished spherical reflector.
To make matters worse, the inefficiency of Fresnel lenses increase as the source of light diverges from that of an ideal point source. For example, given their open geometry, tungsten lamp filaments don't nearly approximate a true point source. As such
light rays enter the prisms of a Fresnel lens at different angles (angles of incidence), and because some undergo multiple reflections or refractions or are totally internally reflected for this reason, not all of them emerge on the other side of the array.
The width of the vertical step between grooves in a Fresnel lens also block light. This loss does not exist for rays parallel to the optical axis of the grooves. But, for rays making a large angle (20 degree or greater) with the optical axis, the loss can be
significant. The more the source departs from an ideal point source, the greater the angles of incidence, the more light that is blocked by the steps. The more the light source approaches a point source, the more the light output favors the central portion
of the lens, which has greater transmittance. Since there is no single-diode LED with sufficient output to serve as a point source for a Fresnel lens, by default LED "Fresnel" fixtures have to use an array of LEDs. Far removed from an ideal point source,
an LED array not only increases the inefficiency of a Fresnel Lens (requiring a larger array) but also changes the quality of its light output from the collimated source that is desired.



The ARRI L7 LED Fresnels
Regardless of the difficulty, Arri seems to have developed a true LED Fresnel in their new L7 series LED Fresnel heads. At NAB in 2011 Arri introduced the first of their L-Series LED Fresnels: the L7-D, L7-T and L7-C. All three models share the same basic housing and the same 7" Fresnel lens, and all have output comparable in intensity and quality to a conventional 1K Fresnel.

As you can see in the pictures above, that compare the output of the L7 Fresnel to an Arri ST-1 Quartz Fresnel, the L7 Fresnel has clear and defined shadow rendering capability like that of the ST-1 Quartz Fresnel. And, as the pictures below demonstrate, the L7 Fresnel has a spot to flood range similar to that of the ST-1 Quartz Fresnel and excellent field homogeneity in both flood and spot.

And, just like the ST-1 Quartz Fresnel (pictured below), the beam of the L7 Fresnel (pictured above) is easily controlled with barndoors - enabling the light to be precisely cut to set pieces and talent (see far right photos above & below.)

And, given the discernable amount of light the L-Series Fresnel prototypes threw in a show demonstration video from IBEC in the fall of 2010, on what appears to be a 6x6 Ultrabounce rigged 20’ overhead, and under the high ambient light levels of the show hall, it seems the production model L7 Fresnel has more than enough output to waste some to diffusion and color gel if one so desires (a shortcoming to most LED panels is that they have barely enough output – and certainly none to waste.)

Since the L7 fixtures are in the proto-type stage (production models are due soon), Arri is being very reticent about how they are able to accomplish the characteristics of a true Fresnel from a multi-emitter driver. To speculate, I would have to guess they are using
a simple lens system - possibly like the one illustrated below.

By moving a Fresnel lens forward and back in relation to an assembly consisting of an LED Array and a Condenser Lens with an extremely short focal length, the focal point of the Condenser lens moves in relation to the Fresnel lens much like the lamp/reflector
assembly of a traditional Fresnel Head. This would have the effect of spotting and flooding the light output of the LED Array much like a Fresnel spots and floods the output of a point source. Of course this is nothing but speculation, until we are able to get
our hands on an actual production model of the Arri L7 LED Fresnel.
Where the L7 models differ is in terms of color temperature. The D model outputs a daylight-equivalent 5600 K, the T model a tungsten-equivalent 3200 K, and the top-of-the-range C model offers total color control.
With the L7 series, Arri achieves the best color rendition I have seen yet from a multi-emitter fixture. By blending color with a highly sophisticated LED engine, the L7 series is able to overcome the generally poor color rendering
capabilities of other LED fixtures (both remote phosphor and multi-emitter.) Both the 3200 K and 5600 K color temperature models offer a CRI and CQS greater than 90 so skin tones, costumes and scenery appear more life-like.
The L7-C's fully tuneable white light can be adjusted for different skin tones, camera sensors and mixed-light environments, while specific color shades can be matched through full gamut color mixing. Unlike other LED fixtures, this level of color
control does not involve compromising the quality of the light field: the L-Series is unique in combining uniform light and single shadow rendition with absolute control of color attributes.

Split Macbeth chart: each color patch shows the visible effects of studio tungsten light in the top half of the patch, and a representative multi-emitter LED lighting instrument
in the bottom half. Note: this is not the L7 but results typical of the best of the multi-emitter LEDs up to the release of the L7s.
An added benefit to using a color blending multi-emitter LED engine is that the mix of different color emitters can be adjusted to compensate for the
inevitable color shift and diminished output of the LEDs with age. Using an internal optical sensor, the L7's firmware performs this calibration function at switch-on thereby
assuring consistent realistic color rendition throughout the fixture's life and between fixtures - which means there won't be a variance in color between fixtures when talent walks
out of one key and into another, or when using multiple L7s to create a wash up a cyc or backdrop.

There are two alternative cooling systems: one passive and the other active. The passive cooling system was designed for broadcast studios. It incorporates no moving parts or fans and is therefore completely silent. The active cooling system was designed to provide a more compact and lightweight option for location work. It uses an extremely quiet (<20 dB) fan and weighs 10lbs less than the studio version.

The location fixture carries an IP54 rating for weather resistance which means that it is protected from falling rain and splashing water, and that the internal electronics, optics and LEDs are protected from dust, dirt and humidity - making it a very robust fixture that will stand up to the rigors of location production.

All the L7s feature Power Factor Correction with a near unity Power Factor of .91. Which means that the 200W fixtures will draw no more than 1.98A at 120V (220W) and cause virtually no Harmonic Distortion.
Since it creates virtually no line noise, you will be able to power nine 200W L7s on the 20A circuit of a portable generator without a problem.
To assure that they are not quickly rendered obsolete by the rapid advances being made in LED chip efficiency, the Arri L-Series LED Fresels are designed to be an expansible platform, with replaceable parts, that can incorporate
future developments in LED technology. Not only, do the heads allow for the incorporation of more efficient LED chips when they become available (or when the lumnen output of the original ones drop), but the light engine is also
fully upgradeable, ensuring that the fixtures can take advantage of technology advances as they happen. To accommodate future control protocols (such as ANC), their firmware is also upgradeable through the USB port on the rear of
each unit. They will also be compatible with planned future optic accessories that will expand the L-Series versatility. Able to incorporate future developments in LED technology, the expansible platform of the L7s ensures that
they will have a long useable life and so will assure a return on investment in them. Given the rapid pace of LED Chip development, I can't think of another LED fixture that won't be obsolete in a year or two.

Given the output, the clear and defined shadow rendering, the excellent field homogeneity and the color rendition demonstrated in the show video,
it is evident that Arri has finally engineered the first true production LED Fresnel light (see the 2010 IBEC Show video below or the
NAB 2011 Show Demo for more details (the 2010 IBEC Show video below demonstrates the light quality better, I think.))
Light Emitting Plasma (LEP) Fixtures
Light Emitting Plasma (LEP) is radically new technology that can produce 144 lumens per watt. In contrast, Tungsten Halogen bulbs produce 15 lumens per watt, LED emitters produce between 65 to 85
lumens per watt (in practical applications), and HMI bulbs produce 90 Lumens per watt. In addition to their intense "flicker-free" output, LEP lamps provide a continuous spectrum that is almost identical to Daylight,
long life, and a ruggedness that outperforms other lamps. These characteristics of LEPs make them an ideal source for motion picture lighting applications.

One way to think of a LEP bulb is as a tiny (less than 9 millimeters) discharge lamp. But, unlike an HMI bulb it does not have electrodes. Instead of applying a voltage and drawing a current through the
lamp to create light as does an HMI, the energy that creates light in an LEP comes via a high frequency RF transmitter. The RF waves heat the materials inside the lamp and bring those materials to a
plasma state so that the lamp emits a "flicker-free" light.

The Photon Beard Nova 270 (left), a "Hive" of Hornet 180s (center), and the Helio 270 (right.)
At present there are three motion picture LEP lamp heads on the market: the Photon Beard Nova 270, the Helio 270, and Hive Lighting’s Hornet 180 pictured above. All three lamp heads use the same Luxim
Plasma Emitter behind Fresnel lens. The Photon Beard Nova 270 and Hive Hornet 180 can be operated on batteries at 28 Volts or off a Universal (90-305Vac, 50/60Hz) AC power supply (the power supply is
separate in the case of the Photon Beard Nova 270. The Helio 270, by comparison is a stripped down, more robust location production instrument that offers a built-in 120V/60Hz AC power supply (no DC option)
with near unity (.99) Power Factor. As such, the Helio 270 is nearly half the price of the other two heads.
How LEPs work

Like an HMI, the LEP bulb is made of quartz and filled with an inert gas, Metal Halide salts, and a very small amount of Mercury. The bulb is partially embedded in a ceramic disc attached to a finned heat sink.
The package consisting of the bulb, ceramic disc (puck), and heat sink is called the “emitter,” and acts as a resonant cavity for the RF energy and the source for the light emitting plasma. A separate “driver”
amplifies high-frequency energy, that a "resonator" focuses on the plasma. The radiated energy ionizes the gas in the quartz envelope and free electrons, accelerated by the electrical field,
collide with the gas and metal atoms, creating a plasma ball. Some electrons circling around the gas and metal atoms are excited by these collisions, bringing them to a higher energy state. When the electron
falls back to its original state, it emits a photon, resulting in visible light. Since the excitation of the plasma is at very high frequency (> MHz), thousands of times faster than film or shutter speeds, the light
output is "flicker-free" at all speeds and shutter angles.

Like an HMI, the stages of excitation are demarcated by changes in the color and intensity of the light put out by the emitter. Upon ignition, as the electric field ionizes the gas molecules, the lamps emits a dim
purplish light which gets gradually brighter of over a period of about 8 seconds as the plasma grows. When the plasma reaches sufficient power to vaporize the Metal Halide salts there is a half second flash of blue
light, that gives way to a bluish white as the salts begin to join the plasma. As more and more of the Metal Halide salts join the plasma the light output grows to an extremely intense full spectrum white light of
about 5300 degrees Kelvin. The whole ignition process takes no more than 20 seconds.
This different method of transforming electricity into light has multiple benefits over the conventional way it’s done in HMI and LED luminaries.
Near perfect CRI (94+): colors are more vibrant and natural looking.
Continuous color spectrum: colors reproduce accurately on screen. Color meters are able to make accurate CT and green/magenta readings
Longer lamp life: an LEP bulb will run 7 times longer than an HMI bulb before exhibiting the same lumen depreciation. Unlike LED fixtures, the color temperature of an LEP bulb
drops just 500 degrees Kelvin in 10’000 hours.
More efficient uniform light output: The pill sized LEP bulb is an almost ideal point source for Fresnel type heads.
Increased energy efficiency: a LEP fixture uses 75% less power than a comparable HMI fixture.
Greater light output: a 273 W LEP fixture has a light output comparable to a 575W HMI.
"Flicker-Free" at all speeds: continuous output that is not dependent on line frequency
Quiet Operation: unlike LED Fresnels there are no cooling fans.
Compact & Robust:
since the plasma light source is very compact, head designs are more compact with greater performance than larger ones.
Let’s look at some of these benefits over HMI & LED luminaries in more detail.
Color Rendering
LEP lamps have very high CRIs (94+.) But, more important than their high CRI ratings, LEP lamps generate light with a continuous color spectrum. If we compare the spectral power distribution graphs of natural
daylight and LEP lamps below, we see that, except for very brief drop outs at approximately 410 nm and again at 451 nm, the light output of LEP lamps is almost identical to natural daylight.

As can also be seen in the spectral distribution graphs above, Plasma lamps have a much more continuous color spectrum than even the best LED luminaries on the market today. For instance, LEP lamps, unlike LED lamps,
generate light at wavelengths shorter than 425nm - which means that violet colors render well. And, unlike LED lamps, LEP lamps also output in the medium blue-cyan-turquoise range from about 465-510nm so aqua-type
colors render well by comparison. Skin tones and warm, amber-yellow colors stand out under LEP lamps because of the strong presence of their complementary colors. And, since the output of LEP lamps extend all the
way out on the long-wavelength end (well beyond the 600 nm cutoff of LEDs), pinks, reds, oranges, and other long wave-length colors look vibrant under LEP light where they tend to look a little dull under LEDs. As a
continuous spectrum source, colors not only appear more natural and vibrant under LEP lamps than under LED lamps, they also reproduce more accurately on the screen since, as is also evident by the spectral distribution
graphs above, the output of LEP lamps matches the spectral sensitivity of film emulsions and digital sensors. Plasma lights deliver the same true-to-life color rendition previously achievable only with full-spectrum
Daylight or HMI sources.
As an added bonus, color meters, like the Minolta III F, that make their calculations of the Color Temperature (CT) based on a light sources continuous spectrum, are able to generate accurate reading of the CT and Green/Magenta of LEP lamps. As we saw above, color meters are completely useless with LEDs.
Lumen Depreciation, Color Shift, & Lamp Life
In contrast to HMI lamps that use electrodes connected through the quartz envelope to transfer the energy necessary to vaporize the metals in the envelope, a LEP lamp radiates the energy through the quartz envelope. Eliminating electrodes in this
fashion offers several real benefits. First, since, electrode deterioration is usually the limiting factor in the lamp life of HMI bulbs (the gap between the electrodes widens to the point that the ballast can not create enough electrical potential
to jump it), LEP bulbs last much longer - between 65,000 and 100,000 hours before ignition failure. Second, with no electrodes to deteriorate and blacken the inside of the quartz envelope, a LEP bulb exhibits very little lumen depreciation over
its long life. Finally, the cooler ignition and operating temperatures at which LEP lamps operate greatly reduces the devitrification of their quartz envelope. The end result is that LEP lamps remain brighter longer and have much better lumen
maintenance than even LED luminaries.

Without electrodes, there is also no arc gap in an LEP lamp, as there is in an HMI globe, that widens over time and results in an increase in arc voltage and on some ballast types an increase in lamp power that results in a drop in color temperature.
Even more significant are the complex chemical reactions between the electrodes (again not present in LEP) and metal halides which also result in color shifts. As a result the color temperature in LEP lamps is much more consistent over longer spans
of time - dropping in 10’000 hrs as much as a HMI bulb does in 500 hrs. Like LEDs, LEPs will keep on producing light at declining levels but at a much more gradual rate and shift in color. For this reason, it is more practical to measure the useable
“lamp life” of an LEP using the same criteria as an LED rather than that used for conventional lamps like HMIs.

If we apply the same L85 criteria to LEPs that we applied to LED lighting luminaries, their rated lamp life would be an unparalleled 5000 hrs (compared to 750 for HMIs and approximately 1500 for LEDs.) In other words, the interval in which the output of an LEP drops-off of to 85 percent of its’ original value (L85) is 5000 hrs. Unlike an LED, the bulb of an LEP can be replaced after reaching low-light failure, so the fixture does not have to be thrown away.
With such imperceptible drop in color temperature and lumens over their useable life, LEP lamps offer many practical benefits that HMI & LED lights do not. For example, it is possible for head manufacturers to compensate for variances in bulb manufacturing by “tuning” their output to exact specifications so that there is very little deviation between heads. If “tuned”, the lumen maintenance of LEP bulbs is such that, there will be hardly perceptible differences between lamps - even between ones with old and new bulbs. HMI lamps, do not offer the same possibility.
Why would there be a variance between new bulbs in the first place? In the manufacture of both HMI and LEP bulbs, the manufacturer must dose (fill) their bulbs with tiny quantities of numerous chemical elements and metals. Because this is extremely
difficult to do consistently in a manufacturing process, there are inevitably differences in color temperature from bulb to bulb right off the production line. For example, after many years of manufacturing HMI bulbs, Osram is still not able to
dose HMI bulbs so that they match in color temperature or CRI. While the quality control of LEP bulbs is better, there is still some variance in the color temperature from bulb to bulb right off the production line.
What makes it possible to tune LEP bulbs, but not HMI bulbs, is the fact that their color temperature rises very rapidly when they are dimmed even slightly. While this is a disadvantage if one wants to dim the lamps (scriming is recommend instead),
manufacturers like Helio take advantage of this characteristic of Plasma to individually "tune up" their heads to a consistent 5500 degree Kelvin without an appreciable loss in output (HMI lamps, do not offer the same possibility.) Once tuned, the lumen depreciation of LEPs, compared to other light sources, is such that there will be hardly perceptible differences between old and new bulbs.
After tuning the color output of their heads, the almost imperceptible drop in color temperature and lumens over the useable life of LEP bulbs, means that the Helio LEP lights offer many practical benefits that HMI & LED lights do not.
For instance, the consistent color of a tuned LEP lamp assures that the color of wardrobe and skin-tones will not change as talent steps out of one Helio 270 Key and into another. Or, that there will be inconsistencies in color between Helio Space
Lights when multiple fixtures are used to wash a wall or cyc. Finally, LEPs in general do not require the active microprocessor color control that is required to assure consistent color rendition in LEDs. Absent such microprocessor based color
management systems, LEP fixtures like the Helio 270 can be considerably less expensive and more robust than LED luminaries. The biggest cost benefit to LEP lights in general, and the Helio 270 in particular, has got to be the savings in not having
to replace lamps every 750 hrs (HMIs) or the entire fixture when its' emitters reach low light failure (LEDs.) Where a 575w HMI globe typically retails for approximately $150.00, the 5000 hr L85 lamp life of an LEP bulb is equal to seven HMI globes, which amounts to a savings of $1050.00, or nearly half the cost of the Helio 270 Plasma lamp head.
LEPs and Fresnel Lenses
Efficient and very compact, LEP bulbs work extremely well in Fresnel type optical systems. The result is more light output, of a better quality, for less power consumption, when compared to HMI and LED light sources.

The Helio 270 with Luxim LIFI Plasma Emitter and 175mm Fresnel Lens
When the pill sized LEP bulb in mounted in the puck, the emitting area is no more than 1/4" x 1/4"
and all of its’ output is forward directed within a 60 degree angle. In this configuration, the 273W LEP bulb will deliver 14000 lumens. Such a highly localized forward directed light
is ideal for Fresnel type instruments.

As close an approximation to the ideal point source that exists today, fewer of the light rays emitted by an LEP bulb are lost in or blocked by the facets of a Fresnel lens. The reason for this is that a greater proportion of the light output of an LEP bulb is on the optical axis of the lens, and therefore fewer of the rays will be blocked by the vertical steps between the grooves in the lens. And, since more of its light rays enter the prisms of the lens on axis, fewer undergo multiple reflections or refractions or are totally internally reflected. Finally, where an LEP approaches an ideal point source, its light output favors the central portion of the lens, which has greater transmittance. For these reasons, 90 percent more of the output of an LEP lamp will be transmitted through a Fresnel lens than that of a tungsten filament lamp, making it a more efficient system. For these reasons, LEP emitters (unlike LED arrays) make an almost ideal source for Fresnel instruments.

The light output of LEP Fresnels, like the Photon Beard Nova 270 or the Helio 270, is highly collimated, very clean and crisp making it great for cutting shadows or gobo effects. It is easily controlled by barn doors and flags and so can be easily cut off highly reflective set elements.

It’s light field in flood is uniform across a wide angle making it ideal for lighting large areas, and it can be spotted to throw light a great distance. These characteristics of LEP Fresnels, make them extremely versatile and much better than LED panels to serve as a Key or Backlight source in dramatic set lighting.
Power Efficiency
A LEP bulb can produce 144 lumens per watt. In contrast, Tungsten Halogen bulbs produce 15 lumens per watt, LED emitters produce between 65 to 85 lumens per watt (in practical applications), and HMI bulbs produce 90 Lumens per watt. This unparalleled light output, coupled with the greater efficiency it brings to Fresnel lenses as a result of its approximating an ideal point source, make LEP Fresnels the most efficient Fresnel lamp heads available today by far.

For instance, the Helio 270 LEP lamp head draws only 2.27 Amps at 120V, yet has an output comparable to that of a 575W HMI. That works out to be 75% less power than the 9 Amp draw of a 575W HMI with standard
electronic ballast. A number of practical benefits come as result of the efficiency of LEP technology.
In studio applications, the greatly reduced power consumption of LEPs translates into greatly reduced costs in the build out and operation of studios. Not only is the electrical service required greatly reduced, money is also saved on
the power bill. With higher efficiency, the lamp head draws less power, the fixture produces less heat, and so the studio requires less A/C, which means even less power consumption.
On location, you will be able to generate more light on standard wall circuits and generator circuits than has ever been possible before. Able to operate eight 270W LEP instruments on a single 20A circuit, LEP technology
makes it possible to get the output of a 4k HMI from a single wall or generator outlet. When it comes to operating lights on portable gas generators, the greater efficiency of LEP technology is only half the story.
The other half is the fact that LEP lamps, like the Photon Beard Nova 270 and the Helio 270, are Power Factor Corrected (PFC.) The power supply used in the Helio 270, for example, has a Power Factor of .99, making it a near linear load. As a result, the Helio 270 uses power more efficiently, minimizes return current, and generates virtually no line noise.

As the oscilloscope shots above comparing the current and voltage waveforms of the PFC Helio 270 with an equivalent wattage of non-PFC LEDs illustrates (current is represented here as the voltage drop on a 1
Ohm resister), the PFC circuit of the Helio 270 reduces the amount of current drawn, aligns it with the voltage, and induces a smoother power waveform. For these reasons, the PFC power supply of the Helio 270
enables a portable gas generator to operate more heads than it could otherwise. Where, as we shall see below, it is as much the Harmonic Noise that non-PFC HMI, Fluorescent, and LED power supplies (ballasts)
kick back into the power stream, as it is their higher Apparent Power, that limits the total number of them that can be reliably operated on conventional generators; the efficiency and near unity Power Factor
of the Helio 270 means that you can operate more of them on portable gas generators. For instance, you can operate four 575W HMIs on a 6500W portable AVR generator, where you can operate 23 Helio 270s (each
with an output comparable to a 575W HMI). And, if the generator is one of our modified Honda EU6500is Inverter generators, you will be able to operate up to 27 Helio 270s on its enhanced 7500W output. I think
you would have to agree, that is a major increase in production capability (use this link for details.)
A Robust Location Light Source
Plasma emitters use solid state, hardened components that improve their reliability under harsh location production. Plasma bulbs are rugged and vibration resistant, and so will not break or explode inside expensive lighting heads. Since the LEP emitter is extremely compact, in the case of the Helio 270 the emitter, driver, and power supply all fit in the lamp head, eliminating the need for a separate ballast connected by header cables (the acknowledged Achilles heel of HMI systems.) Finally, with much lower UV emissions, LEPs do not require elaborate and ultimately finicky safety switches. In total, LEPs have an order of magnitude better reliability than conventional HMI lamps while offering the intense beam and the colorful spectrum needed for stage, studio and theatrical lights.
Conclusion
Where we are a long way off from having a single-die LED with sufficient output and correlated color temperature to match HMIs, LEP lamps are the most cost effective alternative to expensive HMI Fresnel systems when
it comes to generating daylight balanced light. This feature of LEPs benefits Red users, as well as users of DSLRs, in particular.

The Helio Space Light with three 270 Luxim LIFI Plasma Emitters has a daylight balanced output equivalent to a 6kw Tungsten Space Light
One downside to lighting for the 5000K native color balance of CMOS sensors in the past has been that it requires an all 5000K balanced lighting package and HMIs are considerably more expensive to buy or rent than
other light sources and not available in popular studio configurations like Space Lights. Kino Flo fixtures, particularly the Parabeams, are a cost effective alternative to HMIs because they can use either 3200K or 5500K tubes. But, the drawback to
fluorescent fixtures (like LED fixtures) is that they generally have a very broad soft light output that drops off rapidly which means the units need to be positioned close to the subject they are lighting. This characteristic has always made them
better suited to lighting documentary interviews than dramatic scenes.
With a 5300K output comparable to that of a 575 HMI Fresnel, the Helio 270 in particular offers the same benefit of being a less expensive alternative to HMIs, but also offers the added benefit of being more versatile than a Kino Flo or LED fixture.
Not only does it offer the capacity of traditional Tungsten/HMI Fresnels to throw and control its light output (making it a more suitable Key and Backlight source for lighting dramatic scenes), but it also has sufficient output to bounce it or waste
some output to diffusion material to make it softer (existing LEDs put out barely enough, with none to waste.) Plasma technology in general is proving to be a better fit with CMOS Sensor based imaging systems, especially for studio lighting applications, than both LED and HMI.
LEPs offer the capacity to provide both hard crisp light that will throw a distance and is easily controlled, as well as offer soft light in Space Light configurations, making it more versatile than Fluorescent, HMI, or LED light for daylight balanced studio production with CMOS sensors.
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Review
To review, the lighting loads placed on generators fall into three basic categories. The tungsten filament of lncandescent lights have no inductive or capacitive properties, but merely create resistance in a circuit.
The voltage and
the current are in-phase, meaning that the peaks and valleys of their sine waves will occur at the same time. A purely resistive load has a power factor of 1.0 (also
called a unity power factor or 100% power factor). When an AC load involves coils, such as those in a magnetic HMI ballast, it creates inductance as well as
resistance. When there is inductive reactance present in a load (an induced current that opposes the flow of the primary current), the phase of the current will be shifted so that its peaks
and valleys do not occur at the same time as those of the voltage.

Voltage/Current phase syncrhonization of lighting loads: Incandescent Lights (top), Magnetic HMI Ballast (middle), non-PFC HMI Ballast (bottom)
Inductive reactance causes current to lag behind the voltage. The degree to which the two waveforms (current & voltage) are put out of phase depends on the relative amount
of resistance and inductance offered by the transformer and the number of capacitors built into the ballast to counter the inductance. The more they are out of phase, the
lower (poorer) the power factor (with a PF commonly between .7 and .9.) If the load has a large capacitive component (electronic ballasts), capacitive reactance (the return of unused portions of the current waveform) likewise
puts voltage and current out of phase. However, capacitive reactance acts on the waveform in a way opposite to inductive reactance. It causes current to lead voltage. Again, the more the
two wave forms are put out of phase, the lower (poorer) the power factor (with a PF commonly below .6.)
As we have seen, when a sinusoidal voltage is applied to a load through a distribution system, the load, depending on its Power Factor, may or may not affect the quality of the current traveling though the system.
With an incandescent light (a resistive load), the current drawn by the light is proportional to the voltage and impedance and the current waveform follows the envelope of the voltage waveform
having a negligible effect on the quality of power in the distribution system. This type of load is referred to as a linear load (loads where the voltage and current follow one another without
any distortion to their pure sine waves).
ILLUSTRATION COURTESY OF ELECTRICAL CONSTRUCTION & MAINTENANCE (ECM) MAGAZINE

Shown are plots of different linear load currents, Ip is a pure resistive circuit current. IL is a partially inductive (lagging) circuit current. IC is a partially capacitive (leading) circuit current.
In contrast, loads like magnetic and electronic HMI and fluorescent ballasts, return current in the form of secondary currents that put the primary current out of phase with the voltage. These loads are classified as
nonlinear loads. Where it is these harmonics that affect the operation of our production equipment, a basic understanding of harmonics is essential to providing safe and reliable power on set.
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Harmonics
Harmonic Basics
When dumped back into the electrical distribution system of a generator, harmonic currents can combine with the fundamental (60 Hz) current to create distortion of the voltage waveform similar to what can be seen below.

When looked at on an oscilloscope, the current waveforms of nonlinear loads appear like the non-sinusoidal waveform above because they contain additional waveforms of the secondary currents superimposed upon the primary sinusoidal current waveform, creating multiple frequencies within the normal 60-Hz sine wave. The multiple frequencies are harmonics of the fundamental frequency.

Undistorted Fundamental Pure Sine Wave
The current sine wave above represents what is called the fundamental wavelength. This is how the power waveform should look on an oscillosocpe in an ideal
situation. However, in practicality nothing is ever ideal. For example, as we saw above, solid state electronic components found in electronic HMI and Kino
Flo ballasts use only portions of the sine wave. These devices then return the unused portions as harmonic currents.

Isolated Fundamental and its' Third Harmonic
The harmonic currents that have the most adverse effects are the high frequency odd number multiples of the original frequency. With 60Hz power, the 3rd order harmonic
will be 180Hz and the 5th order will be 300Hz, and so on. While modern test equipment is able to detect up to 63 orders of harmonics, there is no doubt among electrical engineers that there are higher frequencies present that are undetectable. The
diagram above shows the fundamental sine wave (in blue) and the third order harmonic (in green) together for comparison.

Third Harmonic superimposed on Fundamental as it would appear on oscilloscope.
When the wave is measured on an oscilloscope, it will not appear as two waves but one (depicted above in blue.) The harmonics are super-imposed onto the
fundamental wave creating a ripple effect. These ripples are known as harmonic distortion. Below is a diagram showing the fundamental and 3rd order harmonic
waves super-imposed for the two predominant types of non-linear lighting loads - inductive and capacitive.
ILLUSTRATION COURTESY OF ELECTRICAL CONSTRUCTION & MAINTENANCE (ECM) MAGAZINE

The waveforms on the left illustrate the effect of the 3rd harmonics of capacitive loads (where current leads voltage) like the SMPS-based ballasts used for
HMI, fluorescent, and High Output AC LED lights. The waveforms on the right illustrate the effect of the 3rd harmonics of an inductive load (where current lags voltage) like
the magnetic ballasts of older HMIs and fluorescent practicals.
If we were to add the effect that the 5th, 7th, 9th, etc. harmonic currents would have on the waveform, we would see a further distortion of the waveform
from its' ideal sinusoidal shape. In the case of highly capacitive non-linear loads like electronic HMI ballasts, we would see a further squaring off of the power waveform.
The Adverse Effects of Harmonics
Voltage Waveform Distortion
In theory, each harmonic current in an electrical distribution system will cause a voltage at the same harmonic to exist when the harmonic current flows into an
impedance. For example, a 5th harmonic current will produce a 5th harmonic voltage, a 7th harmonic current will produce a 7th harmonic voltage, etc.
Because a distorted current waveform is made up of the fundamental plus one or more harmonics currents, each of these currents flowing into an
impedance will, in theory, result in voltage harmonics appearing at the load bus, a voltage drop, and distortion of the voltage waveform.

Each harmonic current in the electrical distribution system will cause a voltage at the same harmonic to exist when the harmonic current flows into an impedance.
As can be seen in the illustration above, voltage distortion will be greatest at the loads themselves, since the harmonic currents are subjected to the full system
impedance (generator, cables, etc.) at that point. In other words, the voltage will be the least distorted nearest to its source and will become more distorted
nearer to the load, where the harmonic current encounters the greatest impedance. This is a characteristic most often misunderstood about distribution systems
with a high THD. It means that even if voltage distortion levels are low at the power source, they can be unacceptably high at the loads themselves.
In practice, when you plug a HMI light into a wall outlet you need not be concerned about current harmonic distortion producing voltage distortion. However, it is an all together different situation when plugging a HMI into a small portable generator. That is because the magnitude of voltage waveform distortion in a distribution system depends upon three factors: the impedance of the power system, the quality of the original applied power waveform, and the relative size of the nonlinear loads with respect to capacity of the power generating system. Let’s look at each one of these factors in more detail.
Inherent Applied Voltage Waveform
A pure sinusoidal voltage, like the one represented below, is a conceptual quantity produced by an ideal AC generator built with finely distributed stator
and field windings that operate in a uniform magnetic field.

Since in reality neither the winding distribution nor the magnetic field can be uniform in a working AC generator (not even power plant generators), voltage waveform distortions exist, and the voltage-time relationship deviates from our conceptual pure sine function. Typically, the distortion of grid power is very small (less than 3%), but nonetheless it exists.
WAVEFORM ILLUSTRATIONS COURTESY OF HONDA POWER PRODUCTS

Waveforms Left to Right: Grid Power, Brushless Generator, AVR Generator, MSW Inverter Generator, PWM Inverter Generator
As we saw at the outset, it is an all together different situation when it comes to generators. Since, there is a direct trade off between generator cost and quality of the power waveform, voltage distortion in the original power waveform varies greatly between the types of generators (see representative waveforms above and chart below.)

ILLUSTRATION COURTESY OF HONDA POWER PRODUCTS
Total Harmonic Distortion Values for original waveforms of Brushless (blue), Conventional AVR (green), Inverter (red) generators.
System Impedance
Since harmonic currents react with impedance to cause voltage drop, the magnitude of a voltage waveform distortion caused by a non-linear current demand is a function of the source impedance. In the case of generators, source impedance is not an easily defined value as generator reactance varies with time following a load change.
However, what is certain is that the generator with the lowest internal reactance to an instantaneous current change at a given load will typically have the lowest value of total harmonic distortion under nonlinear load conditions.

To visualize why this is the case, imagine a birds eye view of a 1400 Amp Crawford Studio Unit parked on top of the Hoover Dam next to a Honda EX5500 portable gas generator with Barber Coleman
frequency governor. If you had 2ks plugged into each power source and switched them on at once. Which generating source would be affected the most? The change in load would have no effect on the
turbines of the hydroelectric generating plant. Given the force exerted by millions of gallons of water driving the turbines and the inertia of their mass, they would not be disturbed at all by a small load change.

In the case of the Crawford 1400A Studio Unit, switching on a 2k might create a very slight momentary fluctuation in the engine speed of the 1400A Crawford. But given the mechanical inertia of its large diesel engine and the sophistication of it governing systems, the effect will be negligible. However, given the small mass of the Honda EX5500’s engine and the relative simplicity of its’ governing systems, switching on a 2k load will cause the Honda EX5500 engine to fluctuate for several seconds as the voltage and frequency governors adjust for the change in load.

While exaggerated, this example demonstrates why, depending on the size and design of the generator, it may have 5 to 100 times greater internal reactance to an instantaneous change in load than a power grid transformer. Consequently, non-linear loads which work fine on utility power, will react entirely different when powered by a generator set. And, the generator with the lowest internal reactance at a given load will typically have the lowest value of total harmonic distortion under nonlinear load conditions.
For this reason, voltage waveform distortion as a result of harmonic currents is not a problem on grid power and is for the most part not a practical problem on large film sets. In practice, when you plug a HMI light into a wall outlet you need not be concerned about current harmonic distortion producing voltage distortion. The impedance of the power source is so low, the distortion of the original applied power waveform so small (less than 3%), and the power plant generating capacity so large by comparison to the load, that harmonic currents fed back to it will not effect the voltage at the load bus.
To say that harmonic currents are not a practical problem on large film sets is more of a testament to the industry and the means it has developed to remediate the problem than to say that
harmonics do not exist. Voltage waveform distortion is for the most part not a problem on large film sets because of remedial steps taken in the design of form specific generating and power distribution systems engineered to remediate the adverse effects of harmonic currents. With 2/3 pitch windings, MQ Power studio (Crawford) generators are specifically designed to remediate the most troublesome of the harmonics generated by non-linear loads and as such have specifications for total harmonic distortion (THD) values of less than 7% under full linear load, and of not more than 3% of any given harmonic current. For this reason, and the fact that they offer a comparatively low sub-transient impedance value and are typically oversized for the load, harmonic currents do not cause substantial voltage waveform distortion.
Percentage of Load
However, it is an all together different situation when plugging a couple of 1200W HMIs into a small portable generator that is not specifically designed to remediate the effects of harmonics. Given the comparatively large sub-transient impedance of conventional AVR portable gas generators, and the high THD value of their inherent power waveform (see no load waveforms below), you have a situation where even a small amount of harmonics being fed back into the power stream will result in a large amount of harmonic distortion in its’ voltage. Making the matter worse is that, given the increasing prevalence of non-linear light sources in production, it is likely that the percentage of the generator’s capacity taken up by non-linear loads will be very high given its small size relative to the size of HMIs typically used on these generators (575-2500 Watts.) Small portable conventional AVR generators present a perfect (electrical) storm
where the return of any harmonic currents results in a very high degree of voltage distortion.

Left: Original Grid Waveform w/no load & low THD (>3%) Right: Original conventional AVR Generator (Honda EX5500) waveform w/ no-load & high THD (@17%)
The means by which the industry has more or less successfully dealt with harmonics - namely the over-sizing of generators, the over-sizing of neutrals, the incorporation of power factor
correction circuitry in large HMI ballasts, and finally the use of generators with 2/3 pitch windings – are generally not available to users of small portable generators as their primary
source of power. It is generally not an option for small independent productions using portable gas generators by necessity to upscale to larger generators; and, given that there is not much that the end user can do to alter the power output panel of a portable gas generator, it is not an option to customize their distribution package for the requirements of higher neutral currents resulting from non-linear loads. All that users of small portable generators can do to remediate the adverse effects of harmonic currents is downsize their lighting package when it consists predominantly of non-linear light sources.

Left: Pkg. of 2-1200 HMI Par w/ non-pfc ballasts & Kino Wall-o-Lite powered by grid power. Right: Same Lighting Pkg. powered by conventional AVR Generator (Honda EX5500) Note different effect that the same non-linear load harmonics have on grid power and power from conventional AVR generator.
What we see above is the voltage distortion at the power bus of our distribution system created by the harmonic currents, or "noise", being thrown back into the system by a typical non-linear lighting package. An artifact of this noise, that is evident here and worth noting, is the zigzag saw tooth pattern as voltage ascends from zero potential and descends to zero potential. This zigzag saw tooth pattern is an indication of the existence of high frequency “wavelettes” within the primary sine wave. When interpreting the highly distorted voltage waveform above, it is worth remembering that the square wave depicted on our scope is in fact comprised of many, many voltage spikes, at extremely high frequencies, stacking one on top of the other.

Harmonics making up a Square Wave.
That is, if we were to break out the components contributing to the generation of the square-wave we see on our scope it would be comprised of more than just the three orders of current harmonics depicted in the example above. We would find that it is generated by many many high frequency harmonic currents, each inducing a voltage spike of its' own. Each of these voltage spikes is induced by high frequency harmonic currents being thrown back into the power stream by the electronic ballasts of our non-linear lighting package. The accumulative effect of all these induced spikes in voltage stacking one on top of the other is the square wave with zigzag pattern as voltage ascends and descends from the zero crossover point that we see in the oscilloscope shot above.

Sprectrum analysis of the high frequency Harmonic Currents that create a Square Wave
It is important to realize that the oscilloscope shot above is of the voltage waveform at the distribution bus of the generator "upstream" of the load (a 1200W non-PFC Electronic HMI ballast in this case) and that the oscilloscope probe is reading between hot and ground. While, as we will see below, harmonic currents stack on the neutral return of a distribution system, what we are looking at here is the effect of harmonics currents that are also feeding back up through the distribution system all the way to the generator's Stator and Rotor windings. What this means is that any piece of equipment plugged into this distribution system sees only this distorted waveform as its' power supply.
This harmonic distortion of the voltage waveform exists only in the case of the portable generator power, where it would not in the case of grid power, because of the inherent distortion in the applied voltage and the
relatively high impedance of the generator and distribution system compared to power from the utility grid. To put it in the most simplistic terms, if I had to explain this electrical phenomenon to my 5 year old,
I would say that Ms. Sinusoidal Voltage met Mr. Harmonic Current over Impedance, and had a baby they named Pseudo Sine Wave. While this description is overly simplistic, it drives home the point that this Pseudo Sine Wave is a completely new entity
created from the other two, and is all that equipment on the distribution system will see.
Other Adverse Effects of Harmonics
Without a doubt, as the trend toward HD production continues, the increasing use of personal computers and microprocessor-controlled recording has created an
unprecedented demand for clean, reliable power on set. At the same time a parallel move toward HMI and Florescent lighting instruments is dumping more and
more harmonics back into the power stream. Where, as we have seen, these loads can have undesirable effects on the current wave form of generated power,
an awareness of these effects will help us to build production systems that avoid or mitigate problems, as well as show us how to solve problems should they arise.
Here is a quick summary of other adverse effects that can result from excessive harmonic distortion.
Adverse Effects to the Generator & Distro
Overheating
Harmonic currents produce high frequency flux change in the generator’s Stator core which can lead to them overheating. Higher core temperatures result in higher winding
temperatures. Winding heating is, in fact, proportional to effective or RMS current squared. Rotor loss can also occur because harmonic currents in the Stator will induce
currents in the Rotor pole faces and windings. Of course, harmonic currents cause increased resistive losses everywhere, resulting in increased temperatures everywhere,
not only in the windings.
Erractic Voltage Fluctuation
As discussed previously, the Automatic Voltage Regulator (AVR) of conventional portable generators maintain the terminal voltage of the generator at a constant value by sensing the output voltage, comparing it with a set value, and correcting any error by suitably changing the field excitation current. Given how it works, the sensing part of an AVR system is the most important part from an operational standpoint.
How the AVR system senses the generated voltage varies from one generator design to another. Regardless of how the voltage is sensed, a considerable amount of harmonic distortion in the terminal voltage will result in the voltage getting regulated at a wrong level unless the AVR system is specifically designed for non-linear loads. Modern designs on large gen sets that are specifically engineered for non-linear loads use filtering in the voltage sensors, sense on all the power phases, and use true rms calculation (either using analog electronics or by using digital techniques in micro processors) to avoid voltage regulation problems when serving non-linear loads. Needless to say, conventional portable gas generators do not use AVR systems of this level of sophistication, and so distortion of the terminal voltage as a result of harmonic distortion results in the voltage getting regulated at a wrong level. Because an AVR system is a closed-loop control system, as the voltage is incorrectly changed, based on the distorted information, it is then even more incorrect and the output voltage finally gets so far off that the generator ceases to produce an output that is usable.
Erractic Speed Fluctuation
Another problem that can result from high THD values is the malfunctioning of the generator’s AC frequency governor. As discussed previously, the engine governor system needs a speed feedback signal. In the case of after market engine governors designed for portable gas generators, this signal is generated by measuring the frequency of the sensed output voltage inside the AVR unit.

Voltage notching can create multiple zero crossings
Where this frequency calculation involves zero-crossing information from the waveform, high THD values can cause problems. For example, voltage notching and heavy ringing transients like the ones present in our
distorted waveform (above) create multiple zero-crossings within one cycle of AC waveform. This leads to large magnitude random errors in the frequency signal prepared by the AVR unit for use by the governor unit.
The governor unit gets confused and there results instability of the speed governing system.
In our discussion above, we covered a number of the adverse effects that harmonic noise can have on the generator itself. To review they include over heating, voltage regulation and speed regulation problems. Kevan Shaw’s
You-Tube video “Compact Fluorescent verses The Generator" (discussed previously) clearly demonstrates these effects. It is informative not only for the
point he sets out to make, but also for the point he makes unintentionally. If you will recall, in his video (below), lighting designer Kevan Shaw set out to demonstrate that CFL bulbs have a poor power factor (.5) and
consume double the energy (Apparent Power) for the 18 Watts of light (True Power) they generate. However, his video also clearly demonstrates the severe effect that leading power factor loads can have on the governing
systems of conventional AVR generators.

When Kevan turns off the 18W CFL bulbs one at a time until the generator stabilizes, he is not only demonstrating that 15 – 18W CFL bulbs has roughly the same Apparent Power
(535W), according to the generator’s Watt meter, as a 575W incandescent light; but, also that the maximum Leading Power Factor load a 850W conventional generator can operate
satisfactorily is 270 Watts (15 – 18WCFL bulbs). Looked at another way, 576 Watts of Apparent Power with a Leading Power Factor (16 - 18W CFL bulbs) overloaded the generator,
while 575 Watts of Apparent Power with a Unity Power Factor (the 575W Quartz Leko) did not. What accounts for this difference? Since the load is almost the same (576 & 575
Watts of Apparent Power respectively), the only factor that can account for the generator going berserk with the equivalent load of CFL lights is the harmonic currents that
they generate that the Quartz Leko does not. Without a doubt, Kevan Shaw’s video is a clear demonstration of the adverse effect that harmonic currents have on the
governing systems of conventional AVR generators.
For the same reason that Kevan Shaw was not able to operate more than 270 Watts of CFL bulbs (15 – 18W bulbs), it has never been possible to reliably operate more
than a couple of 1200W HMIs with non-PFC electronic ballasts on 6500W conventional AVR generators. The adverse effects of the harmonic currents they generate, so
graphically demonstrated in Kevan’s video, limits the total amount of Leading Power Factor loads, as compared to Unity Power Factor loads, that can be reliably operated
on conventional AVR generators. So much so that, manufacturers take the type of load that a generator will likely operate into account in determining the continuous
load rating of a generator for a specific market (more on this subject latter.)
High Neutral Returns
With incandescent lights, if we draw equal current from each leg of our single phase portable generator, there will be no return current on the neutral.
That is because the current on the legs is 180 degrees out of phase, and so the current cancels out when combined on the neutral return. When an inductive
or capacitive load causes current and voltage to be out of sync, the phase currents no longer cancel when they return on the neutral. When using magnetic
ballasts, it is normal to have as much as 20-25% of the total amperage return on the neutral when the legs are evenly loaded.
Electronic square wave ballasts, in addition to pulling the voltage and current out of phase, also create harmonic currents that can stack on top of one
another, creating very high currents returning to the power source on the neutral wire. If the nuetral return path has not been oversized to accomodate additinal
current, these high currents can cause excessive heat on the neutral wire, and the neutral bus of the generator. Where the neutral of a distribution system is not fused,
this excessive heat can lead to a possibly hazardous situation. Where high currents
on the neutral can be hazardous, it is important to understand the root cause of these currents so that we can design a location lighting package that
eliminates, or at the very least mitigates, these factors.
The harmonic currents produced by electronic HMI ballasts are primarily generated by the diode-capacitor section of the ballast. As you may recall from our
discussion above, the diode-capacitor section rectifies the AC input power into DC, which is then used by the power module to create the square wave. The
diode-capacitor section accomplishes this by first feeding the AC input current through a full wave bridge rectifier, which inverts the negative half of
the AC sine wave and makes it positive. The rectified current then passes into a bank of capacitors which removes the 60 Hz rise and fall and flattens out
the voltage-making it essentially DC. The required DC is then fed from these capacitors to the power module. Since the rectifying circuit of the power supply
only draws current from the AC line during the peaks of the supply voltage waveform, charging the capacitors to the peak of the line voltage, these power
supplies draw current in high amplitude short pulses and pull current out of phase of the voltage. The remaining unused current feeds back into the power stream as harmonic currents.

The Triplen Harmonics Stack to create excessive current on the Nuetral of a distro system
Of the harmonic currents that electronic ballasts generate, the odd harmonics (i.e. 3rd, 5th, 7th, 9th, etc.) are more of a concern because the even harmonics have
a tendency to still cancel out. Of these the 3rd harmonic, and odd multiples of the 3rd (9th, 15th, etc) are particularly troublesome. These harmonics are called the “triplens.”
What makes them troublesome is that the triplen harmonics dumped back onto each phase of the distribution system are all in phase with each other. For this reason, rather
than cancel each other out on the neutral conductor, as the out of phase fundamentals normally do, they instead add up. By generating harmonic currents that stack one upon another,
and shifting the phase of the primary currents so that they don't entirely cancel, electronic square wave ballasts can create
unusually high returns on the neutral of the distribution system. If the lighting package consists entirely of non-linear
light sources without power factor correction, about 80 percent of the current does not cancel out between legs, resulting in very high current on the neutral return.
Return currents of this magnitude can cause sufficient heat to overload the neutral wire, and the neutral bus of the generator, leading
to a possibly hazardous situation since the neutral return has no fused protection.
For this reason it is a standard practice when powering large numbers of electronic ballasts on large film sets to size the neutral feeder of the distribution system to carry the sum of the currents of the phase legs times 80 percent (.8). Likewise, the generator is typically oversized to handle the higher return current. However, productions using conventional portable gas generators by necessity, for whom it is not an option to upscale their generator and customize their distribution package for the requirements of a non-linear load, the only alternative is to de-rate the generator and distribution equipment.
Given that there is not much that the end user can do to alter the power output panel of a portable gas generator, all they can do is downsize their lighting package when it consists predominantly of non-linear light sources. The general rule of thumb is to maintain a factor of 3 or 2 to 1 between the continuous rated load capacity of the generator and the total lighting load when it consists of predominantly non-linear light sources. This translates to operating no more than a couple of 1200W HMIs on a 6500W generator if the ballasts are not power factor corrected.
Adverse Effects on Loads
Thus far we have examined the adverse effects on the generator of loads that generate harmonic currents. Now, let us consider the effect that power with a high THD value has upon
the distribution system and the loads operating upon it.
Increased Resistance
As we saw above, harmonic frequencies are always higher than the 60Hz fundamental frequency. Where THD is high, the higher frequencies create what is known as
“skin effect.” Skin effect is a phenomenon where the higher frequency causes the electrons to flow toward the outer sides of a conductor. Since the flow of the
electrons is no longer evenly distributed across the cross sectional diameter of the conductor, more electrons are flowing through less copper and the resistance
of the conductor increases. The increase in resistance reduces the ability of the conductor to carry current, resulting in greater voltage drop over shorter distances
and overheating of the conductor. The greater voltage drop as a result of “skin effect” has several adverse effects.
Skin Effect

The area of the cross sectional diameter of a conductor used by DC current (left), Low Frequency AC Current (center), High Frequency AC Currents (right).
One adverse effect is that it causes equipment connected to the circuit to draw more current to maintain the power rating (watts) of the unit. This, in turn,
can cause protective fuses on electrical boards of equipment to blow - even those of the square wave electronic ballast itself. I experienced this
first hand, when I first tried to operate a 4k HMI Par on a Honda ES6500 (a conventional AVR generator) with the first generation of electronic square wave
ballasts - a Lightmaker. The ballast inexplicably failed when it had never given us problems on mains power. Upon closer inspection back in our shop, we
found that a protective fuse on the main board had failed. We replaced the fuse and continued to operate the ballast off of grid power without incident. But
as soon as we tried to run it again on the Honda the fuse blew. In hindsight, what accounts for the ballast’s erratic behavior was the amount of harmonic
distortion it was feeding back into the power stream. The harmonic currents were not a problem on grid power because they did not induce voltage distortion for the reasons discussed above. But, fed back into the power
stream generated by our Honda ES6500, the same harmonic currents created voltage distortion and sufficient voltage drop from skin effect to blow protective fuses on the ballast's boards.
Originally designed to operate large HMIs on DC generators, the first AC/DC Lightmaker ballasts did not incorporate Power Factor Correction or Harmonic Filters. For this reason, when operated on AC power, they fed so much harmonic distortion back into
the power stream that they were nicknamed Troublemaker ballasts by many set electricians. We discovered the hard way, a design that worked well on DC sources, was not compatiable with small portable AC genrators like
the Hondas for which they were not intended.
Building upon Lightmaker's basic design, manufacturers such as Power Gems, Walker, and Bausch (the manufacturers of Arri's ballasts) incorporated filters to reduce the number of
harmonic currents the ballast feeds back into the power stream. Such improvements led to a second generation of electronic ballasts that operated more reliably on AC
power sources. To reduce the number of harmonic currents generated in the first place, the latest generation of electronic ballasts incorporate Power Factor Correction circuitry (PFC), as well as active line filtration (ALF.) However, since Power
Factor correction is not commonly found in HMI ballasts smaller than 4000W, voltage drop from “skin effect” can still create problems when operating HMI lights on conventional portable generators.
Whenever a piece of electrical equipment inexplicably fails while operating well below its design ratings, and it was operating on the same distribution system as HMIs without power factor correction, it is a safe bet that you will find blown fuses.
Another common problem associated with skin effect is the apparently inexplicable tripping of breakers. Since it is not uncommon to use portable gas
generators to power 1200W HMIs with non power factor corrected electronic square wave ballasts, even a slight increase in load resulting from the voltage
drop caused by skin effect can cause what appear to be the inexplicable tripping of circuit breakers in the distribution system or
on the generator. If you recall, a 1200W non-power factor corrected HMI ballast can draw upwards of 19 Amps under normal circumstances (grid power), it doesn’t
take much increase of circuit resistance to push its load over the 20A threshold of distribution circuit breakers. Especially, given that 1200W ballasts are commonly
wired with u-ground Edison plugs rated for 15 Amps, resulting in overheating of the plug end, and an increase of resistance even under normal conditions.
RF (Radio Frequency) Interference
If you will recall, the distorted square wave depicted on our scope is in fact comprised of many voltage spikes, at extremely high frequencies, stacking one on top
of the other. That is, if we were to draw out the time base of our scope we would see the square portion of the wave break out into many more voltage "wavelettes" of
a higher amplitude than what we already see in the zig-zag portion of the wave. Each of these high frequency voltage spikes are the result of discreet harmonic currents
being thrown back into the power stream by non-linear lighting loads.

Sprectrum analysis of the high frequency Harmonic Currents making up a Square Wave that can cause RF Interference
The power stream can become so full of high frequency harmonic currents, that it creates RF
(Radio Frequency) interference. Sensitive electronic devices that are not even hooked up to the distribution system, but simply in close proximity to it, may pick up
the RF (Radio Frequency) interference and begin to show its artifacts, or worse not function at all. Examples of RF interference include lines or fuzzy picture in set
monitors, a buzz in audio tracks, and poor reception in radio mics.
Ground Loops
It is also worth noting that “ground loops” can result from the harmonic currents that non-pfc electronic ballasts throw back into the distribution system. Current on
neutral conductors with a high THD value will induce voltage in ground wires greater than the 2 volt maximum stipulated by IEEE Standard 1100-1992 "Recommended Practice
for Powering and Grounding Sensitive Electronic Equipment." For instance, there was an episode, recently reported on CML, of a pilot shooting in HD that found they had 50
volts between the shield of the SDI line and ground. In that case the problem was fixed by running a "Drain" wire from the SDI Shield back to the Genny via the electrical
lunchbox at the DIT station. Clearly, if not corrected high neutral-to-ground voltages will cause current to flow on the ground wires and lead to the creation of ground
loops between the tethered components of a HD production package.
A ground loop occurs when there is more than one ground connection path between two pieces of equipment. The duplicate ground paths form the
equivalent of a loop antenna that very efficiently picks up interference currents. Lead resistance transforms these currents into voltage fluctuations. As a consequence of
ground loop induced voltages, the ground reference in the system is no longer a stable potential (a floating ground), so signals ride on the noise. The noise becomes part
of the program signal. The result is that the unwanted signal will be amplified until it is audible and clearly undesirable. Whenever you have current induced on the
grounding system as well as the multiple connections between electronic components that is typical of HD production packages, there is the potential for a "ground loop."
PHOTO COURTESY OF THOMI ENGDAHL

Interference bars caused by induced voltage on ground loop.
Small voltage differences just cause noise to be added to the signals. This can cause an audio hum, interference bars to video signals (above), and transmission errors
in computer networks. Higher currents can cause more serious problems that can damage equipment like sparking in connections and burned wiring. As more and more electronic
components, like lap top computers, hard drives, and HD monitors, are integrated into the typical location HD production package, ground loops become more of a hazard.
Overheating and Component Level Failure
The excess part of a distorted voltage waveform (the shaded area in the diagram below) must be dissipated somehow. This comes in the form of heat. The bigger the
current draw from the unit, the more it produces excess heat within the unit that was not factored for in its’ original design.

Unuseable portion of distorted waveform (shaded) dissipated in heat.
Extended exposure to power with harmonic distortion, and the heat it generates, may eventually cause premature component level failures within the unit. Imagine having to replace a new flat screen
HD monitor after only a couple of years.
"Inexplicable" Operational Malfunctions
Where there is appreciable voltage waveform distortion created by operating non-linear light sources on a conventional generator, other electrical devices operating on
the same power are unable to use the distorted waveform effectively.

Left: Waveform of grid power. Right: Waveform of conventional AVR Generator (Honda EX5500) operating non-linear lighting pkg. consisting of two Arri 1.2kw non-PFC ballasts and a Kino Flo Wall-o-Lite.
For instance, other production equipment that utilizes diode-capacitors and therefore depend on the peak value of the voltage waveform to operate effectively will work sporadically, if at all, on the squared off wave-form caused
by harmonic currents (above). Like the battery charger operating on a Modified Square Wave Inverter (discussed previously), the Switch Mode Power Supplies (SMPSs) of computers, hard drives, and electronic HMI and Kino ballasts
operating on the pseudo square wave of distorted voltage will be starved of power even though you may read full line voltage with an RMS meter and the power indicator lights light.
Kevan Shaw’s You-Tube video “Compact Fluorescent verses The Generator" clearly demonstrates this effect.
As discussed previously, Kevan Shaw's video (below) demonstrates that, because of their poor power facgtor, CFL bulbs consume twice the power as the same size incandescent load and generate harmonic
currents that adversely effect the governing systems of conventional AVR generators. A closer analysis of the video also shows that the voltage waveform distortion created by the harmonic currents will also adversely affect electronic
equipment operating on it.

If you will recall, after Kevan has turned off 18W CFL bulbs until the generator has stabilized, he is still "not getting all the lamps to illuminate properly." What accounts for the bulbs not illuminting properly even
though the generator has stablized? While the Harmonic Distortion generated by the remaining CFLs is not sufficient to affect the generator governor, it is clearly affecting the CFLs themselves - an indication that,
short of affecting the generator's governing system, the voltage waveform distortion generated by harmonic currents will adversely effect electronic equipment operating on the distorted power.
Common symptoms are unexplainable operational
malfunctions like computers locking up, tripping breakers, and HMIs not striking or holding their strike. To explain these "inexplicable" operational malfunctions requires a close examination of the characteristic distortion
generated by our various lighting loads. For this reason let us put off that analysis until we look at the waveforms of different lighting loads in the section below titled "Interpreting the Sines."
A Viscious Cycle
As more and more electronic components, like lap top computers, hard drives, and HD monitors, which are themselves sources of harmonic distortion (but of a lower amplitude
than solid state lighting ballasts) are integrated into the typical location production package, harmonic currents begin to combine with unpredictable consequences. In fact,
a viscous cycle can get started. The more harmonic orders that are generated, the more distorted the power supplied by the generator becomes. The more distorted the power
waveform becomes, the more harmonic currents are thrown back into the electrical distribution system, which in turn, creates additional voltage distortion. In this
fashion, something akin to a feedback loop can get started. Very often, the operation of electrical equipment may seem normal, but under a certain combination of conditions, the impact of harmonics is enhanced with unpredictable results.
To summarize, the possible effects that non-linear lighting loads can have on the current waveform reveal themselves in the form of overheating and failing equipment , efficiency losses, circuit breaker trips, excessive current on the neutral wire, interference and instability with generators, noisy or over heating transformers, and service equipment.
Power Factor Correction
The first step in designing a production system that mitigates the problems caused by harmonic currents is to largely eliminate the currents. Where customarily the largest source of harmonic currents in a typical lighting
package are HMI and fluorescent lights, using only ballasts with Power Factor Correction (PFC) circuitry will go a long way in reducing the number of harmonic currents in the power stream. By eliminating the generation
of harmonic currents, a PFC circuit realigns voltage and current and induces a smoother power waveform at the distribution bus. As a result, the ballast uses power more efficiently with minimized return current and
line noise and also reduces heat, thereby increasing their reliability. Where Power Factor Correction in HMI and fluorescent lights offer tremendous benefits in many production applications, but is seldom understood
accurately, let’s explore how it works in more detail.

The effect of Power Factor Correction on the Apparent Power of Arri Electronic Ballasts.
To start, here is a quick summary of what we know of power factor thus far. With a purely resistive “linear load” (Incandescent Lamps, Heaters, etc.) voltage and current waveforms
are in step (or in phase), changing polarity at the same instant in each cycle ( a high power factor or unity.) With “non-linear loads” (magnetic and electronic HMI, fluorescent, & AC LED ballasts) energy “storage” in the loads, impedes the flow of current and results in a time difference between the current and voltage waveforms – they are out of phase (a low power factor.) In other words, during each cycle of the AC voltage, extra energy, in addition to any energy consumed in the load, is temporarily stored in the load, and then returned to the power distribution a fraction of a second later in the cycle. The "ebb and flow" of this nonproductive power increases the current in the line. Thus, a load with a low power factor will use higher currents to transfer a given quantity of real power than a load with a high power factor. The purpose of PFC circuitry is to bring the voltage and current waveforms back in phase (closer to unity power factor.) How this is accomplished depends on whether poor factor is caused by inductive reactance or capacitive reactance. Let us look first at how poor power factor as a result of inductive reactance is corrected in HMI magnetic ballasts.
To understand how Power Factor Correction in magnetic ballasts is accomplished, let’s review what we learned about the operation of magnetic HMI ballasts above. Between the power input and the HMI lamp is a transformer that acts as a choke coil. The transformer provides the start-up charge for the igniter circuit, rapidly increasing the potential between the electrodes of the head’s arc gap until an electrical arc jumps the gap and ignites an electrical arc between the lamp electrodes. The transformer then acts as a choke, regulating current to the lamp to maintain the pulsating arc once the light is burning.

Left: Transformers of a 12k Magnetic HMI Balllast
As you can see in the picture above, the transformers of magnetic HMI ballasts are essentially large coils of wire that are tapped at several places to provide for various input voltages and a high start-up voltage. As such, the transformers of magnetic HMI ballasts exhibit high self-inductance. As we learned above, self-inductance is a particular form of electromagnetic induction characteristic of coils (like those in magnetic HMI ballasts and electric motors) that inhibits the flow of current in the windings of the coil. This opposition to the flow of current is called inductive reactance. In the case of a magnetic HMI ballast, the multiple fine windings of the ballast transformer induces appreciable voltage and considerable current that is in opposition to the primary current, causing the primary current to lag behind voltage, a reduction of current flow, and an inefficiency in the use of power supplied to it. Put simply, the ballast draws more power than it uses to create light.

The Capacitor Bank of a 12k Magnetic Ballast
A common strategy used to correct the self-inductance of transformers in magnetic ballasts (both fluorescent and HMI) is to supply reactive power of the opposite type – i.e. adding capacitors to cancel the high inductance of the transformer’s windings. Power-factor correction capacitors will draw a current with a leading phase angle to offset the lagging current drawn by the ballast transformers. For this reason a bank of capacitor is typically included in the design of magnetic HMI ballasts to bring the current partially back in phase with the voltage. In this sense all magnetic ballasts are power factor corrected.

Since, capacitive reactance distorts the shape of the voltage waveform from a sine wave to some other form (example above), the addition of linear components such as inductors cannot counteract the capacitive reactance of electronic ballasts as the addition of capacitors counteracted the inductive reactance of magnetic HMI ballasts. In the case of electronic ballasts, other more complicated (translate expensive) means of Power Factor Correction is required to smooth out the power waveform.

To understand how Power Factor Correction works in electronic ballasts (HMI, fluorescent, & AC LED) it would help to review what we know about the source of the harmonic currents
that create the high level of capacitive reactance in these ballasts. The harmonic currents produced by electronic ballasts are generated by its’ diode-capacitor section.
As you may recall from our discussion above, the diode-capacitor section rectifies the AC input by first feeding it through a bridge rectifier, which inverts
the negative half of the AC sine wave and makes it positive. The rectified current then passes into one or more conditioning capacitors that remove the 60 Hz rise and fall
and flattens out the voltage - making it essentially DC. The DC is then fed from these capacitors to some type of Switch-mode Converter, that in the case of fluorescent and HMI ballasts, switches it into an
alternating power waveform that excites gases in the lamp. In the case of High Power LEDs, the Switch-mode Converter further conditions the DC power fed to the diode.

Thin Black Trace: Rectifier Bridge converts AC power to rectified sine wave. Thick Black Trace: Stored Capacitor Voltage. Red Trace: Current drawn by capacitors once input voltage is greater than voltage stored in the capacitor (thick black trace.)
Regardless of the type of type of Switch-mode Converter used in the ballast, its’ rectifying circuit only draws current from the AC line during the peaks of the supply voltage waveform. As can be seen in the illustration below, electronic ballasts draw current in high amplitude short pulses. The remaining unused current feeds back into the power stream as harmonic currents.

Voltage and
Current Waveforms generated by Fluorescent ballasts without power factor correction (left)
and with power factor correction (right)
In order to not draw current in high amplitude pulses, and consequently not return unused portions of the power waveform as harmonic currents, the conditioning capacitor(s) must
charge over the entire cycle rather than just a small portion of it. The PFC circuitry of electronic ballasts ( HMI, fluorescent, & AC LED) use some type of multi-stage boost converter typology
to accumulate energy in the capacitor(s) over the entire AC cycle rather than just a brief portion of it.

Voltage and
Current Waveforms generated by High Power AC LED ballasts without power factor correction (left)
and with power factor correction (right)
Now that the capacitor(s) charge throughout the AC cycle rather than just a brief portion of it, the peak current is reduced and harmonic currents are not generated. And, if the
output voltage of the boost converter is set higher than the capacitor(s) input voltage (which is why they are called boost converters), the load is forced to draw current in
phase with the AC main line voltage. In this fashion, the PFC circuit realigns voltage and current and induces a smoother power waveform at the distribution bus. As can be
seen in the comparisons above of the current and voltage waveforms of fluorescent and High Power AC LED ballasts without power factor correction (left)
and with power factor correction (right), PFC circuits can substantially increase power factor (to as much as .98), making ballasts with it near linear loads. As a result, the ballast uses power more efficiently with minimized return current and line noise and also reduces heat, thereby increasing their reliability.

Left: AVR Gen. No-load Waveform. Center: AVR Gen. 1.2KW non-PFC Elec. Ballast Waveform. Right: AVR Gen. 1.2KW PFC Elec. Ballast Waveform.
As the voltage waveform comparisons above demonstrates, a PFC electronic HMI ballast (right) has very little adverse effect on the power waveform of a conventional generator as compared to a non-PFC electronic ballast (center.) If anything it has a positive effect.
For this reason, all major manufacturers include PFC circuitry in large HMIs (12-18kw), and offer PFC circuitry as an option on medium-sized ballasts (2.5-6kw). However, because of the added cost, weight, and complexity of
PFC circuitry, manufacturers have not until recently offered PFC circuitry in HMI ballasts smaller than 2.5kw. Except for one notable exception, when manufacturers do offer PFC circuitry in smaller ballasts it is at a
premium, adding as much as a $1000 to the cost of a 1200W ballast for instance. Ballast manufacturer Power-to-Light, on the other hand, is including PFC circuitry in their ballasts at the same price point as other manufacturer’s non-PFC ballasts.

Power to Light PFC 800W ballast (left) and PFC 1200W ballast (right.)
A typical 1200W power factor corrected electronic HMI ballast has a power factor of .86 which means it will draw 11.5 Amps at 120 Volts to generate 1200 Watts of light (11.5A x 120V= 1380W, 1200W/1380W= .86). While not a huge advantage when plugging into house power, the added efficiency of a PFC 1200 ballast can make a huge difference when powering a lighting package off of a portable generator. For example, when you consider that a Kino Flo Parabeam 400 draws only 2 amps, the 8 Amp difference between using a PFC 1200W electronic ballast and standard non-PFC 1200W electronic ballast, can mean the difference between running four additional Parabeam 400s on a portable generator or not – I think you would have to agree that is a major boost in production capability.
Clearly, the first step in designing a production system that mitigates the problems caused by harmonic currents is to use only Power Factor Corrected ballasts. The next step, as we will see next, is to start with as pure a power waveform as possible.
A Whole New World
Common questions I hear are: Why are harmonics suddenly an issue in motion picture electrical distribution systems? And, why haven’t we needed Power Factor Correction in HMIs until now? To answer these questions, one must appreciate the historical interplay between power generation and load in the past. The lagging power factor (current lags behind voltage) caused by the inductive reactance of magnetic ballasts had a considerably less adverse effect on conventional AVR generators than the leading power factor (current leads voltage) caused by the capacitive reactance of electronic ballasts. That was because Power Factor Correction in the form of capacitor banks brought voltage and current in phase enough that magnetic ballasts operated reliably for the most part; while the type of voltage waveform distortion they generated did not have an adverse effect on the relatively simple linear loads making up production packages of the day (principally the motor drives of film cameras and quartz lighting instruments.)
However, we are no longer in our parent’s linear world. The power generation and electrical distribution systems developed then were not designed to deal with the abundance of non-linear loads like electronic HMI and Kino
Flo ballasts that make up lighting packages today. It’s a problem that has only recently begun because of the increasing use of non-linear lighting loads (for a comprehensive overview see the just released 4th Edition of Harry Box's "Set Lighting Technicians Handbook" - send me a self addressed stamped envelope & I will return it with a discount coupon good for 30% off the 4th Edition through the publisher's website.) The problem is being further compounded by the increasing prevalence
on set of sophisticated electronic production equipment like HD cameras, computers, hard drives, and monitors which are not only sensitive to harmonic distortion, but are themselves sources of harmonic distortion.
For instance, the self-excited AVR systems of conventional generators were not designed to operate with leading power factor loads. If you will recall from our
previous discussion, in AVR systems the AC voltage generated is controlled by DC excitation of the electro-magnets of the generator's Rotor. The amount of DC
excitation required is a function of generator load; or, put another way, the excitation required to maintain constant voltage increases with load. The type
of load also affects the amount of excitation required. Lagging power factor loads (magnetic ballasts) require more excitation than a unity power factor load
(Quartz Lights.) Leading power factor loads (electronic ballasts) require less excitation than unity power factor loads.
Rudimentary AVR systems like those in portable generators are ill equipped to deal with leading power factor loads like electronic ballasts because the harmonic currents
they generate create flux in the armature coils of the Stator that reacts
additively with the Exciter flux in the field poles of the Rotor to increase saturation and produce a higher terminal voltage than called for a given load. Consequently, the AVR system
responds erroneously to control voltage by reducing excitation. The end result is that the regulator goes to its minimum excitation capability while the additive
excitation of the armature flux from the leading power factor causes the terminal voltage to continue to rise and not be controlled by the voltage regulator.
Erroneous regulation of voltage is just one example of the more severe effect that leading power factor loads have on conventional AVR generators than do lagging power factor loads. In the next section, where we compare the characteristic voltage waveform distortion created by different lighting loads on different generators, we will see that leading power factor loads also have a more severe effect on other production equipment operating on the same power. And, that
after partial Power Factor Correction with capacitors, the lagging power factor of magnetic ballasts can actually have a positive effect on the already distorted power waveform of conventional AVR generators like the Honda EX5500. For these reasons, as long as you could shoot at one of the safe “flicker free” frame rates, magnetic ballasts worked reasonably well on conventional AVR generators with frequency governors until the introduction of electronic square wave HMI ballasts.
When electronic square wave HMI ballasts came on the market, they were at first thought to be the solution to all the problems inherent in running HMI lights on small portable generators. Since they are not frequency dependent, it was thought at first that electronic square wave ballasts would operate HMIs more reliably on small portable generators – even those without frequency governors. By eliminating the flicker problem associated with magnetic ballasts, they also eliminated the need for the expensive AC governors required for flicker free filming with magnetic HMI ballasts and portable gas generators.
For these reasons, as soon as electronic square wave ballasts appeared on the market, many lighting rental houses replaced the expensive crystal governed Honda EX5500 with the less expensive non-synchronous Honda ES6500. The theory was that an electronic square wave ballast would operate reliably on a non governed generator and allow filming at any frame rate, where as a magnetic HMI ballast operating on an AC governed generator allowed filming only at permitted frame rates. In practice, electronic square wave ballasts turned out to be a mixed blessing. As we have seen in this section, the leading power factor caused by the capacitive reactance of the new electronic ballasts proved to have a more severe effect on conventional AVR generators than did the old magnetic ballasts.
Since magnetic ballasts worked reasonably well on AVR generators with governors, in the past, attention was only given to portable generator features such as automatic voltage regulation, speed regulation and AC Frequency. But, given the increasing prevalence of leading power factor loads and the problems they cause, an increasingly more important feature today is the quality of the generated waveform and the impedance of the power system. For this reason, it is imperative that today’s power generation and electrical distribution systems be designed for non-linear lighting loads, not just linear lighting loads. This is especially true of the systems to be used in low budget independent production because these productions have traditionally relied upon portable gas generators that are more susceptible to the adverse effects of harmonic distortion. These productions are also increasingly embracing the use of HD digital cinema production tools, like inexpensive HD camcorders, laptop computers and hard drives, that require cleaner and more reliable power on set to operate effectively.
__________________________________________________________________
Interpreting the Sines
As we learned above, the magnitude of the current and voltage waveform distortion depends upon the quality of the original applied power waveform and the relative size
of the nonlinear loads with respect to the source impedance and capacity of the power generating system. That is, the amount of voltage distortion increases as distortion
of the applied waveform increases and the percentage of nonlinear loads taking up the total capacity of the power generating system increases. For this reason, when
designing a better production system, it is worth looking at the specific magnitude and order of the harmonics generated by each type of lighting load on each type of power supply (Grid, Conventional AVR Generators, Inverter
Generators.) A thorough understanding of the interaction between these elements will enable us to design a produciton system capable of providing cleaner and more stable
power. To that end, I ran a series of tests in order to analyze the interaction of conventional AVR generators with AC
Frequency Governors (a Honda EX5500 with Governor), as well as inverter generators (a Honda EU6500is), with the prevalent linear and non-linear light sources.
The Test Set Up

Left: Honda EU6500is (L) Honda EX5500 (R) Center: Test Set-Up w/60A Full Power Transformer. Right: P@L PFC 1200W Elec. Ballast (L), Arri Non-PFC 1200W Elec. Ballast (C), Arri 1200W Magnetic Ballast (R)
The test consisted of running different loads (quartz, kino, mag HMI, non-PFC HMI, PFC HMI) on each generator and grid power as a sort of control. I then took
pictures of the resulting waveform on an oscilloscope. I have attached the side by side comparisons for each load type. The frame on the far
left is always grid power (our control), the center frame is always the EX5500 power, the right frame is always the EU6500is power as measured at the power bus.
They appear in the following order: no-load, 2k Open Face Quartz Light, Arri 1200 Par Plus with Magnetic Ballast, the same Arri 1200 Par Plus with a non-PFC electronic
ballast, the same Arri 1200 Par Plus but with a Power-to-Light 1200 PFC ballast, and finally a Kino Flo 4'-10 tube Wall-o-Lite fixture.
Voltage Waveforms
No Load Waveforms

Left: Grid Power w/ no load. Center: Conventional AVR Power w/ no load. Right: Inverter Power w/ no load.
As one would expect the wave form of the grid power is a nice sinusoidal waveform and has a Total Harmonic Distortion (THD) in this case of less than 3%. The waveform of the EX5500 exhibits the less sinusoidal waveform, with a THD of 17%, that is typical of conventional AVR generators. The waveform of the power generated by the EU6500is is, as Honda claims, a true sinusoidal waveform with a THD of 2.5%. The power generated by the EU6500is is in fact cleaner than the grid power coming out of our wall outlet.
Incandescent Lights (Resistive Linear Loads)

Left: Grid Power w/ 2K Open. Center: Conventional AVR Power w/ 2K Open. Right: Inverter Power w/ 2K Open.
As a purely resistive load our Mole 2k Mighty open face has very little adverse effect on the respective waveforms. If anything it has a positive effect on the Honda EX5500.
The result confirms what every electrician knows first hand from operating these machines. Namely, that they run smoother under load and that fact is reflected in the
smoother power waveform under load than without a load.
Unfortunately, incandescent lights are the least efficient light sources of the three that we are testing here. Since eighty percent of the energy consumed by an incandescent light goes into the generation of heat, they generate less lumens per watt of any other light source. Add to that, the fact that the Full CTB gel required to convert incandescent lights to daylight has a transmission factor around .3 (it takes a 1000 Watt incandescent source to generate 300 Watts of day light balanced light) make them the most impractical light source for daylight fill or the creation of cool moonlight.
As near a pure linear load as we will find, incandescent lights interact well with small portable generators. However, their inefficiency make them a poor choice when power is limited.
Magnetic HMI Ballasts (Inductive Non-linear Load)

Left: Grid Power w/ 1.2Kw Arri Magnetic Ballast. Center: Conventional AVR Power w/ 1.2Kw Arri Magnetic Ballast. Right: Inverter Power w/ 1.2Kw Arri Magnetic Ballast.
What we see within the inverter power waveform (right) is a spike in the voltage generated by current created by the self-inductance of the coils inside the ballast’s transformer. If you will recall from our discussion of magnetic ballasts above, an opposing current is induced in a current-carrying wire within a coil when the principle current changes as it alternates. Since the opposing current is induced after the voltage peaks and begins to descend again, the induced current lags the voltage and pulls the primary current out of phase with the voltage so that it lags behind the voltage. When it encounters an impedance, this opposing current induces voltage that appears as a spike in the oscilloscope waveform.
Harmonic currents of this magnitude can cause false circuit breaker tripping. For instance, when running multiple magnetic ballasts, these harmonic currents can stack and induce peak voltage values many times higher than the power waveform. Under such circumstances, peak sensing circuit breakers will trip even though their amperage value has not been exceeded.
Voltage spikes, as a result of stacking harmonic currents, goes a long way toward explaining this nightmare scenario: a number of years ago, I was gaffing a night shoot for American Experience with a 25KVA Mulitquip Silent Star generator and we had problems with breakers on our HMIs tripping intermittently. We put a handheld scope meter on the power line and there was harmonic distortion from the magnetic ballasts that we were using, but not so much that I thought would be a problem for a 25KVA (180A) generator. Throughout the night, each time an HMI went out unexpectedly in the middle of a shot, we eliminated one in our set up until we found a happy medium of a couple of babies, a 1200 Par and a 2500 Fresnel – much less than I would have expected a generator of that size could run reliably. I learned that hellish night that there are no hard and fast equations to determine how many magnetic HMIs you can safely run on a generator. The harmonics of ballast noise react in unpredictable ways.
Non Power Factor Corrected Electronic HMI Ballasts (Capacitve Non-linear load)

Left: Grid Power w/ 1.2Kw Arri non-PFC Elec. Ballast. Center: Conventional AVR Power w/ 1.2Kw Arri non-PFC Elec. Ballast. Right: Inverter Power w/ 1.2Kw Arri non-PFC Elec. Ballast.
The first thing to note is that the noise fed back into the distribution system by the electronic ballast creates harmonic distortion in the power generated by
both generators where it has no adverse effect on the grid power. The reason for this is that the magnitude of voltage waveform distortion is a function of the source
impedance and the relative size of the nonlinear load with respect to the capacity of the power generating system. As we see in the frame on the left, an HMI
light with non-PFC electronic ballast operating on a wall outlet will not produce voltage distortions because the impedance of the electrical path from the power plant to
the light is so low, the distortion of the original voltage waveform so small (less than 3%), and the plant capacity so
large, that loads placed upon it will not effect the voltage at the load bus.
However, as we see in the center and right frames, it is an all together different situation when plugging a 1200W non-PFC HMI ballast into a small portable generator. Where,
in this case, the sub-transient impedance of the generators are higher, and the percentage of the capacity of the generator that the non-linear electronic ballast takes up is
relatively high, current distortion from the harmonics created by the electronic ballast produces voltage distortion. These frames clearly demonstrate that the electrical artifacts
generated by electronic ballasts are amplified on small generators where they are not on grid power.

Even though RMS voltage remains the same, the Peak Value drops as a result of squaring of waveform from harmonic currents
The second thing worth noting is the type of voltage distortion created by the 1200 Watt non-PFC electronic ballast in the power of both generators. Since, according to Ohm’s Law
current reacts with impedance to cause voltage drop, in the case of capacitive non-linear loads like electronic ballasts that consume current only at the
peak of the voltage waveform (to charge their smoothing capacitor/s), voltage drop occurs only at the peak of the voltage waveform -
causing the “Flat Topping” we see in the oscilloscope shots above that is characteristic of this type of load. In other words, since electronic ballasts consume current only at the
peak of the voltage waveform, voltage drop due to system impedance occurs only at the peak of the voltage waveform. This explains why the
harmonic currents fed back into the distribution system by the electronic ballast has the effect of squaring off the voltage waveforms of the power generated by both types of
generators.

Left: Conventional AVR Generator w/1200W non-pfc electronic ballast. Right: Inverter Generator w/1200W non-pfc electronic ballast
A third thing worth noting is that the artifacts of harmonic distortion are amplified to a lesser degree in the inverter generated power (above right) than the non-inverter power (above left). Possible explanations for this are, as we saw above, the original waveform of the power generated by the EU6500is (our inverter generator) has less harmonic distortion at the outset than that originally generated by the EX5500 (our conventional AVR generator.) Another possible explanation is that the sub-transient impedance of inverter generators is appreciably less than that of conventional AVR generators. As discussed at the outset, in the case of inverter generators, voltage and frequency are independent of the engine. As a consequence inverter generators have very low internal reactance to changes in load. And, as discussed above, the generator with the lowest internal reactance to an instantaneous current change at a given load (impedance) will typically have the lowest value of total harmonic distortion under nonlinear load conditions (more on this latter.)

Voltage notching at the zero cross over is an indication of high frequency “wavelettes” within the primary sine wave.
A fourth thing to note is the character of the greater voltage distortion created by the 1200 Watt non-PFC electronic ballast in the power generated by the conventional generator
(EX5500.) As discussed above, each harmonic current in an electrical distribution system will cause a voltage at the same harmonic to exist when the harmonic current flows into
an impedance. In other words, the higher the system impedance the more likely harmonic currents will induce voltage at the same frequencies. These voltage harmonics appear in the
oscilloscope shot above as a zig-zag saw tooth pattern. This pattern does not appear in the voltage waveform of the inverter generator because of its’ much lower impedance. Once again,
we see that the generator with the lowest internal reactance to an instantaneous current change at a given load (impedance) will have the lowest value of total harmonic distortion under nonlinear load conditions.

Harmonics making up a Square Wave.
The zig-zag saw tooth pattern above is also an indication that a square voltage waveform is created by not just the primary current creating a voltage drop when it encounters system impedance, but in fact by many many
harmonic currents, at extremely high frequencies, also creating voltage drop as they also induce voltages at the same frequencies. Put another way, the square wave depicted on our scope is in fact comprised of many, many
voltage spikes, at extremely high frequencies, stacking one on top of the other. Harmonic currents at these frequencies can create RF (Radio Frequency) interference in sensitive electronic devices in close proximity to
it. Examples of RF interference include lines or fuzzy picture in set monitors, a buzz in audio tracks, and poor reception in radio mics.

Inverter Generator w/1200W non-pfc electronic ballast
In the case of the Inverter Generator (EU6500is), even though the same harmonic currents are fed back into the distribution system by the electronic ballast, because of its’ lower
system impedance and purer original power waveform, it retains an over all sinusoidal shape. The shape of its’ waveform is such that electrical devices that are dependent on peak
values may still operate effectively. It also exhibits much less severe distortion as a result of high frequency harmonic currents. The appreciable difference in voltage distortion
created here by the same light demonstrates that an inverter generator will provide cleaner power regardless of the type of load. Not only will a non-PFC electronic ballast have
fewer adverse effects on other equipment when operating on an inverter generator, it will operate more reliably as well (more on this when we look at the effect of multiple non-linear loads below.)
Power Factor Corrected Electronic HMI Ballasts (Capacitive Near Linear Load)
Because of the problems we have seen above, ballast manufacturers incorporate Power Factor Correction (PFC) circuits into their large electronic HMI ballasts (6-18kw)
by necessity. As discussed, a PFC circuit realigns voltage and current and induces a smoother waveform. As a result, the ballast uses power more efficiently with minimized return
current and line noise. Less heat is generated so the ballast operates more reliability.

Left: Grid Power w/ 1.2Kw P-2-L PFC Elec. Ballast. Center: Conventional AVR Power w/ 1.2Kw P-2-L PFC Elec. Ballast. Right: Inverter Power w/ 1.2Kw P-2-L PFC Elec. Ballast.
A quick look at the waveform comparison confirms these characteristics of power factor corrected HMI ballasts. A near linear load, the PFC electronic ballasts tested here has
no adverse effect on the respective waveforms. If anything, like the purely resistive load of the 2k incandescent light, it has a positive effect on the Honda EX5500. The
generator runs smoother under the PFC load than without a load. That fact is reflected in the smoother power waveform under load.

Left: AVR Generator No-Load Right: AVR Generator with PFC Electronic HMI Ballast Note the positive effect that
the near-linear load has on the power from a conventional AVR generator.
It is also worth noting that since PFC electronic ballasts have no adverse effect on power, the power generated by the inverter generator (EU6500is) retains its near perfect sinusoidal
waveform. For this reason, sensitive electronic equipment running on the same power will operate reliably and effectively.
All major manufacturers include power factor correction on large HMIs (6-18kw) because the heat and noise reduction is absolutely necessary for their reliable operation. However, because of the
added cost, weight, and complexity of PFC, manufacturers offer PFC as an option on medium-sized ballasts (2.5-4kw) and have not until recently offered PFC on HMI ballasts smaller than 1.2kw.
What sets the Power-to-Light (P2L) HMI Ballast product line apart from others is that P2L is incorporating Power Factor Correction (PFC) into their 800w, 1200w, 2.5kw/4kw ballasts at the same
price points as other manufacturer’s conventional non-PFC electronic ballasts.
Electronic Fluorescents Ballasts (Capacitve Non-linear Load)

Left: Grid Power w/ Kino Flo Wall-o-Lite. Center: Conventional AVR Power w/ Kino Flo Wall-o-Lite. Right: Inverter Power w/ Kino Flo Wall-o-Lite.
The first thing to note is that with a power factor around .6 the older style electronic ballasts of the Kino Flo Wall-o-Lite do return some harmonic currents to the power
stream that
distort the power waveforms of the generators – but to a much lesser degree than a non-PFC electronic HMI ballast. The second thing to note is that the distortion of the
voltage waveform is considerably less in the case of the inverter power (far right) than that of the conventional generator (center.) The reason for this is that, as
we saw above, the original waveform of the power generated by the EU6500is (our inverter generator) has less harmonic distortion at the outset than that originally
generated by the EX5500 (our conventional AVR generator.) Where the harmonic distortion of the power generated by the inverter generator is on par with the grid power,
what little voltage distortion there is comes as a result of the generator’s high sub-transient impedance.
Given how well Kino Flo ballasts interact with inverter generators, not to mention their versatility (they can operate both 5500K & 3200K lamps) and their efficiency
(they consume 1/10 the power of comparable incandescent soft lights), Kino Flo lights would appear to be an ideal light source to operate off of portable inverter
generators, and hence a good candidate for our better production system, except for one drawback. Fluorescent lights have a very broad soft light output that is hard to
control. The light also tends to drop off rapidly which means that to serve as key sources, the units need to be positioned close to the subject they are lighting. These
characteristics make them best suited to be fill sources in dramatic productions. They are really only suited to serve as key sources in documentary interview set ups where the keys are typically positioned close to the interview subject. In that capacity they generate a wonderful
soft light that wraps around the interview subject without wilting them. Given these characteristics, fluorescent lights in the past had only limited applications in
set lighting until the development by Kino Flo of their ParaBeam fixtures (see below for more details.)
__________________________________________________________________
The Effects of Multiple Non-Linear Loads
Thus far we have looked at the effect of just one 1200W non-pfc electronic ballast on 5500W & 6500W generators. What would be the accumulative effect of multiple non-linear loads on a generator? To see, I ran a package consisting of two Arri 1200 Par Pluses with non-pfc electronic ballasts, as well as a Kino Flo 4’ – 10 tube
Wall-o-Lite on the EX5500 (our conventional AVR generator). And for the sake of comparison, I ran the same package but with power factor corrected electronic HMI ballasts on the EU6500is (our inverter generator.) The difference between the resulting waveforms is startling.

Left: Conventional AVR Power w/ Pkg. of non-PFC Elec. Ballasts & Kino Flo Wall-o-Lite. Center: Scope time base adjusted to bring elongated waveform back on screen. Right: Inverter Power w/ Pkg. of non-PFC Elec. Ballasts & Kino Flo Wall-o-Lite.
The waveform on the left is no longer grid power but the power of the EX5500 distorted by the noise generated by multiple non-PFC HMI & Kino electronic
ballasts. As we would expect, since the percentage of the total capacity of the generator taken up by non-linear loads has increased, the amount of voltage
distortion in the power generated by the conventional AVR generator (the EX5500) has increased as well. The first artifact of the higher Total Harmonic
Distortion (THD) we notice is that the entire waveform is elongated such that it no longer fits on the oscilloscope display. The center frame is the scope
adjusted so that the entire waveform fits on its screen. The elongation of the waveform indicates that, despite the regulation of its engine speed by the
Barber Coleman AC Frequency governor, the greater load of non-PFC electronic ballasts has caused the generator to slow down slightly. As you would expect with a conventional AVR generator like the EX5500, the drop in RPMs results in a shift in the frequency (HZ) of the AC power waveform. The AC Frequency of the inverter generator, on the other hand, is unchanged by the additional non-linear load.

Left: Effect of harmonics of one non-pfc 1200W Electronic Ballast. Right: Effect of stacked harmonics of two non-pfc 1200W Electronic ballasts and solid-state ballast of Kino Flo Wall-o-Lite
The slow down of the EX5500 (our conventional AVR generator) might be attributable to the second artifact of the higher THD we notice - the amplitude of the high frequency “wavelettes” within the primary sine wave (the zig-zag saw tooth pattern) has also increased. The high voltage notching and heavy ringing transients present in the more
distorted waveform (above) is creating multiple zero-crossings within one cycle of the AC waveform. Since, the Barber Coleman engine governor used in this particular Honda EX5500 uses a
speed reference signal obtained by sensing the zero-crossings of the frequency of the output voltage inside the AVR unit, the multiple zero-crossings may be confusing the governor unit,
causing it to regulate the engine at the wrong speed.
There was a similar case reported on the Cinematographer’s Mailing List (CML.) It involved a Honda EX5500 equipped with a Barber Coleman governor. The EX5500 also had a digital frequency meter installed on the front panel. As reported in the post, the digital meter worked fine with tungsten lights. But, as soon as a 1200 Par was struck the digital meter read 120Hz rather than 60Hz. The gaffer knew the meter was malfunctioning, and not the governor. In order, to generate 120Hz power, the generator would have to run 7200 rpm and the pitch of the engine had not changed. When the gaffer metered the frequency of the generator is was slightly off, but they were not too concerned because they were using flicker free electronic ballasts
and there was no problem visible in the monitor or on playback. However as soon they tried to run a second 1200 Par the engine began heaving. The lights continued to run without visible flicker; but, a lap top that was being used to check the download of footage to the hard drive locked up. When generator power was metered again, the Hz was cycling over a wide range. If one of the 1200 pars was turned off, the frequency would become stable again.
Clearly the harmonic noise generated by the electronic ballasts was the problem in this case. The higher voltage notching and heavier ringing transients were creating multiple zero crossings and throwing the governor off speed.

Left: Effect of harmonics of one non-pfc 1200W Electronic Ballast. Right: Effect of stacked harmonics of two non-pfc 1200W Electronic ballasts and solid-state ballast of Kino Flo Wall-o-Lite
Also of note in the waveforms above is that the peak voltage has dropped even further, and the duration of the flat plateau is extended. Where there is appreciable voltage waveform distortion of this type, created by operating capacitive non-linear light sources on a conventional generator, other electrical devices operating on the same power may be unable to use this distorted “pseudo square wave” effectively. For instance, other production equipment that utilizes diode-capacitors and therefore depend on the peak value of the voltage waveform to operate effectively will work harder, if at all, on the squared off waveform caused by harmonic currents (above).
Most electronic production equipment in use today utilizes AC-to-DC diode-capacitor power conversion circuits in one way or another. As discussed
at length above, HMI and Fluorescent electronic ballasts utilize them to convert AC input power to DC power so that a Switch-mode Converter can
convert the DC power back to an alternating power waveform that ignites the lamp (50/60Hz Square wave in the case of HMIs and high frequency
sine wave in the case of Fluorescent ballasts.) The AC power supplies of lap top computers and video cameras, as well as DC battery chargers,
also use diode-capacitors to convert AC-to-DC. But, instead of using a Switch-mode Converter to switch the DC back to AC, they use power
conditioning components to supply DC power of a prescribed voltage. Regardless of the type of power (AC or DC) ultimately generated, what is
important to realize is that all diode-capacitor power conversion circuits place the load on the peaks of the supply AC. Given this fact, what effect would a highly distorted voltage waveform with peak voltage drop have
upon them? To see, lets first review what we know about how diode-capacitor circuits operate.

Step 1: Rectifier Bridge converts line frequency AC power to rectified sine wave. Step 2: rectified sine wave is flattened to DC by conditioning Capacitor.
If you will recall from our discussion of electronic ballasts, the diode-capacitor section converts the AC power to DC power by first feeding the
AC input through a bridge rectifier, which inverts the negative half of the AC sine wave and makes it positive. The rectified current
then passes into a conditioning capacitor/s that removes the 60 Hz rise and fall and flattens out the voltage - making it DC.

Yellow Trace: Rectifier Bridge converts AC power to rectified sine wave. Blue Trace: Stored Capacitor Voltage. Red Trace: Current drawn by capacitors once input voltage is greater than voltage stored in the capacitor (Blue trace.)
As shown in the illustration above, the diode-capacitor circuit only draws current during the peaks of the supply voltage waveform as it charges the conditioning capacitor to the peak of the line voltage.
Since the conditioning capacitor can only charge when input voltage is greater than its stored voltage, the capacitor charges for a very brief period of the overall cycle time. Since, during this very brief
charging period, the capacitor must be fully charged, large pulses of current are drawn for short durations. Consequently, all diode-capacitor circuits draw current in high amplitude short pulses that roughly
coincide with the peak of the voltage waveform. The remaining unused current feeds back into the power stream as harmonic currents.

A pseudo square wave after being rectified by a full bridge rectifier
Based upon how diode-capacitor circuits operate, what effect would a "flat topped" voltage waveform exhibiting peak voltage drop (like the one pictured above) have upon loads, like lap tops, camera power
supplies and battery chargers, that also utilize SMPSs? If we compare one half
cycle of a rectified sine wave to one half cycle of the distorted pseudo square wave generated by just one non-pfc 1200W electronic ballast,
we see that one consequence is that the period during which the capacitors of their SMPSs must recharge is appreciably shortened. Given a shorter interval to
charge, the capacitor/s will draw current in even higher amplitude shorter bursts. The diode-capacitor circuit therefore works harder, drawing more current during an even briefer charging period, reducing its power
factor and increasing its apparent power or load. As a consequence protective circuit breakers may trip or fuses blow.

Left: half cycle of rectified sine wave. Right: half cycle of rectified pseudo square wave. Blue Line: Minimum Capacitor Voltage. Red Lines denote interval during which current will be drawn by capacitors once input voltage is greater than voltage stored in the capacitor.
Another adverse effect is that more harmonic currents are generated as less of the power waveform is used by the circuit. In fact, a viscous
cycle can get started. The more harmonic currents that are generated, the more distorted the power supplied by the generator becomes. The more
distorted the power waveform becomes, the more harmonic currents are generated. In this fashion, something akin to a feedback loop can get started
until the effect of the harmonics is enhanced to the point where equipment stops working all together.

Blue Line: Minimum Capacitor Voltage. Red Lines denote interval during which current will be drawn by capacitors once input voltage is greater than voltage stored in the capacitor.
To see why this might happen we have only to compare the pseudo square wave created by the single non-PFC 1200W electronic HMI ballast to that
created by the 2500W package of non-PFC electronic HMI and Kino ballasts above. Based upon our discussion of how diode-capacitor circuits operate,
we can see in the oscilloscope shot on the right that the peak value of the psuedo square wave created by the 2500W package (after it has be rectified)
may not reach a sufficient level to charge the capacitor/s of a power supply. Whether the ballast of a light, or the AC power supply of a lap top,
the equipment may be starved of power even though its’ power indicator lights up, and a true RMS voltmeter would indicate about 120 volts on the line.
Common symptoms of power starvation are computers locking up, breakers tripping, and HMIs not striking or holding their strike. And, where now more of
the distorted wave falls outside a sinusoidal waveform, more excess heat will be generated in its' electrical components causing them to overheat and eventually burn up.

Unuseable portion of distorted waveform (shaded) dissipated in heat.
The magnitude of THD we see here, created by the harmonics of multiple non-PFC electronic ballasts stacking in our distribution system, goes a long way toward explaining this recent scenario: a local broadcast rental house sent several
non-linear editing systems to the Iron Man Triathlon for field editing. The laptops kept inexplicably locking up until their power supply was changed from a generator that was also supplying a large number of HMIs to the onboard generator
of the satellite truck. Once they were moved from the highly distorted power supply of the lighting generator to the highly refined power supply of the satellite truck the laptops operated flawlessly.

Same as Above Left: Conventional AVR Power w/ Pkg. of non-PFC Elec. Ballasts & Kino Flo Wall-o-Lite. Center: Scope time base adjusted to bring elongated waveform back on screen. Right: Inverter Power w/ Pkg. of non-PFC Elec. Ballasts & Kino Flo Wall-o-Lite.
The third frame on the right, is the same package of lights but with power factor corrected electronic HMI ballasts on the EU6500is (our inverter generator.)
As you can see, the difference between the resulting waveforms is startling. Even though we are running the same overall load in terms of watts, the fact
that the ballasts are power factor corrected, that the power generated by the inverter generator has very little inherent harmonic distortion
(less than 2.5%), and that the system impedance is very low, results in virtually no voltage waveform distortion of the power running through the distribution system. For this reason, sensitive
electronic equipment running on the same power will continue to operate reliably and effectively without damage even though the overall load on the
generator has increased. These frames clearly demonstrate that it is essential to have PFC circuitry in your ballasts, and to operate them on an inverter
generator, when your load consists primarily of HMIs and Kinos.
What it all Means
From the results of these tests the outline of a better production system is beginning to take shape. If there is one conclusion to be drawn from these tests, it is that when your lighting package
consists predominantly of non-linear light sources (HMI, Fluorescent & LED lights) it is essential to have PFC circuitry in the power supplies and to operate them on an inverter generator. The
combination of improved power factor and the nearly pure power waveform of the inverter generator makes it possible to power larger lights, or more smaller lights, than has ever been possible
before on a small portable gas generator.
In the past, the primary factors limiting the use of non-linear light sources on portable generators have been their inefficient use of power and the harmonic noise they throw back into the
power stream (below left.) However, with the recent incorporation of PFC circuitry in electronic HMI ballasts smaller than 4kw and the introduction of inverter generators, it
is now possible to generate clean stable set power (below right) capable of operating larger lights (HMIs up to 6kw or Quartz lights up to 5kw), or more smaller lights, off of portable gas
generators than has ever been possible before.

Left: Power waveform distorted by Non-PFC 1200W HMI ballasts on conventional generator.
Right: Near perfect power waveform of the same lights with PFC ballasts on inverter generator.
That is, where the harmonic distortion created by non-PFC power supplies reacting poorly with the distorted power waveform of conventional AVR generators, limited the number of non-linear light sources
you could use to
roughly half (65%) of the generators capacity. An inverter generator can be loaded to capacity with PFC HMI, Fluorescent, and LED power supplies because the near-linear nature of the load and the extremely
low harmonic distortion (less than 2.5%) of the original AC power waveform of inverter generators results in virtually no distortion of the power waveform.
What this means is that you can safely power bigger lights, or more smaller lights, on a portable gas generator than was ever possible before. For example, where a
Kino Flo ParaBeam 400 draws only 2 amps, the 8 Amp difference between using a PFC 1200W electronic ballast and non-PFC 1200W electronic ballasts, can mean the
difference between running four additional ParaBeam 400s on a portable generator or not. Given this new math, when you add up the incremental savings in power to be gained by using only PFC HMI ballasts, add to it energy efficient sources
like Kino Flos, and combine it with the pure waveform of inverter generators, you have what, I would argue, amounts to a paradigm shift in lighting with small portable generators.
Where before you could not operate more than a couple 1200W HMIs on a conventional AVR generator, now you can run a lighting package consisting of PFC 2.5kw, 1200, and 800 Watt HMI Pars, a couple of Kino Flo ParaBeam 400s, ParaBeam 200s, and a Kino Flo FlatHead 80 off of a Honda EU6500is Inverter Generator with the aid of a 60A Full Power Transformer/Distro. Given the light sensitivity of HD Camcorders, this constitutes a complete location lighting package for HD Digital Cinema productions.
Sizing Portable Generators
Sizing a portable generator for a lighting load can be very complicated. As we have seen, it matters not only what type of generator you use but also what type of power supplies the lights use because the Harmonic Noise that magnetic and non-Power Factor Corrected electronic ballasts (HMI, Kino, CFL, & LED included) kick back into the power stream can have a severe adverse effect on the power waveform of some generators, but not others. You, therefore have to be very vigilant when choosing a portable generator when your lighting package includes HMIs, Kinos, CLF lamp banks, & even LEDs – especially when it includes a number of LEDs.

Why? As more and more powerful LED fixtures come onto the market, they are going to be used in large arrays (like the one pictured above) or in quantity (like the production pictured below) on portable generators. In such situations, a potential hazard can develop when, because of the low wattage of the individual fixtures, users are lulled into complacency. If the LED fixtures are not Power Factor Corrected, then their low wattage can create a dangerous sense of false security when it comes to sizing a portable generator for the lighting load

For example, let's use (to keep the math simple) a hypothetical indie short film shooting a night scene on a city street with a DSLR. Because of the speed and light sensitivity of the camera and the amount of ambient light from store windows and street lamps they figure they can get away with a lighting package consisting of a 800W Joker Buglite to augment the background and two 40W 1x1 Litepanels to key their talent? For a generator they choose a conventional 1000W AVR generator figuring it will be enough (800W+40W+40W = 880W). Will it work? No. Why not, after all they are using only energy efficient LEDs and a Joker 800? The reason it won’t work is that because of the low wattage of the lights, they failed to consider their Power Factor when calculating the load that they will put on the generator and so they overload it. A careful analysis of the Power Factor of their lights (the Joker 800 and 1x1 Litepanels) indicates that their lighting package would in fact draw 1525W.
If we look at the technical specifications for the Joker 800 Buglite, we see that it uses a non-Power Factor Corrected ballast with a Power Factor of .58. According to the K5600 website, the Joker 800
ballast draws 12.5 Amps rather than the 7 Amps you would think using Ohm’s Law (800W/110V=7.2A.) What that means is that it has an Apparent Power of 1375W (110V x 12.5A = 1375W) or draws nearly twice
the power to generate 800 Watts of light output than a quartz instrument of the same wattage. Used on wall outlets, this relatively inefficient use of power is negligible because the power draw of the
Joker 800 fits easily on a standard wall circuit. However, the greater Apparent Power of the Joker 800 must be factored when using portable generators because the generator must be sized to supply the Apparent Power (1375W), even though only the True Power (800W) provides light.
The same is true when it comes to the 1x1 Litepanels. According to the manufacturer, the AC-to-DC power supply that Litepanel uses for their 1x1 fixtures has a Power Factor of .54 and so draws nearly
twice the power (an Apparent Power of 75W) for it’s true power output of 40W. If you were to use this lighting package on a 1000W conventional generator, the total Apparent Power of 1525W
(1375W + 75W + 75W = 1525W), would overload the generator because the “continuous load” rating of 1000W conventional generators are usually only 850W. Even though it’s power is cleaner and more
stable, you would not be able to run this package on a Honda EU1000is Inverter Generator either because the accumulative load of 1525W of
Apparent Power would overload its'
1000W capacity.
Could you operate this lighting package on a 2000W conventional generator? Again, the answer is “no.” As we discovered above, the greater Apparent Power of lights with a poor Power Factor is not the only
consideration when operating them on conventional generators. Of equal importance, is the Harmonic Noise that power supplies with poor Power Factor kick back into the power stream that severely limits the total amount of Leading Power Factor loads, as compared to Unity Power Factor loads, that can be reliably operated on conventional generators.

Left: Grid Power w/ 1.2Kw Arri non-PFC Elec. Ballast. Center: Conventional AVR Power w/ 1.2Kw Arri non-PFC Elec. Ballast. Right: Inverter Power w/ 1.2Kw Arri non-PFC Elec. Ballast.
Given the large sub-transient impedance of conventional generators, as the oscilloscope shots above illustrate, even a small degree of harmonic noise being fed back into the power stream will result in a
large amount of distortion in its’ voltage. Add to that, the fact that the original supply voltage waveform of conventional generators is appreciably distorted to begin with, and you have a situation
where the return of any harmonic currents by a non-PFC HMI, Fluorescent, or LED power supplies will result in significant waveform distortion of the voltage at the power bus and operational problems with the
generator voltage and frequency regulation.
This was graphically illustrated in the You-Tube video, “Compact Fluorescent verses The Generator", by Lighting Designer Kevan Shaw, when even an equivalent Apparent Power of CFLs, as incandescent light, would not operate without problems on his 850W generator.

In fact, Kevan Shaw’s You-Tube video illustrates the old math that it is not possible to load conventional generators beyond roughly 65% of their rated capacity for more than a short period when the
load consists of lights with a poor Leading Power Factor (Max Apparent Power of 540W/850W Generator = .64.) According to this old math, a 2000W conventional generator can only sustain a maximum load of 1300W for an extedned period of time.
Where the total Apparent Power of our lighting package consisting of a Joker 800 and a couple of 40W 1x1 Litepanels is 1525W, it will overload even a 2000W conventional generator.
Will our lighting package operate on a 2000W inverter generator like the Honda EU2000is? The oscilloscope shots above indicate that it would. Even though the non-PFC ballasts of our lighting package kick back the same harmonic currents, the voltage waveform of inverter generators retain an over all sinusoidal shape because of their lower system impedance and purer original power waveform. The appreciable difference in voltage distortion created here by the same light demonstrates that an inverter generator will provide cleaner power, and operate more reliably, regardless of the type of load.

Left: Grid Power w/ 1.2Kw P-2-L PFC Elec. Ballast. Center: Conventional AVR Power w/ 1.2Kw P-2-L PFC Elec. Ballast. Right: Inverter Power w/ 1.2Kw P-2-L PFC Elec. Ballast.
As the oscilloscope shots above illustrate, Power Factor Correction can be of tremendous benefit when operating HMIs, Kinos, and LEDs on portable gas generators because a PFC circuit realigns voltage
and current, eliminates the generation of harmonic currents, and induces a smoother power waveform at the distribution bus. PFC circuits successfully increase the power factor to as much as .98, making
power supplies with it near linear loads. As a result, a PFC ballast will use power more efficiently with minimized return current and line noise and also reduced heat, thereby increasing its' reliability. For
instance, if you were to replace the Joker Ballast with a Power-2-Light 800W PFC HMI ballast instead, the same head would draw 8 Amps at 110 Volts (instead of 12.5) and have an Apparent Power of only
880 Watts. If you were also able to replace the non-PFC AC power supplies of the 1x1 Litepanels with Power Factor Corrected ones, the oscilloscope shots above also indicate that you would likely be
able to operate the whole package on a 1000W inverter generator (880W + 40W + 40W = 960W.)

Current drawn by HMI Ballasts
We chose as our example a small indie short in order to keep the math simple. However, what is true of small lighting loads on small generators, is also true of larger lighting loads on larger generators.
For instance, before reading this article, you would have thought that you could reliably operate a 4kw HMI with non-PFC ballast on a conventional 6500W generator. But, where a non-PFC 4kw electronic
ballast will draw 58A at 120V it will overload a 6500W. To understand why, simply compare its’ Apparent Power of 6960W (58A x 120V = 6960W), to the continuous load capacity of a conventional 6500W
generator after de-rating it for a load with Leading Power Factor of .58 (6500W x .65 = 4225W.) Likewise, if you were to replace the non-PFC 4kw electronic ballast with a Power Factor Corrected one, the light would only draw 38A at 120V and have an Apparent Power of 4560W. And since, the ballast has a near Unity Power Factor, the 6500W generator would not have to be de-rated, and so could operate the 4560W Apparent Power load without a problem.
Where our tests have only compared the response of different light sources to the power waveforms of conventional AVR generators and inverter generators, let us now see how these generator types compare in the areas of speed stability, noise of operation, portability, and power capacity.
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Movie Blimped Inverter Generators
Production Features
Super Quiet
At first glance, you notice that unlike the typical “deluxe” AVR generators that use open frame designs that let everything “hang out,” the design of inverter generators consist of isolated chambers that are completely enclosed. For example, the noise of the Honda EU6500is generator has been greatly reduced by integrating a triple-chamber construction for the exhaust, engine and air intake. The exhaust chamber is now lined with a sound-absorbing material and houses a larger muffler that is secured to the frame and enclosed in the body of the generator, reducing both noise and vibration. The engine chamber is also lined with a sound-dampening material and has fully sealed panels to contain acoustic energy.
ILLUSTRATION COURTESY OF HONDA POWER PRODUCTS

Honda triple-chamber construction
The central air intake and exhaust system is designed to reduce mechanical noise by making airflow smoother by use of an air guide and intake nose. A newly designed rigid frame also aids in the sound attenuation of the EU6500i. And, instead of covering the frame with a single layer of plastic, the shell of EU6500is is made up of a layer of vibration-dampening foam sandwiched between layers of plastic. This sandwich of material prevents the enclosure from resonating which dramatically reduces sound levels.
While the totally new frame design of inverter generators in general greatly reduces noise, what makes the Honda inverter generators incredibly quiet, as well as more fuel efficient, is what Honda calls its’ micro processor controlled Eco-Throttle.
Eco-Throttle is simply the marketing name Honda uses to describe two of the characteristics of PWM inverter modules discussed above that make inverter generators considerably
quieter than conventional AVR generators. First, with their multi-pole rotors and small stator, inverter generators produce more electrical energy per engine revolution than
is produced in conventional AVR generators. Their greater efficiency, and the fact that the frequency of the power they generate is not linked to engine speed, means they can
run at much slower RPMs for a given load than a conventional AVR generator.
The second reason that inverter generators are quieter than conventional AVR generators is that their PWM inverter modules permit their engine speed to be varied with load. Which means that, at less than full load, the engine can be slowed down which tremendously reduces the noise it generates. Put simply, an inverter generator is much quieter because the engine does not have to run at full speed constantly as is the case with conventional generators. Honda calls these two features “Eco Throttle” because it results in a substantial reduction in fuel consumption. But, what is of more importance for motion picture production is that these features make inverter generators substantially quieter than traditional AVR models.
ILLUSTRATION COURTESY OF HONDA POWER PRODUCTS
 
Improved Noise Level and Fuel Consumption as a result of Eco-Throttle
Through this combination of innovative frame design and “Eco Throttle,” the Honda inverter generators achieve a noise reduction of ten decibels. Which makes them half as loud as the comparable EM7000is and ES6500 generators typically found at lighting rental houses. Honda's EU Series generators operate at 34 to 44 dBA at 50 ft. - well below what is required for trouble free location recording and quieter than our Crawford 1400 Amp “Movie Blimped” Generator.
ILLUSTRATION COURTESY OF HONDA POWER PRODUCTS

Comparative Noise Levels of Honda Generators and other sources.
Smaller Size
Inverter Generators provide stable, clean power in a smaller, lighter, quieter package. This is accomplished by integrating parts from the engine and generator set into a wholly new combination flywheel/alternator. In the case of the Honda EU6500is, this results in a generator that is more compact and 33% lighter than the comparable Honda EX5500. This is a significant reduction in footprint for a unit producing such a high power output.


ILLUSTRATION COURTESY OF HONDA POWER PRODUCTS
Combination flywheel/alternator makes Honda Inverter Generators smaller and lighter than convential AVR Generators

Solid as a Rock
If you will recall from our discussion at the outset, conventional generators, with simple two-pole cores, require Barber Coleman governors to govern their engines to run at a constant 3600 RPM to produce
stable 60 hertz (cycle) power. To regulate voltage, their AVR systems control the strength of the electro-magnetic field in the Alternator's Rotor through DC excitation. Voltage
and Frequency in conventional generators are intractably linked to their Engine/Alternator. Inverter generators by comparison do not have to run at a constant speed because the AC power they output is generated from high voltage DC power that is micro-processor switched according to a PWM control logic with a voltage stability of ± 1%, and Frequency stability of ± 0.01 HZ.
This simple fact, that the voltage and frequency of inverter generators is no longer linked to its’ Engine or Alternator, offers a number of benefits for filmmakers.
First off, leading power factor loads, like electronic ballasts, do not affect the regulation of voltage in inverter generators as they do in conventional AVR generators.
As discussed above, the AC power that inverter generators output is generated from a fixed high voltage DC that is modulated according to a PWM control logic to provide
a variable AC voltage and frequency. The DC voltage is generated by a fixed Diode Bridge Rectifier that converts the more than 300 three phase AC sine waves
(at frequencies up to 20 kHz) generated by the multi-pole Rotor to a fixed DC value (about 200 V in at least one unit). Since the inverter module completely
processes the raw power generated by the Alternator, the voltage of the AC power it outputs is no longer a function of the strength of the electro-magnetic field of the Alternator's Rotor, nor controlled by DC excitation.
Where the AC voltage generated by inverter generators is no longer controlled by DC excitation, the armature flux generated by harmonic currents in the Alternator Sator
no longer causes
erroneous voltage regulation as was the case with conventional AVR systems. Consequently, leading power factor loads do not cause voltage regulation errors in
inverter generators as they did in conventional AVR generators.

TABLE COURTESY OF KIRK KLEINSCHMIDT
A second benefit to filmmakers is that inverter generators have very low sub-transient impedance. If you will recall from our earlier discussion, impedance is a function of
the internal reactance of the engine to changes in load. But, since the inverter module completely processes the raw power generated by the Alternator (converting it to DC
before converting it back to AC), the AC power it generates is completely independent of the Engine/Alternator. So independent, in fact, that the microprocessor can actually
vary the engine speed without effecting the voltage or frequency of the power output. Now that the inverter module separates the internal reactance of the engine from the
power output, harmonic currents encounter very little impedance; and, as is evident in the oscilloscope shots above, there is considerably less voltage distortion at the
load bus. The net benefit to filmmakers is that non-linear loads, like electronic HMI & Kino ballasts, do not adversely effect the power of inverter generators as they do
the power of conventional AVR generators.
The rock solid power and low sub-transient impedance of inverter generators enable you to operate larger non-linear loads on a portable gas generator than has been
possible before. For instance, we have struck 6k HMI Pars on a modified Honda EU6500is inverter generator without problem. These features of inverter generators
make them an ideal power source for motion picture production with non-linear lighting loads.

Honda's sophisticated micro-processor based "i-monitor" control system
Finally, with micro-processor based control systems, most inverter generators also incorporate a suite of temperature, voltage and current sensors to make sure everything is operating correctly and to ensure that the generators can put out extra power for short time periods to start demanding loads such as electric motors which can require three times the amount of power to start as they require to run.
New Life to Magnertic HMI ballasts
If you don’t have access to the newest Power Factor Corrected (PFC) electronic ballasts, you are better served by using the older magnetic ballasts on an inverter generator (like the Honda EU6500is) over non-PFC electronic ballasts on conventional AVR generators (like the Honda EX5500 or ES6500.) Where this is contrary to the conventional wisdom, allow me to explain some of the advantages to operating magnetic ballasts on inverter generators.
With a frequency variance of only hundredths of a cycle, magnetic ballasts will operate “flicker free” on inverter generators, without the need for costly crystal
governors, as long as you shoot at one of the many safe frame rates. Besides the extra bulk and weight of magnetic ballasts, the smaller magnetic ballasts
(575-2500W) offer the distinct advantage of being less expensive and drawing less power (13.5A versus 19A for a 1.2kw) once they have come up to speed than
the commonly available non-PFC electronic equivalents. Finally, magnetic ballasts will operate more reliably on inverter generators, than non-PFC electronic
ballasts operate on AVR generators. The reason being the leading power factor caused by the capacitive reactance of non-PFC electronic ballasts have a more
severe effect on the power waveform of conventional AVR generators than do magnetic ballasts on the power waveform of inverter generators.

Left: Grid Power w/ no load has a THD of <3%. Center: Conventional AVR Power w/ no load has a THD aprox. 19% Right: Inverter Power w/ no load has a THD of aprox. 2.5%.
With an inherently distorted voltage waveform (see above) of upwards of 19.5%, high impedance AVR generators (like the Honda EX5500 or ES6500) do not interact well with the harmonic currents generated by the capacitive reactance of electronic ballasts. The net result is that the harmonic currents thrown back into the power stream, result in severe voltage waveform distortion and ultimately to equipment failure or damage.

Characteristic voltage waveform of a non-PFC electronic HMI ballast on grid power (left), on power generated by a conventional AVR generator (middle), and power generated by an inverter generator (right)
This is clearly evident in the oscilloscope shots (reproduced above) of what results from the operation of a 1200W HMI with non-power factor corrected ballast on grid power (left), on a conventional AVR generator (Honda EX5500) (middle), and inverter generator (Honda EU6500is)(right.) The adverse effects of the harmonic noise generated by non-PFC electronic ballasts and exhibited here in the middle shot, can take the form of overheating and failing equipment, circuit breaker trips, excessive current on the neutral wire, and instability of the generator’s voltage and frequency. Harmonic noise of this magnitude can also damage HD digital cinema production equipment, create ground loops, and possibly create radio frequency (RF) interference.

Characteristic voltage waveform of a 1200W magnetic HMI ballast on grid power (left), on power generated by a conventional AVR generator (middle), and power generated by an inverter generator (right)
As is evident in the oscilloscope shots (reproduced above) of a 1200W magnetic HMI ballasts on grid power (left), on power generated by a conventional AVR generator (middle), and power generated by an inverter generator (right), the lagging power factor caused by the inductive reactance of magnetic ballasts has by comparison only a moderately adverse effect on the power waveform. Outside of causing a voltage spike in the inverter power, magnetic ballasts actually show a positive effect on the already distorted power waveform of the Honda EX5500 conventional generator. For this reason magnetic ballasts work better on conventional generators with frequency governors than do non-PFC electronic square wave HMI ballasts.
These oscilloscope shots show that if you don’t have access to the newest PFC electronic ballasts, the older magnetic ballasts are in fact cleaner running on portable gas generators than non-PFC electronic ballasts. And, where inverter generators like the Honda EU6500is do not require crystal governors to run at precisely 60Hz, you can operate magnetic HMI ballasts reliably on them.
Of course there are downsides to using magnetic ballasts. One down side is that you are restricted to using only the safe frame rates and shutter angles. But, when you consider that every film made up to the early 1990s were made with magnetic HMI ballasts you can see that being limited to the safe frame rates is not all that restrictive. Another downside to magnetic ballasts is that you can’t load the generator to full capacity because you must leave “head room” for their higher front end striking load.
When choosing HMIs to run off portable generators, bear in mind that magnetic ballasts draw more current during the striking phase and then they “settle down” and require less power to maintain the HMI Arc. By contrast, an electronic ballasts “ramps up.” That is, its’ current draw gradually builds until it “tops off.”
For example, even though a 2.5 magnetic ballast draws approximately 26 amps you will not be able to run it reliably on the 30A/120V twist-lock receptacle of either
a 6500W Inverter or AVR generator. As mentioned above, magnetic ballasts have a high front end striking load. So, you must leave “head room” on the generator to accommodate the strike. And, even though the twist-lock receptacle is rated for 30 Amps, 6500W generators are only capable of sustaining a peak load of 27.5 Amps on a single leg of the generator for a short period of time. Their continuous load capacity (more than 30 minutes) is 23 Amps per leg. And, if there is any line loss from a long cable run the draw of a 2.5 magnetic ballast will climb to upward of 30 Amps. To make matters worse, as we saw in the oscilloscope shots above, the lagging power factor caused by the inductive reactance of the magnetic ballast causes a spike in the supply voltage that can cause erratic tripping of the breakers on the generator or ballast. In my experience the load of a 2.5kw magnetic ballast is too near the operating threshold of an unmodified 6500W generator for it to operate reliably.

Honda EU6500i Inverter Generator with 60A Full Power Transformer/Distro
The only sure way to power a 120V 2.5kw (or even a 4kw) HMI magnetic ballast on a portable gas generator is from its' 240V circuit through a 240v-to-120v step down transformer like the one we manufacture for the Honda EU6500is (pictured above.) A transformer will step down the 240V output of the Honda EU6500is generator to a single 120V circuit that is capable of accommodating the high front end striking load, and even the voltage spikes, of either a 2.5kw or 4kw magnetic ballast at 120V (see below for additional benefits to using step-down transformers with portable gas generators.)
Since magnetic HMI ballasts will operate flicker free at all standard frame rates on them (without the need for a crystal governor), inverter generators give new production life to older 120V magnetic HMI ballasts.
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For all their benefits true sine wave inverter generators had limited applications in motion picture production because they had limited output. It was not until the introduction of the
Honda EU6500is inverter generator in the fall of 2007 that the benefits of inverter technology became available in a generator with output comparable, if not greater, to the conventional
AVR generators commonly used in motion picture production. The benefits of inverter technology discussed above mean that inverter generators can put out 20% more power than conventional
AVR generators using the same engines. For instance, it is possible to get 7500W of continuous power in a single 120V circuit out of a Honda EU6500is generator. That is enough power
to run a lighting package consisting of a 2.5kw, 1200, & 800 HMI Pars (with PFC ballasts), a couple of Kino Flo ParaBeam 400s, a couple of ParaBeam 200s, and a Flat Head 80. Given the
light sensitivity of electronic imaging systems, this is just about all the light needed to light a large night exterior.
In order to understand how it is possible to get 7500W of continuous power in a single 120V circuit out of a Honda EU6500is generator, one must first appreciate two
things about the continuous load ratings given for generators. First, the factors generator manufacturers use to derive load ratings include not only the mechanical
components (engine & alternator), and the electrical components (circuitry & wiring), but also the prevailing electrical codes of the market for which it is intended (where & how it will be used) and the brand
image of the manufacturer (life expectancy of the product.) A quick survey of the wide range of continuous load ratings (5000W-7000W) of generators, by manufacturers other
than Honda, using the same Honda GX390 engine as the EU6500is supports this fact. Second, when Honda engineered the EU6500is it was not only for the North American market.
Like a car, Honda engineered a base model for the world market that they then customize for the different national markets. The difference between the various national models
is primarily in the power output panel, which is configured according to the electrical standards and prevailing codes of the national market in which the generator
will be used. For these reasons, the true power generating capacity of the Honda EU6500is is open to speculation.
When you compare how Honda outfits the base model of the EU6500is generator for the European and UK markets, where the standard circuit for domestic power is 230/240 Volts
and 16 Amps (3680/3840 Watts), to how Honda outfits the same generator for the North American Market, where the standard circuit is 120 Volts and 20 Amps (2400 Watts), one
realizes that the continuous power rating of 5500w for the North American Model of the generator is under-rated. Where England and Ireland have not entirely conformed to
the European Union Standard of 230 Volts, but still generate 240V power, Honda must engineer into the base model the capacity to generate 240V/16A circuits (3840 Watts/circuit) for the UK market.
Empirical tests show that, in fact, the base model is designed to generate two 240V/16A circuits or 7680 Watts (2x3840W/circuit = 7680W.)
To empirically test how much more generating capacity the base model is capable of, we tapped an EU6500is in a similar fashion to the UK model and used a step-down transformer to convert the 240 Volt output to a single 120
Volt circuit. We then used the generator's overload sensor to empirically test its' capacity with a load bank following the parameters as set forth in the manual:
"If the generator is overloaded, or if the inverter is overheated, the red overload indicator will go ON.... When an electric motor is started, the red overload indicator may come on. This is normal if the red overload
indicator goes off after about five seconds.... When the generator is operating overloaded, the red overload indicator will stay ON and, after about five seconds, current.... will shut off"
Gradually increasing the load from the load bank, we found that we could power a continuous load of up to 7680 Watts without the overload indicator coming on. When we exceeded 7680 Watts, the red indicator
blinked intermittently. When we exceeded 7800 Watts the red indicator came on continuously and power was cut off to the receptacles. Since, according to the Honda Manual it is normal for the overload indicator to come on
for short front-end loads, like electric motors starting, our results suggest that the continuous load capacity of the base model, or the EU6500is after our modification, is actually 7680 watts. And, when you consider that
electric motors require up to three times more power to start than is required to keep them running, suggests that the peak rating is actually well above 7680W. Our tests confirm that the
inverter module of the EU6500is generator is in fact capable of generating more power than is provided to us by the North American Power Output panel.
It makes perfect sense that Honda would engineer a continuous load capacity of 7680 watts into the base model of the generator when you consider the electrical systems of the UK countries. Where we have 15 and 20A circuits,
they have 13 and 16A circuits. Two 240V/16A circuits provides a total of 7680W (3840 Watts/circuit x 2 = 7680 Watts) which is what we found that the electronic circuit breaker in the inverter module is set for. Suspecting that
it was not just coincidental that the actual continuous load capacity of 7680 Watts is the equivalent of two standard household circuits in the UK, we took our suspicions to
Honda Motors USA, who confirmed that in fact the base model of the EU6500is generator is engineered to generate the equivalent of two UK circuits and has a continuous load capacity of 7680Watts. When confronted, they also
admitted to us that when they configure the base model for the North American market with 120V circuits, they are not fully utilizing the power generating capacity they have built into the machine for the worldwide market.
Even though the inverter module of the EU6500is may support continuous loads of 7680W does not necessarily mean that the generator's engine can. Quite often, when you find yourself in the situation with a conventional AVR
generator, where HMI lights that have been running fine, suddenly cut out when another light is turned on, it is because the generator engine bogs down under the additional load. As the engine rpms drop, frequency and voltage
drop as well, causing the HMI lights to cut out from low voltage. For this reason it is important to factor engine capacity whenever sizing a generator for an HMI load.
The power behind the EU6500is is Honda's workhorse GX390 engine. According to Honda literature, the GX390 is a 13HP Twin Cylinder, Overhead Cam (OHV), Liquid Cooled gas engine with a Displacement ( Bore X Stroke ) of 389cc
/ 23.7 cu. inches and a Gross Torque of 20 ft-lb at 2,500 rpm. This same engine is used worldwide by manufacturers of all kinds of power tools, from pumps to roto-tillers, and is rated with a maximum output of 9600 Watts
(13ps, 13bhp) at 3,600 RPM.
Surveying the continuous load capacity ratings of 5000W-7000W of generators by manufacturers other than Honda that use the GX390, one quickly realizes that the factors generator manufacturers use to derive these ratings
include more than just the mechanical components (engine & alternator.) To get an idea of the true power generating
capacity of this engine we need look no further than the Coleman Model PM0497000 Generator. Coleman uses the Honda GX390 engine in this conventional "industrial generator" it manufactures for the construction market. Colman
rates the Model PM0497000 Generator at 7000W continuous and 8750W peak load capacity. Where the Model PM0497000 Generator is manufactured by Coleman for the construction trades to run power equipment with high front
end loads it is probably safe to bet that Coleman is under-rating the PM0497000 generator at 7000W continuous and 8750W peak load capacity.
Using Coleman's rating of the Model PM0497000 Generator as a conservative bench mark of the engine's true capacity, and taking into account that an inverter generator draws 20% more power from each revolution of the
generator core (thanks to its multiple coils and multiple magnets generating several hundred overlapping sine waves per revolution), it is probably safe to assume that the GX390 engine in an inverter generator is
capable of generating at least 8400W of continuous and 10500W of peak power.
Where Honda does not make this information public and electronically breakers the power output at 7680W, there is no way of knowing for certain what the actual generating capacity of the GX390 engine is in an inverter generator like the EU6500is. We can however safely conclude that the GX390 provides
a quiet and efficient power plant that more than compliments the 7680W continuous power output of the EU6500is' inverter power module.
To understand why Honda under-rates the EU6500is generator in the North American market, one only has to look to the guidelines for the use of portable generators set by the Occupational Safety and Health Administration (OSHA) in this country.
In Article 29 CFR 1926.404(b)(1)(ii), OSHA exempts portable gas generators from the requirement to provide Ground Fault Circuit Interrupters (GFCIs) if they meet certain criterion. Article 29 CFR 1926.404(b)(1)(ii) reads as follows:
"Receptacles on a two-wire, single-phase portable or vehicle mounted generator rated not more than 5kW (latter increased to 5.5kw continuous load), where the circuit conductors on the generator are insulated from the generator frame and all other
grounded surfaces (a Floating Neutral configuration), need not be protected with ground-fault circuit interrupters."
What this means is that under these conditions, the manufacturer does not need to put the normally required GFCIs on a generator. It is because OSHA requires that portable generators rated for more than 5500W of continuous
load have GFCIs, that Honda, as well as other
generator manufacturers, do not rate "Home Standby" generators, like the Honda EU6500is, for more than 5500W continuous load. To understand why, we must understand how GFCIs work and why you can't have them in a generator designed for home standby
power.
OSHA requires that portable generators that do not meet the exemption above be monitored by a Class A GFCI to protect against serious harm from electrical shock. A Class A GFCI is designed to interrupt power to a circuit if it detects current
leakage that is greater than 6 mA. At 6 mA, almost all adults and children can let go of the source of a shock. At higher currents, people are progressively less able to overcome muscle contractions caused by the shock, and therefore less able
to disconnect themselves from the fault source. A GFCI will de-energize the circuit in less time than it takes to receive a harmful amount of current - which is why OSHA requires them on portable generators.

GFCI protection is a problem on a generator designed for home standby power because of the way they work. A GFCI works by monitoring the current between the hot conductor and the neutral conductor. When it senses a very small difference in current between
the two, typically three to six milliamps (0.003+/-mA - 0.006mA), it trips by opening internal current conducting contacts. The reason Home Standby generators can not have GFCIs is that, for GFCIs to operate reliably the Neutral of the generator must be
bonded to ground through the frame of the generator (a Bonded Neutral generator.)

Bonding Neutral to ground through the generator frame is a problem in home standby applications because as
illustrated in the figure below our National Electrical Code (NEC) also requires the main service head (panel) of homes to also have Neutral bonded to ground. Where that is the case, if the generator Neutral is also bonded to ground,
two parallel paths back to the generator are created, one using the neutral wire and one using the ground wire. The neutral current will then flow through both the Neutral and Ground conductors. Since the Hot and Neutral wires pass through
the ground fault sensor but the Ground wire does not, a GFCI on the generator will sense current imbalance and trip as soon as the genrator is turned on. In the case of home standby power, the Neutral in the generator cannot be bonded to ground
when the Neutral is bonded to ground in the main service panel. For this reason generators, like the Honda EU6500is, that are designed for home standby power applications have unbonded Neutrals (they are called "Floating Neutral" generators.)

While a Floating Neutral design enables it to be used for home standby power, an unmodified Honda EU6500is would not meet OSHA guidelines for use on job-sites if it were rated at its' true power because they can not
offer the GFCI protection mandated by OSHA in generators larger then 5500W. GFCIs require a bonded Neutral, the EU6500 has to have a Floating Neutral in order to provide home standby power. In other words, in the North American market Honda has to under-rate the EU6500 in order qualify for the exemption from
OSHA's mandate that they provide GFCI protection. In order to rate the generator higher, our national codes would require Honda to put GFCI protection on the EU6500is. But, if they did that, the generator would not be applicable
for home standby power which is it's primary market. This is why Honda under-rates the EU6500is at a continuous load rating of 5500W when our empiracle tests proved it is capable of much more. This is also why you do not see portable gas generators designed for home
standby power by any manufacturer (Honda, Onan, Subaru, Coleman, or Yamaha) with continuous load ratings over 5500W - they too would be required by OSHA to provide GFCI protection if they were rated for more than 5500W (use
this link for a detailed explanation of OSHA
requirements and why almost all portable generators do not meet them.) Unfortunately for filmmakers the
implication of the OSHA guidelines for portable generators is that none of the Honda inverter generators (the EU series and EM5000is) meet OSHA requirements for use on film sets. So what is a film electrician to do when they have to operate a
portable generator in wet hazardous conditions that require GFCI protection?

A 100 GFCI with our 60A Transformer/Distro meets OSHA requirements for use of a Honda EU6500is generator on work sites.
Our system meets OSHA requirements for the use of Floating Neutral generators like the Honda EU6500is on set. Our 60A Full Power Transformer/Distro bonds the Neutral to ground on its' secondary or load side. Our
HD Plug & Play Gen-set set-up is in fact identical to that of a bonded building service head fed by a home standby generator. With Neutral and Ground bonded only in our Transformer/Distro
and not in our modified Honda EU6500is, you have a complete circuit on the load side of the Transform/Distro that creates a low resistance path (illustrated below) for fault current back to the transformer
windings and a breaker that will trip from the over-current situation.

Where this is the case, to completely comply with the OSHA requirements for the use of a EU6500is on set all you need to do is use GFCI protection downstream of our 60A Full Power Transformer/Distro. With the Neutral and Ground bonded in our
60A Transformer/Distro, in the event of a Fault, current will go to ground and GFCIs will operate reliably even when the power is being generated by a Floating Neutral generator like the EU6500is (use this link for more details.)
Our 60A Full Power Transformer/Distro offers many benefits when used with our modified Honda EU6500is (use this link for more details), but the ability to use GFCI protection in wet conditions or
locations has got to be the greatest benefit of all. Not only can you use a generator that is quiet and produces clean power, but it also makes it possible to use GFCI technology, like film style 100A GFCIs, that are specifically designed
for motion picture applications (use this link for more details about the advantages to using GFCI protection specifically designed for motion picture applications.)

100A GFCI provides ground fault protection on wet locations
There are other reasons for Honda to under-rate the Honda EU6500is, especially when their market research shows that they do not need to provide more than 5500W continuous load rating for the average consumer. One is
maintaining the Honda brand image of manufacturing generators that will last forever. Honda claims the life of the GX390 engine in their generators is an impressive 2000 hours. One of the reasons they may obtain that
kind of longevity is by under rating their generators for their consumer markets. The type of load that is put on a Home Standby generator is another reason for Honda to under-rate the EU6500is.
The typical load a consumer places on a Home Standby generator is Reactive (the computers, microwaves, & fluorescent lighting loads of RVs or Homes), as opposed to the typically Resistive loads of a construction site (motors,
heaters, and incandescent lighting)
loads of construction sites.) Since, Reactive loads generate harmonic currents that can distort the voltage waveform and can have a severe adverse effect on both the generator and the equipment operating on it,
Honda may de-rate the inherent generating capacity of the Honda EU6500is - i.e. lowers its' continuous load rating - in order to build in a safety margin that will allow for the harmonic distortion generated by
Reactive Loads (both inductive and capacitive.) In other words, the reason that the same engine and generator components (the gen-set) marketed to the construction trades (the Coleman Model PM0497000) carries a higher continuous
load rating than that marketed for RV Power or Home Standby Power (the Honda EX5500, ES6500, EU6500is, & EM7000is) is that the load that the construction trades put on generators does
not create harmonic currents. Where as, the same gen-set marketed for RV Power or Home Standby Power will carry lower load ratings because the typical load put on it creates harmonic currents and distortion of the power
waveform that can have severe adverse effects on both the generator and the equipment operating on it.
Why Honda would de-rate the load capacity of its' generators intended for markets that use non-linear reactive loads is graphically illustrated in the You-Tube Video
“Compact Fluorescent verses The Generator" discussed previously. In our discussion above, we covered a
number of adverse effects that harmonic noise can have on a generator. To review they include over heating, voltage regulation and speed regulation problems. Kevan Shaw's You-Tube Video “Compact Fluorescent verses The Generator" demonstrates that the result of these effects on the
operation of a generator can be so severe that they can not possibly be ignored when determining the "Continuous Load" rating of a generator.

If you will recall, when Kevan intentionally "overloads" his 850W two stroke gas generator with a purely reactive load consisting of 30-18W CFL bulbs, he is in fact (because of the
CFL's poor Power Factor of .5) loading the generator with 1120W of Apparent Power. But, because this apparent power load is drawn in short amplitude bursts, it never trips the
breaker on his 850W generator. Instead, the generator simply goes berserk. Where the average user of a portable generator can not distinguish between Resistive and Reactive Loads, manufacturers routinely de-rate the Peak
Load capacity of a gen-set for safety reasons when it will likely operate a predominantly Reactive Load. When, in his demonstration, Kevan turns off the 18W CFL bulbs one at a time until the generator stabilizes with a
Leading Power Factor load of 270 Watts (15 – 18WCFL bulbs), he is in effect doing what generator manufacturer’s do to determine the Peak Load rating of a generator for the RV & Home Standby markets: they determine the maximum
Leading Power Factor load, as compared to Unity Power Factor loads, that a gen-set can reliably operate. What Kevan Shaw finds is that it is not possible to load his generator beyond roughly 65% of it's rated capacity when the
load consists entirely of lights with a poor Leading Power Factor (Max Apparent Power of 540W/850W Generator = .64.)
Reliable operation is only one criterion that manufacturers use to determine a gen-set’s maximum Leading Power Factor load. Another criterion is the effect that continuous exposure to harmonic currents will have on a gen-set.
The overheating of a generator’s wiring and windings as a result of sustained exposure to high Total Harmonic Distortion (THD) levels is an effect of harmonics on generators that manufacturers take into account in
the Continuous Load Ratings (longer than 30 minutes) that they give to generators.
As discussed above, harmonic currents produce heat in several ways. First, harmonic currents can stack on top of one another, creating very high currents returning
to the power source on the neutral wire. If the neutral of the generator has not been oversized to accommodate the additional current, these high currents can
cause excessive heat on the neutral bus of the generator. Second, harmonic currents produce high frequency flux change in the Alternator's Stator core which can
lead to them overheating. Higher core temperatures, in turn, result in higher winding temperatures. Winding heating is, in fact, proportional to effective
or RMS current squared. Rotor loss can also occur because harmonic currents in the Stator will induce currents in the pole faces and windings of the Rotor. And, of course,
harmonic currents cause increased resistive losses everywhere in the generator's electrical distribution, resulting in increased temperatures everywhere, not
only in the Alternator windings.
For these reasons, if a gen-set is intended for a market whose typical load is Reactive (the computers, microwaves, & fluorescent lighting loads of RVs
or Homes), as opposed to Resistive (the motors, heaters, and incandescent lighting loads of construction sites), the manufacturer de-rates the inherent generating
capacity - i.e. lowers the continuous load rating - for that gen-set for that market in order to reduce flux in the Stator core
that leads to heat build up, and eventually to the windings burning out under "normal load." In other words,
the lower Continuous Load rating builds in a safety margin that allows for
the harmonic distortion generated by Reactive Loads (both inductive and capacitive.)
As we have seen Honda has several good reasons to under-rate the generating capacity of the powerful EU6500is for the North American consumer market. But, the fact that they have to keep its' continuous load rating
to no more than 5500W in order to be exempted from mandatory GFCI protection is probably the primary reasons they
under-rate the powerful EU6500is (note the higher rated Coleman generator was for the construction market and offers GFCI protection.)
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A Production System for a New Age
Where, the typical load placed on portable generators in motion picture lighting applications today consists predominantly of Reactive Loads like HMI & fluorescent ballasts that generate harmonics,
the conventional wisdom among Gaffers is to further de-rate the Continuous Load capacity over and above what the generator manufacturer has already de-rated the generator set for the RV or Home Standby Power
applications. The conventional wisdom is to further de-rate the continuous load capacity of portable generators because the means by which the industry has successfully dealt with harmonics has, in the
past, not been available to the user of portable gas generators.
The means by which the motion picture industry has more or less successfully dealt with harmonics - namely the over-sizing of generators, the over-sizing of neutrals, the incorporation of power factor correction circuitry in large HMI ballasts, and finally the use of generators with 2/3 pitch windings (Crawford Studio Generators) are generally not available to users of small portable generators as their primary source of power. That is because, productions using portable gas generators are using them by necessity. For budgetary or logistical reasons, it is simply not an option to upscale their generator and customize their distribution package to accommodate a heavily harmonic load. The only alternative is to de-rate the continuous load capacity of the generator and distribution equipment.
Where the severe harmonic noise of a typical lighting package exhibited above can cause overheating and failing equipment, efficiency losses, circuit breaker
trips, excessive current on the neutral return, and instability of the generator's voltage and frequency, the conventional wisdom in the past has been to not
load a generator beyond 65% for more than a short period (the maximum recommend continuous load on a 6500W generator, with a continuous load rating of 5500W, would
be roughly 4200 watts.) Like the generator manufacturer, by de-rating the load capacity, the Gaffer minimizes the adverse effects of high THD so that the generator will operate more reliably.
The New Math of Low Line Noise
This conventional wisdom, however, no longer holds true of inverter generators when used with Power Factor Corrected (PFC) HMI & Kino ballasts. For example, the power waveform below on the right, is the same 2500W load but with power factor correction operating on our modified Honda EU6500is Inverter Generator. As you can see, the difference between the resulting waveforms is startling. Even though the load is the same, the fact that it is power factor corrected and the power is being generated by an inverter generator, results in virtually no power waveform distortion. What this means is that an inverter generator can be loaded to capacity with PFC HMI and Kino Flo ballasts without its' stator core overheating from high frequency flux change, its electrical wiring overheating from excessive resistance, and its distribution panel overheating from a high neutral return. The substantial reduction in line noise that results from using PFC ballasts on the nearly pure power waveform of an inverter generator creates a new math when it comes to calculating the continuous load you can put on a portable gas generator.
According to this new math, it is possible to maximize the continuous load that can run off of an inverter generator, by using HMI and Kino Flo lights with Power
Factor Corrected ballasts. Where, in the past we had to de-rate portable generators because of the inherent short comings of conventional generators when dealing with the harmonic
noise generated by non-PFC electronic ballasts; now an inverter generator can be loaded to capacity. According to this new math, when you add up the incremental savings in power
to be gained by using only PFC HMI ballasts, add to it energy efficient sources like the Kino Flo Parabeam fixtures, and combine it with the pure waveform of inverter generators,
you can run more HMI lights on a portable gas generator than has been possible before. For example, the 7500W capacity of our modified Honda EU6500is Inverter Generator can power
a lighting package that consists of a PFC 2.5kw HMI Par, PFC 1200, & 800 HMI Pars, a couple of Kino Flo ParaBeam 400s, ParaBeam 200s, and Tegra 400s. Given the light
sensitivity of HD cameras, this is pretty much all the light you will need to light even night exteriors.

Left: Distorted power waveform created by Non-PFC 1200W HMI ballasts on conventional generator.
Right: Near perfect power waveform created by the same lights with PFC ballasts on inverter generator.
As we have seen, the primary factors limiting the use of HMIs on portable generators has been their
inefficient use of power and the harmonic noise they throw back into the power stream. The power waveform below left is typical of what results
from the operation of a couple of 1200W HMIs with non power factor corrected ballasts on a conventional portable generator. The adverse effects
of the harmonic noise exhibited here, can take the form of overheating and failing equipment, efficiency losses, circuit breaker trips, excessive
current on the neutral wire, and instability of the generator voltage and frequency. For these reasons it has never been possible to operate more
than a couple of 1200W HMIs on a conventional 6500W portable gas generator. Harmonic noise of this magnitude can also damage HD digital cinema
production equipment, create ground loops, and possibly create radio frequency (RF) interference.

Our 60A Full Power Transformer/Distro provides 7500 Watts of power in a single 120v circuit from the
new Honda EU6500is Generator
The increasing use of personal computers, hard drives, and microprocessor-controlled recording equipment in production has created an unprecedented
demand for clean, reliable power on set. At the same time, the trend in set lighting is toward the use of more and more non-linear light sources that dump harmonic
noise into the power stream. Taking advantage of recent technological advances in electronic ballast design and power generation it is possible
to design a new production system that will generate clean stable set power capable of operating larger lights (HMIs up to 6kw or Quartz lights up
to 5kw), or more smaller lights, off of portable gas generators than has ever been possible before. For example, the power waveform above on the right,
is the same package of HMI lights but with power factor corrected electronic HMI and Fluorescent ballasts operating on our an
Inverter Generator. As you can see, the difference between the resulting waveforms is startling. Even though we are running the same overall load, the
fact that the ballasts are power factor corrected and the power is being generated by our an Inverter Generator, results
in virtually no power waveform distortion. For this reason, sensitive electronic production equipment will operate reliably and without damage. And, the generator is capable of operating larger, or
more smaller, lights than has ever been possible before on a portable gas generator.

Our 14 Gallon Fuel Caddy enables our modified Honda EU6500is to operate up to 20hrs without refueling
Now that we can operate bigger, or more smaller, lights on a portable generator, the last impediment to using them in motion picture production it the noise they make.
A lot of filmmakers hesitate to use a portable gas generator on their production because of the noise. Whether you pick up generator noise on your audio tracks comes down to what generator you
use and how you use it. We have specifically designed our HD Plug-n-Play Gen-set to enable you to record clean audio even under the worse case scenario (see
sample production below.) How does it do it? We start with the super quiet Honda EU6500is Inverter generator and then augment it with a custom distribution system that enables you to operate the
generator at a distance (where it won't be heard) yet still maintain full 120V line level on set.

Our inventory of enhanced 7500W Honda EU6500is generators
A common problem with portable generators, even the super quiet Honda Inverter generators, is that by the time you move them far enough off set that you don't hear them you have significant "Line Loss"
(often referred to as "Voltage Drop") from the long cable run back to set (if you use regular cable.) To the problem of line loss, you have the added problem that as you add load, the voltage drops on
portable generators (it is not uncommon for a generator to drop 5-10 volts under full load.) The combination of voltage drop on the generator and line loss on a long cable run can cause voltage to drop
to the point where HMI and Kino ballasts cut out unexpectantly or won't strike at all. Low voltage can also cause problems such as reduced efficiency and excessive heat in equipment, unnecessary additional
load on the generator, and a dramatic shift in the color temperature and in the output of lights (use this link for a
details .) For these reasons, portable gas generators are typically
operated too close to set where they are picked up on audio tracks. The trick to recording clean audio is to use a generator, like our modified Honda EU6500is, with a boost transformer, like our Full
Power Transformer/Distro, that enables you to operate the generator at a distance without suffering from voltage drop.
As noted above, the Honda EU6500is to begin with is much quieter than other portable generators and even Honda's older movie blimped Honda EX5500. Where conventional generators like the Honda EX5500 and ES6500
have to run full speed at a constant
3600 RPM to produce stable 60 hertz (cycle) electricity, a Honda EU6500is only needs to run as fast as required to meet the load demand. Since their engines do not have to run at full speed, and given the fact
that an inverter generator generates 20% more power per revolution of the engine, makes the Honda EU6500 substantially quieter than conventional models.
The net result is that it operates between 34 to 44 dBA at 50 ft. - half as loud (ten decibels) as the comparable EM7000is and ES6500 generators and comparable to full size movie blimped generators
like the Crawfords. But you can't park a Crawford right on set and record sound without picking up the generator either. With sound specs this good all you need to record sound with a Honda EU6500is without
picking up generator noise is a real distro system that will allow you to move the EU6500is off set (like you would a Crawford), minimize line loss over a long cable run, and provide plug-in pockets
conveniently close to set. That is where our Full Power Transformer/Distros comes in.
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60A Full Power Transformer/Distros
A Transformer doubling as a distro box can be used to step down the 240V output from an inverter generator to a single 120V circuit that is
capable of powering a big light like a 5k Quartz light or 4kw HMI Day Lite Par - thus eliminating the need for the diesel generator typically required to power
these lights. And, where with the right lights (pfc electronic HMI ballasts) you can utilize the full capacity of a inverter generator, a transformer/distro will enable you
to power more smaller lights off of the generator than you can without it because it provides you access to the full continuous rated power capacity of the generator in a single
circuit.

60A Full Power Transformer/Distro on location
Single Large 60A/120V Circuit
How do they do it? A transformer typically consists of two sets of coils or windings (a basic two-winding transformer is shown in the Figure below.) Each set of windings is simply an inductor. AC voltage is applied to one of the windings, called the primary winding. The other winding, called the secondary winding, is positioned in close proximity to the primary winding, but is electrically isolated from it.

The alternating current that flows through the primary winding establishes a magnetic flux, some of which links to the secondary winding and induces a voltage across it.
The magnitude of this voltage is proportional to the ratio of the number of turns on the primary winding to the number of turns on the secondary winding. This is known as
the “turns ratio.” A 240V-to-120V step-down transformer has a turns ratio of 2 to 1. To maximize flux linkage with the secondary circuit, an iron core is used to provide a low-reluctance path for the magnetic flux.

Generator Wiring Schematic
Used to step down the 240V output of a generator, a transformer will give you the full capacity of the generator in a single 120V circuit. To understand why this is, we have
only to look at the wiring schematic of a conventional AVR generator above.
As you can see from the wiring schematic, if you measure the voltage from each hot pin of the generator’s 240V 4-pin receptacle to ground it will be 120 volts, and if you measure
the voltage between the two hot pins of the 4-pin receptacle you will notice that it is 240 volts. As illustrated below, the 120 volts of the two poles adds up to 240V because the 120V circuits
are on opposing legs of a single phase circuit and 180 degrees out of phase with each other.

The voltage of opposing legs of a single phase circuit add while the current carried on the legs subtract.
Now if you feed the 240 Volt output of the generator to the primary side of a transformer, on the secondary or load side of the transformer it will be converted to 120 Volts in a single circuit that is the sum of the
two single phase legs (as illustrated below.) And, as you can see by the wiring diagram above, since the 240V output comes directly from the generator windings, by-passing the breakered branch circuits of the
generator power output panel, the transformer gives you the full capacity of the generator in a single large 120V circuit.

As we saw above, things get quite a bit more complicated with inverter generators. Unlike the simple two-pole alternator of the AVR generator in the wiring schematic above, an inverter generator uses a core that consists of multiple stator coils and
multiple rotor magnets. Each full rotation of the engine produces more than 300 three phase ac sine waves at frequencies up to 20 kHz, which is considerably more electrical
energy per engine revolution than produced in conventional two pole AVR generators. A fixed diode bridge rectifier then converts the more than 300 three phase ac sine waves
to a DC voltage (about 200 V). Single phase AC Output is then generated from the high voltage DC by a inverter module with voltage and frequency set by micro-processor
controlled switches using a PWM control logic.

ILLUSTRATION COURTESY OF KIRK KLEINSCHMIDT
The three phases of the inverter generator process: high frequency AC converted to DC; DC inverted to stable clean 120V, 60 Hz AC.
Because of the addition of the inverter unit, there is not a direct circuit to the alternator windings as there is in the AVR
generator depicted above (not that we could use the high frequency 3-phase power anyway), but the principle is the same. A transformer will step-down the 240V output of an Inverter, just as well as that of a two pole alternator, the wiring
just gets a little more complicated on the generator side. If the generator is one of our modified Honda EU6500is, a 240V-to-120V step-down transformer will convert the
enhanced 7500W/240V output to a 60A/120V circuit capable of powering larger lights, or more smaller
lights, than has ever been possible before on a portable generator.
Now that you have access to the full power of the generator in one circuit, you can load the generator more fully. Without a transformer you can never fully utilize the available power of a portable generator because the load of a light has to go on one circuit/leg of the generator or the other. For example, when plugging lights into the power outlet panel of a Honda EU6500is Inverter Generator, you reach a point where you can't power an additional 1kw light because there is not 8.4 amps available on either one of the factory installed 20A outlets/leg of the generator. With a Transformer/Distro you can still add that 1kw light because the Transformer/Distro not only accesses power through a higher rated circuit (the 30A/240V Twistlock), but it also splits the load evenly over the two legs (4.2A/leg) of the generator on that circuit.
A Honda EU6500is & our 60A Full Power Transformer/Distro powering PFC 2.5 & 1.2 HMI Pars, PFC 800w
Joker HMI, Kino Flo Flat Head 80, 2 ParaBeam 400s, and a ParaBeam 200
And, because the Transformer/Distro perfectly balances the load of what ever you plug into it, the
generator is capable of handling the larger load more easily because it is perfectly balanced.
Simplifies Electrical Distribution
The best part about using a Transformer/Distro is that it splits the load of what
ever you plug into it automatically. The iMonitor display on the EU6500igenerator control panel makes it especially easy to load our modified Honda EU6500is inverter
generator to the max. Simply plug in lights. When the load wattage displayed on the iMonitor reaches 7500 Watts you are fully utilizing the power capacity of the generator.

An overload alarm on the iMonitor display will
tell you if you inadvertently overload the Transformer/Distro. You no longer have to carefully balance the load over the generator's two 20A/120 circuits/legs as you
plug in lights because the Transfomer/Distro does it for you automatically. Now that you are able to fully utilize the generator's
available power, you are able to power larger lights, or more smaller lights, than you could without a Transformer.

Night exterior scene lit with HD P&P Pkg.
For example, our modified Honda EU6500is Inverter Generator with our 60A Full Power Transformer/Distro is capable of powering a 2.5kw Par along with 1200, 800, &
400 Pars with PFC ballasts, plus a couple of Parabeam 400s and Parabeam 200s. Given the light
sensitivity of HD Camcorders, this can constitute a complete location lighting package for a low budget HD
Digital Cinema production.
Cushions the Impact of Large HMI & Tungsten Heads
Another advantage to our system is that our 60A Full Power Transformer/Distro cushions the sudden impact of switching on large Tungsten lights (like 5ks) or striking large
HMIs. This feature is particularly beneficial with older 2.5-4KW HMIs with 120V magnetic ballasts becuase they draw more current during the initial striking phase of the electrical arc and then
“settle down” and require less power to maintain the arc (by contrast, an electronic ballasts “ramps up” its’ current draw gradually during the striking phase until
it “tops off.”) The problem operating older 2.5-4KW 120V magnetic HMI ballasts on portable generators is that the high front end load of the strike creates a sudden impact on
the generator for which the AVR (Automatic Voltage Regulator) cannot adjust in a timely fashion and the output voltage dips. Before the AVR control can compensate, the light shuts off before
it is fully up to color temperature. Not only does your light not stay on, but shutting off before it comes fully up to color temperature, the metals in the bulb fuse inside the globe -
damaging the bulb.
Because our Transformer/Distro automatically splits the load of whatever you plug into it evenly over the two legs of the 240V circuit of the generator, it reduces the impact
on the generator of sudden large loads. Split into two smaller perfectly balanced loads by our Transformer/Distro, the high front end striking load of older 120V magnetic ballasts, or
the sudden load of switching on a large tungsten light like a 5k, has a less severe impact on the generators Automatic Voltage Regulator. In combination with the voltage boost
we design into our Full Power Transformer distro (see below for details), this feature of transformers assures that output voltage will not dip too low under large loads.

Night exterior Two Shot lit with HD P&P Pkg.
Compatible with Standard Film Distribution Equipment
Configured with the industry standard 60A Bates outlet, our Transformer/Distro not only enables you to get more useable power
out of the generator, but it also greatly facilitates the distribution of power on your set. The 60A
Bates outlet on our Transformer/Distro will enable you to power a 5kw Quartz, 2.5kw HMI Par, or even a Power Factor Corrected 4kw HMI Par.

Distro System consisting of 60A Full Power Transformer/Distro, 2-60A GPC (Bates) Splitters, 2-60A Woodhead Box.
Even though the generator is 100' away to reduce noise, plug-in points remain conveniently close to set.
With the addition of 60A Bates
extension cables, 60-to-60 Splitters, and fused 60A GPC-to-Edison Breakouts (snack boxes), our 60A Transformer/Distro enables you to run power
around your set - breaking out to 20A Edison outlets at convenient points. The best part is that no matter where in the distribution system you plug in, the
Transformer/Distro automatically balances the additional load, so that you don't have to. If you are using our modified Honda EU6500is generator, you simply plug in lights
until the load wattage displayed on the iMonitor of the generator control panel reaches 7500Watts. An overload alarm on the iMonitor display will tell you if
you inadvertently overload the 60A Transformer/Distro.

60A GPC (Bates) Splitters and Woodhead Box

60A Woodhead Box running Power to Light PFC 800W ballast (left) and PFC 1200W ballast (right.)
Line-Loss Compensation
A common problem with portable generators, even the super quiet Honda Inverter generators, is that by the time you move them far enough off set that you don’t hear them you have significant “Line Loss”
(often referred to as “Voltage Drop”) from the long cable run (if you use regular cable) back to set. Low voltage on set can cause problems such as reduced efficiency and excessive heat in equipment,
unnecessary additional load on the generator, and a dramatic shift in the color temperature and in the output of lights.

For example, the effect of line loss on tungsten lights can be dramatic because their output falls off geometrically as the voltage decreases. For example a 1k lamp operating at 90% rated voltage (108V) produces about 68% of its normal light output - your 1kw lamp is now a 650W lamp. But, that is not all, as the light intensity decreases, so does the Kelvin color temperature of the emitted light. In the case of
fluorescents, HMIs, and LEDs, because their power supplies are typically of a “constant power” type, they will draw more current as the line voltage decreases in order to maintain constant power to the lamp. In the case of generator output, voltage loss translates into an exponential loss in power. That is because, if you double the ampere load on the cable, the voltage drop also doubles, but the power loss increases fourfold. What this means is that when a distribution system has a large voltage drop, the performance of the generator (its maximum effective load) is reduced. For these reasons it is worthwhile understanding the dynamics of line loss and how to mitigate it.
Line Loss
Line Loss is the erosion of voltage over a long distance caused by the resistance of electrical cables. The severity of line loss increases with the amount of current carried by a particular conductor,
so you can anticipate a significant line loss any time there is a fairly long run of cable and the cable is loaded near it maximum ampacity rating. The three major variables that affect the amount of
line loss are length, wire thickness, and amperage load. Here is why:
1) The resistance of a conductor increases directly with its length. The longer the run, the greater the line loss.
2) The resistance of a conductor decreases in proportion to its cross-sectional area. The larger the conductor the less line loss.
3) Voltage drop varies with the load. The larger the amperage load, the larger the line loss.
How much is too much line loss? Or, put another way, what is an "Allowable Voltage Drop?” According to the National Electrical Code (NEC), the amount of voltage drop that still allows acceptable
performance from equipment operating on it, and does not cause harm to the equipment, is the definition of “Allowable Voltage Drop.” As to what that figure is, lets look to the specific section of the NEC that covers line loss.
The NEC does not regulate allowable voltage drop specifically, but in a fine print note (FPN) in Section 215.2(A)(3), the code reads:
FPN No.2: Conductors for feeder as defined in Article 100, sized to prevent a voltage drop exceeding 3 percent at the farthest outlet of power, heating and lighting loads, or combinations of such loads, and where the maximum total voltage drop on both feeders and branch circuits to the farthest outlet does not exceed 5 percent, will provide reasonable efficiency of operation.
In Lay Men’s terms, what this note says is that if a voltage drop in a distribution system does not exceed 5%, the voltage will provide “reasonable efficiency of operation.” At 120V line level, this translates to a voltage drop of no more than 6 Volts, or the voltage should not drop below 114V from line loss. How likely is it that we will encounter unacceptable line loss operating lights on a portable gas generator? Very!
Let’s take as a practical example the use of a non-Power Factor Corrected (PFC) Arri 1200 Electronic Ballast on a portable generator to light the deep background of a night scene. So that we do not
pick up generator noise on our audio tracks, we will likely have to move the generator, even the super quiet Honda Inverter generators, around the corner of a building or operate it out of our grip
truck. In order to do so will require running, let’s say 200’ of cable from the generator to where the camera is on set. However, it is likely that we will have to run another 100’ of cable from
the camera position to the light if it is lighting the deep background of our shot. What kind of line loss can we then expect over a 300’ cable run and will it be acceptable?
To calculate voltage drop (Vd) you would use the following equation:

According to this equation we need to know the following factors in order to calculate the voltage drop (Vd) our non-PFC 1200W electronic ballast will cause over a 300’ cable run:
Cm: The cross-sectional area of a wire measured in circular mils (cmil). For the sake of this discussion let’s assume we are running regular Hardware Store style 14/3 extension cables which have a cross-sectional area of 4107 cmils.
L: The length of the wire in feet. This is the one-way distance from the source to load. Note that in the equation, this number is multiplied by 2 to get the two-way distance the current has
to flow to complete the circuit. In our example we would then enter 300’.
I: The current carried by the cable. According to the manufacturer’s website, the non-PFC Arri 1200W electronic ballast
has an Apparent Power of 2290VA which means that it will draw roughly 19 amps at 120V (2290VA /120V = 19.08A.)
K: The specific resistance of the material making up the conductor. Since we are using copper cable, K would be 10.8 at 25 degrees C.
As you can see, the math is getting pretty complicated. Since there are Line Loss Calculators for this kind of thing available online (at
www.stealth316.com/2-wire-resistance.htm), let’s use one of those instead. If we enter the parameters for our example into the calculator (at the bottom) we get the results in the table below, or a line loss of nearly 1
5 Volts (14.781) when powering a non-PFC 1200W electronic ballast on 300’ of 14 Awg cable. Where the allowable voltage drop according to the NEC is 6V at 120V line level, our drop is more than double the allowable amount. If we look at the effect of this voltage drop on the ballast, we see why it is not allowable by the NEC.

Since the non-PFC Arri 1200 Electronic Ballast we are using is a “constant Power” electronic ballast it will draw more current to compensate for the drop in voltage to maintain the ballast’s Apparent Power of 2290VA. At 105V it will then draw 21.81A amps (2290VA/105V = 21.81A.) Since the Arri Ballast has an operating range from 90-125V, it is not likely that the ballast will shut off from under voltage, but it is very likely that the 20A breaker providing over current protection to the generator’s Edison U-Ground receptacles will trip and shut the light off.
What can we do? We can move the generator 100’ closer to set. Even though we now pick it up faintly in our audio tracks, we have reduced our cable run to 200’ overall. If we now enter 200’ for our
cable run in the calculator we get the results in the table below, or a line loss of nearly 10 Volts (9.7869) when powering a non-PFC 1200W electronic ballast on 200’ of 14 Awg cable.

Operating at 110V, the non-PFC 1200W electronic ballast will now draw roughly 20.82 Amps (2290VA /110V = 20.82A) to compensate for the drop in voltage in order to maintain the ballast’s Apparent Power of
2290VA. While the breaker may not now trip, you can be certain that the cable and plug ends which are rated for only 15 Amps will start to heat up at nearly 21 Amps of load. While still not in the range of what the NEC considers an allowable voltage drop, it may be tolerable.
Are we in the clear? Not quite. The resistance of copper is not the only cause of line loss. Heat that occurs when a connection is weak or loose, when cable is frayed, when a connector is only partially
inserted, or when a connector or conductor is loaded beyond its capacity also can cause line loss. Whenever you push a circuit to its' maximum capacity, its' weak links will be exposed in the form of heat.
Heat increases resistance, and therefore line loss, and heat also further degrades the cable insulation which causes further line loss.
In this case, it has been my experience that, more often than not, the plug-ends of the multiple stingers running power to the ballast over-heat because they are carrying in excess of 20 Amps when they are only rated for
15 Amps. The increased resistance that results from the heat causes the line voltage to the ballast to drop further and so it has to draw more current to maintain its’ 2290VA Apparent Power. If say the voltage drops an additional 5 Volts (to 105V) because of loose or overheated connectors, a non-PFC 1200W electronic ballast will again draw 21.81A Amps and the 20A breaker providing over current protection to the generator’s Edison U-Ground receptacles will trip and shut the light off.
Let’s say, for the sake of argument, that we are operating our 1200W HMI on a Honda EU3000is which doesn’t provide over current protection to its’ Edison U-Ground receptacles. Are we in the clear? Still
not yet. As you may recall from our discussion above, one of the adverse effects that the Harmonics generated by non-PFC electronic ballasts can have on a distribution system, is “skin effect.” As we saw above, harmonic frequencies are always higher than the 60Hz fundamental frequency. Where THD is high, the higher frequencies create a phenomenon, known as “skin effect”, where the higher frequency causes the electrons to flow toward the outer sides of a conductor. Since the flow of the electrons is no longer evenly distributed across the cross sectional diameter of the conductor, more electrons are flowing through less copper and the resistance of the conductor increases. The increase in resistance reduces the ability of the conductor to carry current (its as if we were using a smaller wire), resulting in greater voltage drop over shorter distances
and overheating of the conductor.
Skin Effect

The area of the cross sectional diameter of a conductor used by DC current (left), Low Frequency AC Current (center), High Frequency AC Currents (right).
Even if voltage drop as a result of skin effect, is slight, there is one final factor working against us. To the problem of cable line loss, over heating plug ends, and skin effect, you also have the
added problem that as you add load on portable generators their voltage output drops. As the table below suggests, it is not uncommon for a generator to drop 5-10 volts under full load.

TABLE COURTESY OF KIRK KLEINSCHMIDT
The 1200W ballast that last drew 21.81 Amps at 105 Volts will now draw 23.79 Amps at 95 Volts from the combined effect of skin effect and load on the generator. If our light continues to operate, what is the practical affect of this line loss? One adverse affect is that we have diminished the capacithy of our
generator. The overall voltage drop of 25V causes our ballast to draw 4 more Amps than it would otherwise. That is a considerable loss in the capacity of our generator when you consider that a Kino Flo
Parabeam 400 only draws 2 Amps. If we are able to eliminate the voltage drop in our example we would be able to operate two more Kino Parabeam 400s on our generator - that would be an appreciable increase in
production capability.
Diminished generator capacity is not the only adverse affect to voltage drop. Since there is no 20A fuse to provide over current protection on the Honda EU3000is, we now have a potentially hazardous situation. Since it has an operating range from 90-125V, the ballast may still not shut off from under voltage. Now drawing nearly 24 Amps through a receptacle rated for only 15 Amps and on extension cords only rated for 15 Amps, the excessive load of the light will likely melt the receptacle or a plug end; or worse, start a fire.
How did we find ourselves in this hazardous situation? To summarize, by the time you move a portable generator far enough off set that you don’t hear it you have significant voltage drop from the long
cable run back to set that can cause problems - especially with lights like non-Power Factor Corrected (PFC) 1200W HMIs that operate at the threshold of a 20A circuit to begin with. If from line loss
from a long cable run, increased resistance from an overheated plug-end or skin effect, or voltage drop because of a large load on the generator, the draw of the
1200W ballast will climb well over 20 Amps. Anyone with first hand experience operating “Flicker Free” 1200W HMIs on portable generators will not find the results of these calculations surprising, since
they have probably suffered their consequences without knowing why. Since, we routinely need to load cables to near their maximum ampacity and run them out a couple hundred feet, how can we avoid these problems.
Some portable AVR generators permit you to mitigate line loss by increasing the voltage at the power source (inverter generators do not.) While a 5% adjustment of the generator’s output is usually
possible by increasing the field strength of the alternator, I do not recommend this approach to mitigating the adverse effects of line loss. Increasing the
voltage at the source has two potential hazards. Equipment being powered at the upstream end of the cable run (such as a battery charger plugged directly into the generator’s power output panel will be
over voltage (the battery charger is toast.) Second, because voltage drop is proportional to amperage load, if the amperage load is reduced suddenly, any remaining equipment will be over voltage. For
example, if a big light is suddenly turned off, the voltage jumps up and the remaining load is over voltage (the sound cart is toast.) Increasing the voltage at the source (the generator) does nothing
to solve the problem of voltage drop: it merely leaves you with a workable voltage after the voltage drop occurs. The generator is still having to work a great deal harder to power the load because the
exponential power loss still occurs. This results in a loss of efficiency, greater fuel consumption (in the case of the generator), and a reduction of the maximum power available from the generator.
The only way to truly reduce these effects is to reduce resistance by adding copper (step up to a larger cable), and/or use a boost transformer to boost voltage at the end of the cable run. In our HD
Plug & Play Gen-set we do both.

2010 BET Hip Hop Awards “Director of the Year” Nahala Johnson, aka "Mr. Boomtown", directing his latest Rap Video: an outdoor dance party with DJ and dancers on top of a speaker stack (upper left.)
So that you can record sync sound without picking up any generator noise, our HD Plug & Play Gen-set is designed so that you can run 200-300 ft of cable between the generator and our Full Power
Transformer/Distro and still have full line level (120V) on set. How does our system eliminate the drop in voltage from line-loss that you get using standard electrical cords? By using a larger gauge
cable to carry a smaller load, our system greatly reduces the voltage drop from line loss. And to compensate for what inevitable voltage drop will still occur from a long cable run, as well as the
voltage drop on the generator from a heavy load, we also build into our Full Power Transformer/Distros a voltage boost capacity. By assuring that you will have full line level (120V) on set, our
system permits the generator to be further away, where you won’t pick it up in your audio tracks, while your plug-in points remain conveniently close to set. It eliminates time consuming multiple
cable runs to the generator and the hazards of voltage drop to distribution equipment, lights, and other production equipment no matter where it is plugged in.

Our modified Honda EU6500is supplies power to set (far left.) Our 60A Full Power Transformer/Distro compensates for line-loss of 300’ cable run (left center) to assure 120V line level to 4K HMI (far right), Speaker Stack Amplifiers, Set Monitors, Battery Chargers, & DIT station (Center.) 60A Bates Splitters, Extensions, and Gang boxes distribute power from Transformer around set (right center.)
To demonstrate how our system works, let’s take the same example of a non-PFC 1200W HMI operating on a portable generator 300’ away. So that we do not pick up generator noise on our audio tracks, we run
200’ of heavy gauge 250V 10/3 Twist-lock feeder cable from the generator to our Full Power Transformer/Distro on set. From the Transformer/Distro, we run another 100’ of 120V 6/3 Bates extension cable from the camera position to the light. What kind of line loss can we now expect over our 300’ cable run and will it be acceptable?
Let’s calculate the line loss on the first leg of our cable run first. Since, the Transformer/Distro automatically splits the load of what ever is plugged into it evenly over the single phase circuit
of its primary side, we are now running 9.5 amps on each cable conductor instead of the 19A we ran before. And, we are running our smaller load on a larger conductor (10 Awg cable instead the 14 Awg cable
before.) If we enter these new parameters for our example into the line loss calculator we get the results in the table below, or a line loss of only 1.93 Volts when powering a 1200W HMI on 200’ of 10 Awg
cable. And, the 30A/250V Twist-Lock plugs of our heavier feeder cable won’t overheat under the smaller 9.5 A load. Unlike the 15 Amp U-Ground Edison plugs we used before, our 30A/250V Twist-Lock plugs won't cause a hot spot, won’t add resistance, and won’t cause additional voltage drop that will cause the
ballast to draw more power and trip the breaker.

Where this is the line loss on just one of the two 10 Awg conductors of the 240V circuit, is this our effective voltage drop? Yes and no. No, in the sense that it is only the line loss on each conductor
of a single phase circuit feeding the primary side of our step down transformer. The voltage drop we experience in a practical sense is what
we get on the secondary side of the transformer where we would plug in our light. To calculate that, we simply divide the 236.14V being fed to the transformer after losing 1.93V to line loss on each of
its two conductors (240V - [2 x 1.93V] = 236.14V) by 2 (the 2:1 step-down ratio of the transformer.) What we get is a voltage output of 118.07V on the transformer secondary, or an effective voltage drop
of 1.93V. So, yes, 1.93V is our effective line loss thus far.
What accounts for the appreciably less line loss? If we go back to the three major variables that affect the amount of line loss covered at the outset - cable length, wire thickness, and amperage
load - we see that the line loss is appreciably less in this case because 1) the resistance of a conductor decreases in proportion to its cross-sectional area (we are now using a larger conductor), and 2)
voltage drop varies with the load. The smaller the amperage load, the smaller the line loss (we have cut the load on each conductor in half by using a transformer to step-down from 240V to 120V.)

To the 1.93 Volt drop from our 200’ 10/3 Twist-Lock feeder cable run, we need to add the line loss we will have on the 100’ run of 120V 6/3 Bates extension cable. If we enter these new parameters
for our example into the line loss calculator we get the results in the table above, or a line loss of only .76 Volts when powering a 1200W HMI on 100’ of 6 Awg cable. The total line loss under our
system then comes to only 2.7 Volts (2.69V), which is well within the 5% acceptable voltage drop mandated by the NEC, and 589% less than what we experienced running 300 ft of Hardware Store style
14/3 extension cords.
To compensate for this inevitable slight line loss, and the voltage drop we can expect on the generator from running it near full load, our Full Power Transformer/Distros offer a voltage boost capacity to assure full line level (120V) on set.

Left: "Select" Upgrade, Center: 60A Full Power Transformer/Distro fully tricked-out w/ "Select" Upgrade & Edison Break-out Box, Right: Edison Break-out Box
Our standard Transformer/Distro is designed to boost the voltage on the load side (secondary) of the transformer by 5 percent. For instance, if you were to plug the Transformer/Distro directly into a genertor running with no load
and feed the supply side (primary) of the transformer with the generator's 240V output, you will get 126 Volts out on the secondary side where you would plug in lights. We have designed this slight boost
into our standard Transformer/Distro to
compensate for the slight line loss that is unavoidable over a long cable run, and the voltage drop on the generator under load.
For instance, if we fed our standard Transformer/Distro the 236.14 volts we would have 200' away from a generator operating the 1200W non-PFC HMI in our example above (240V from the generator – 3.86V
line loss to cable – 5V drop on generator from the load), 121.47 volts would come out on the secondary side where you plug in (115.57V Output of a straight 2:1 step-down ratio + 5.90V boost
of 5% boost to primary voltage after step-down.) This example shows how the slight boost we build into our standard Transformer/Distros, not only enables you to place the generator further from set
where you won't hear it, but also assures that the supply voltage on the secondary side of the transformer does not drop too low. By comparison, without the line-loss compensation of our
Transformer/Distros, to avoid the severe voltage drop in our example above you had to keep the generator close to set where it was heard on the audio tracks.

"Select" Models allow you to adjust for line-loss to maintain 120V on set
Our "Select" model of Transformer/Distros, enables you to adjust the amount of voltage boost in two 5% steps. This enables
you to maintain full line level (120Vs) regardless if the supply voltage has dropped to 228V, or even 216V, from line loss and load running on the generator. To find the optimum switch setting, our
"Select" Transformer/Distros have a built-in volt meter that tells you if the line level is too low or too high.

A good example of how our Transformer/Distro makes it possible to record clean audio tracks even under the worst of conditions is the indie short "Toothbrush." In this story of mistaken identity produced by
Guymanly Productions, a pivotal scene takes place in the middle of a near vacant parking lot of an all night convenience store. With no building or other sound barrier within a reasonable distance to block the
sound of the generator, Gaffer Aaron MacLaughlin had no recourse but to put it behind their grip truck as far from set as possible. As you can see from the photos below, he ran 300' of twist-lock extension cable
from the generator to our Transformer/Distro hidden behind a newspaper box. From the Transformer/Distro he then ran 200' of 6/3 Bates Extension to set where he broke out to 20A Edison receptacles using a 60A
snack box. While running the generator near full capacity with a lighting package that consisted of three 1200W HMI Pars and two 1k Baby Quartz Fresnels, he experienced no appreciable voltage drop on set even
after a 500' cable run because our Select Transformer/Distro was able to compensate for both the line loss of the cable and voltage drop of the generator under near full load.

Left: Scene in parking lot. Center: Transformer/Distro hidden behind newspaper box (set 200' in distance.) Right: Generator baffled by truck (Transformer/Distro
300' in distance.)
This example shows how the variable boost of our Select Transformer/Distros, not only enables you to place the generator further from set where you won't hear it, but also assures that the supply voltage
on the secondary side of the transformer does not drop too low. By comparison, had Aaron run 500' of standard 14 Awg electrical cord he would have experienced a line loss alone of 24.5V (according to the line loss
table below.) With that severe a voltage drop, his HMI ballasts would probably have cut out from low voltage as he added additional loads on the generator. Without the line-loss compensation
of our Transformer/Distros, he would have had to move the generator closer to set where it would be picked up on the audio tracks.

Now that your distro system won’t cause unnecessary voltage drop, eliminating line loss all together just becomes a matter of good set practices. Always bear in mind that Resistance, heat, and line loss
also occur when a connection is weak or loose, when cable is frayed, when a connector is only partially inserted, or when a connector or conductor is loaded beyond its capacity. Also, bear in mind that
circular coils of current carrying cable create impedance, resulting in line loss and increased heating. Good set practices, such as checking for good contact between connectors, locking connectors
tightly, taping connectors where necessary, avoiding circular coils, and replacing overheating parts, will finally rid you of the annoyance of inexplicable line loss and failing equipment.
Since, maintaining full line level will assure that lights will draw their minimum load, distribution equipment will not overheat, and that the generator will deliver its’ full power, it is well worth
following these good set practices.
It also assures that lights, like the new Arri 1800W Baby Max, that operate at the threshold of a 20A circuiit will operate reliably (more details below.)
Enables the Reliable Operation of the Arri 1800W Baby Max on Portable Generators
Another benefit to our 60A Full Power Transformer/Distro is that it will enable you to reliably operate the new 1800W Arri Baby Max on portable generators. The problem with operating the 1800W Baby Max
on generators is that, like non-Power Factor Corrected 1200W ballasts, it also operates at the threshold of a 20A circuit. Even with Power Factor Correction circuitry built into it, the ballast of the
new 1800W Baby Max has an Apparent Power of 2250VA which means that it will draw 18.75 amps at 120V. Basically the same load as the non-Power Factor Corrected 1200W ballast in our example above,
the load of the new 1800W Baby Max is also too close to the threshold of 20 circuits to operate reliably. As we saw above, if there is any line loss from a long cable run, increased resistance from an overheated plug-end, or voltage drop because of a large load on
the generator, the draw of the Arri 1800W ballast will climb over 20 Amps and trip a breaker.


1800w Baby Max
This is one of the big differences between Tungsten lights and HMIs that is important to appreciate. With a drop in voltage the current drawn by a Tungsten light goes down, but goes up with HMIs. The reason for this is because, as discussed above, HMI ballasts use bridge rectifiers and capacitors to first convert AC to DC, and then use IGBTs to convert the DC to an alternating square wave.
(ILLUSTRATION COURTESY OF HARRY BOX)

Step 1: Rectifier Bridge converts AC power to rectified sine wave. Step 2: capacitors flatten the rectified sine wave to DC. Step 3: micro processor switching
alternates polarity of DC creating an AC square wave.
If you recall, the diode-capacitor section of HMI ballasts (as illustrated above) convert the AC input power to DC power by first feeding the AC input through a bridge rectifier, which inverts the negative half of the AC sine wave and makes it positive. The rectified current then passes into conditioning capacitors that remove the 60 Hz rise and fall and flattens out the voltage - making it DC. The DC is then fed from these capacitors to the power module where the IGBTs switch it into an alternating square wave.

Thin Black Trace: Rectifier Bridge converts AC power to rectified sine wave. Thick Black Trace: Stored Capacitor Voltage. Red Trace: Current drawn by capacitors once input voltage is greater than voltage stored in the capacitor (thick black trace.)
As shown in the illustration above, the diode-capacitor circuit only draws current during the peaks of the supply voltage waveform as it charges the conditioning capacitor to the peak of the line voltage. After 90 degrees, the half cycle from the bridge drops below the capacitor voltage; which back biases the bridge, inhibiting further current flow into the capacitor. Since the capacitors have only a short interval to receive their full charge, they draw current in large pulses (which explains the higher Apparent Power of HMIs.)

Given how the diode-capacitor circuits of HMI ballasts operate, the effect of voltage drop is to decrease the interval in which the capacitors have to charge. If we compare (in the illustration above) one half cycle of a rectified sine wave at full line level (115V) to one half cycle of a rectified sine wave at 100 Volts, we see that the period during which the capacitors must recharge is appreciably shortened. Given a shorter interval to charge, the capacitors draw current in even higher amplitude bursts. The diode-capacitor circuit therefore works harder, drawing more current during an even briefer charging period, increasing its’ Apparent Power or load. To find out how much the Apparent Power increases, one only needs to consult the electrical specifications on the ballast.

The Electrical Specifications for the Arri EB1200/1800 Ballasts
If you look at these specifications (pictured above) you see that it is marked that it will draw 19A of current ("I") at 130 Volts ("U"). This works out to be 2470VA (19A x 130V = 2470VA) on the high end. And, if the Voltage drops to 90Volts, the current drawn by the ballast climbs up to 25A for an Apparent Power of 2250VA (25A x 90V = 2250VA) on the low end. Now that the ballast draws current in progressively larger bursts of shorter duration to maintain it’s approximate Apparent Power, protective circuit breakers may trip or fuses blow.

A Honda EX5500 AVR Generator powering two Arri M18 Heads with 150’ Stinger run.
To illustrate this feature of the Arri EB1200/1800 ballast, I ran 150’ of stingers from a Honda EX5500 to power two Arri M18 heads. Then using a stinger pigtail with the outer jacket removed, I put a True RMS Amp probe on the “Hot” conductor. As you can see from the photos attached here, the voltage at the ballast dropped from 115V to 102.9V (from a combination of Line Loss on the cable and load on the generator) and the current climbed to 21.51A.

After a 12V drop from Line Loss and VD from generator load, an Arri M18 drew 21.51A at 102.9V
Arri is guilty of a bit of hyperbole when they claim the Baby Max is “the brightest light that you can plug into the wall.” Lately, they have been footnoting that claim as
follows: ““Into the wall” denotes a single, 20A 120VAC electrical outlet on a single circuit.” They make that disclaimer because the Arri 1800W Baby Max was designed to
operate on a real film distribution system where you bring the 20A receptacle to the light, rather than an extension cord to the receptacle. When you can run a 60A Bates extension
and drop a Snack Box next to the ballast you won’t have a problem with voltage drop. But, if your style of shooting requires that you run multiple stingers to plug into the
generator outlet, you will likely have problems with the plug-ends or the generator receptacle overheating and causing the breaker to overheat and trip.

Our warehouse and some of our 20 M18 systems
The more reliable way to power a 1800W Baby Max on a portable gas generator is from it’s 240V circuit through a 240v-to-120v step down transformer, like our 60A
Transformer/Distro. As discussed previously, our transformer will convert the 240V output of a generator into a single large 120V circuit that is more than capable of
powering the 18.75A load of a 1800W Baby Max. In addition, the heavy-gauge feeder cable we use between the generator and transformer, eliminates the appreciable voltage drop you would have using
standard electrical cords. While, the slight voltage boost we have designed into our Transformer/Distros assures that the supply voltage on set will not drop below 120V and cause the 1800W ballast to
draw more than 18.75 Amps. Finally, our 60A Transformer/Distro is compatible with standard film distribution equipment so that you can use 60A Whips and 60A Snack Boxes to run power to the light (breaking out to 20A Edison pockets next to the ballast), rather than having to run multiple stingers from the ballast back to the generator.
By eliminating the line loss from long cable runs, increased resistance from overheated plug ends, and voltage drop from large loads on the generator, our 60A
Transformer/Distro assures that the Arri 1800W Baby Max will operate reliably on portable generators. When you consider that the Arri 1800W Baby Max has the output of a
2.5kw Par, but the light quality of a Fresnel, being able to operate it reliably on a generator is a big benefit to using our 60A Transformer/Distro (use this link for
more details on the photometrics of the Arri 1800W Baby Max.)

Our Transformer/Distro also enables you to run 1800W Arri Baby Maxs on “house power” from common 240v household outlets as well. Just like it does with a generator, a transformer will step down the 240V power of common high voltage household outlets to a single 120V circuit capable of powering multiple 1800W Baby Maxs. By giving you access to more “house power” through common 240V household outlets, a transformer also enables you to run a real distro system without the need for a dangerous tie-in or expensive tow generator. The ability to run multiple 1800W Baby Maxs off of common 240V house receptacles, or the 240V receptacle of portable generators, is one of the best reasons that I can think of to use transformers on set.
Electrical Hazard Protection
Portable generators are quite often used to provide power in situations where it is not possible to get a large tow plant. Since, many of these situations also include working in, on, and around water (to provide power on boats, beaches, and around remote lakes and streams) we have designed our HD Plug & Play Pkg. Gen-set to meet OSHA requirements (most portable generators do not) and operate safely in wet environments.
The danger of water is that it greatly reduces the resistance between you and ground. In wet grass, moist soil, standing water, or a swimming pool, water is a conductor. Salt water (which is essentially what the human body is made of) is a better conductor than fresh water. Neither is a very good conductor, but both can still pose a threat to life if a Ground Fault exists. To get a shock a person must become part of a closed circuit.
When working in rain (real or manufactured) everything and everyone tends to get wet, and wet hands, gloves, and feet pose little resistance should you come into contact with a Fault. A similar hazard exists any time the ground is thoroughly wet. In fact, water is a better conductor when it is mixed with mineral of soil. A muddy field is more conductive than a freshwater pool.
To protect people from electrical hazard in wet locations certain precautions must be taken. Light fixtures must be properly grounded and GFCI protection should be used on all circuits that are in proximity to water.
The requirement to ground portable generators, and the effectiveness of GFCIs used in connection with them, have been debated in the industry.
Some technicians believe that, like larger studio units, portable gas generators do not require grounding and that GFCIs will function regardless of the grounding arrangement. What fuels the debate is a general ignorance that there are two distinct types of portable generators – those with Floating Neutrals and those with Bonded Neutrals. Which type of generator you are using determines whether it should be earth grounded with a ground electrode and what grounding arrangement is required to make GFCIs operational.
To understand what it means to properly ground requires a basic understanding of the principles of electricity and electrical distribution, and of the parlance of the electrical trade. For example, the word “ground” is used in four totally different ways by electricians.
1) Equipment Grounding: The U-shaped prong on an Edison plug is for the equipment grounding wire. Grounding wires are not meant to carry current under normal circumstances. They carry current only when there is a Fault inside a piece of equipment causing the metal housing to become electrified.
2) Grounded Neutral: The neutral wire is sometimes called a “grounded neutral.” The reason for this will become clear in a moment. Grounded neutral wires are not to be confused with grounding wires.
3) System Grounding: The neutral buss of an electrical service is grounded to the earth by use of a grounding electrode (ground rod) sunk into the earth. The grounding electrode conductor is the wire that makes this connection.
4) Ground Fault: The unintentional grounding that occurs when a live conductor accidentally comes into contact with a metal surface. This type of ground fault is usually arcing and is extremely destructive. When a ground fault occurs in a grounded system the safety device (fuse or circuit breaker) will activate which opens the circuit and current will not continue to flow
Since the nature of electricity is not easy to grasp, analogies can be helpful in understanding the basic concepts in their simplest form.
Current, Voltage, Resistance
To understand the characteristics of electricity - Current, Voltage, Resistance - it helps to compare it to water. Like water, electricity flows. This flow is called current, measured by amperes. Like water pumped up a hill, it will always flow back to its’ source. That is, electricity always travels in a circuit or a loop. When the circuit is broken, so is the flow of electricity. Like water pressure, electricity requires power to push it through a circuit. The power needed to push the flow of electricity through the circuit is voltage. Electricity encounters friction in the form of electrical resistance, measured by ohms. Like plumbing, the bigger the diameter of the electrical pipe (wire), the smaller the resistance. The smaller the diameter of the electrical pipe (wire), the higher the resistance. The higher the resistance, the bigger the pressure or voltage needed to push the same current the same distance.
Like water, when electrical current is given alternate paths to travel, most, but not all, of the current will follow the path of least resistance.
The plumbing of electrical circuits, are conductors. Electricity flows through the conductor with the least resistance. Most metals have low resistance to electricity and make excellent conductors. Water also conducts electricity. Human bodies, made of 90% water, are good conductors, especially when the skin is wet, and so can under certain circumstances become part of an electrical circuit.
Circuits
Electrical current travels from a power source (such as a generator), passes through a load (such as a light), and returns to the power source to complete a circuit. If there is not a complete circuit - a switch is open or an "Air Gap" exists from a missing link or connection - current does not flow anywhere in the circuit. The part of the circuit going out from the power source to the load is called the Hot or “positive” side.

The part of the circuit returning from the load to the power source is called the Neutral or “negative” side. Ideally, the current going out form the power source (Hot) should be equal to the current returning (Neutral.) For obvious reasons, it is preferable that current travels only through electrical wire or other suitable conductors, not people.
Grounding
In a grounded electrical system, the Neutral is intentionally connected to ground, making the ground an alternate part of the electrical circuit. The grounded circuit can therefore be completed by electricity going either from the source to the load (through the positive side) and back to the power source (through the negative side) or from the source through the positive side to ground (negative side) and back to the power source. The “Ground” can be either an equipment grounding conductor that connects all the non-current metal parts of the system, or in its’ absence, the earth.
Faults
An electrical fault can be compared to a leak in a water pipe. A fault occurs when current partially leaks out of the intended path or circuit, using another path to return to the power source. As a result the current flow at the hot side is not the same as the current flow at the neutral side. Almost all electrical equipment leaks some current, this includes stingers, lights, feeder cables, and ballasts. Even dust that has settled inside a light housing can be a conductor and cause a current leak. If the leak is large enough it can cause a Fault. Common causes of Faults are frayed or nicked electrical cords, deteriorated insulation in lights and ballasts, or moisture.
There are two types of Faults:
1) Current leaking directly from hot to neutral – When the current leak is severe enough that there is no effective resistance, it produces a short circuit. In such a case, circuit breakers or fuses in the circuit will trip or blow, de-energizing the circuit.
2) Current leaking to ground – This is called a Ground Fault. In a grounded system the current leak completes the circuit by going back to the generator’s winding through the ground (either an equipment grounding conductor or the earth.)
Ground Faults can be deadly. In the absence of an effective equipment grounding conductor, electrocution can occur when a worker holds a faulty piece of equipment that is energized by a current leak and the current returns
to its’ source using the individual and the earth as a conductor to complete the circuit.

A prime example is an aluminum ladder contacting an overhead power line – the fault returns the current to its source using the ladder, the worker, and the ground as its’ conductor to complete the circuit.
In a true ungrounded or “Floating Ground” system, the circuit is isolated from the earth. For this reason, if a Fault occurs and there is another path back to its source (the equipment ground), the current has no tendency to
go to earth ground to complete the circuit, unless the system becomes grounded by having more than one fault in the circuit (a double fault situation.)
Grounding falls into two categories: Systems Grounding and Equipment Grounding.
Systems Grounding – is accomplished by attaching one current carrying conductor of an electrical system to ground at the source of power, this is called the neutral or common leg. The ground can be the earth or in the case of portable generators, the frame of the generator which will serve as a large conducting body that serves in place of the earth.
Equipment Grounding – is accomplished by attaching all of the non-current carrying metal parts of a system together and connecting them to the same systems ground as the neutral at the source of power (a Bonded Neutral system). The equipment ground is a safety loop that works in conjunction with the over-current protection to protect people against shock from a faulty piece of equipment that has developed a short (contact with housing.) If no grounding wire were connected anyone who touched the fixture, would (as illustrated above) offer current an alternate path for it to complete the circuit by traveling through their body and the ground, back to its’ souce. The individual making contact with energized housing would receive a shock.
With a grounding wire connected to the housing, electricity seeks the path of least resistance, and the bulk of electricity completes the path to ground through the grounding wire instead. If the neutral wire of the circuit is also bonded to the generator
frame (a Bonded Neutral system), when a Fault occurs, the grounding wire provides a path for the fault current back to the neutral bus. Normally this causes an over-current situation, which trips the breaker and removes the Fault from the circuit.

One way to think of equipment grounding is that it is the intentional connecting of all metal parts of a system together through a ground wire so that all exposed conducting surfaces have the same potential. That way if someone touches any two metal surfaces they will not receive a shock because they will not experience any difference in potential
The other intentionally grounded conductor of the system is the neutral or common conductor. This is a circuit conductor, not an equipment ground, and it is grounded to keep it at the some potential as earth, or ground. It should be grounded at the source and nowhere else.
Portable Generator Types:
There are two types of portable gas generators. In one the neutral circuit is not bonded to the frame of the generator or to the earth ground lead. Rubber mounts are used to
isolate the generator winding from the frame and the equipment grounding conductors. As a result, there is no specific hot leg and
neutral leg wiring arrangement for the generator winding connection to the receptacle. As a consequence, both legs on the receptacle
are potentially hot legs. For this reason generators that do
not bond the neutral circuit to the frame are commonly called “Floating Neutral” generators. The Floating Neutral configuration is common for applications such as connection to a recreational
vehicle and connection to home power where the transfer switch does not switch out the neutral to ground connection. When used as a stand-alone power source (a “Separately Derived System” in
NEC parlance), OSHA requires the frame of Floating Neutral generators to be bonded to earth ground for reasons we will explore shortly. This involves putting a rod 8’ into the earth
and attaching a ground cable from the rod to the generator frame.

The other type of portable generator is more akin to a Crawford Studio Generator in that it has the Neutral bonded to the frame of the generator (as illustrated above) and so is called a "Bonded Neutral" generator.
Since Bonded Neutral generators offer a high degree of protection against ground faults (if there was a fault to the frame, the generator’s circuit breaker would trip eliminating the fault)
whether they require an earth ground is up to the AHJ (Authority Having Jurisdiction.) The AHJ, depending on where the work is taking place, may be the local city electrical inspector, the
fire marshal, or the studio’s safety officer. The AHJ is the ultimate authority for what practices will be allowed on set.
Bonded Neutral Generators:
It might seem odd to bond the equipment grounding wires to the neutral, because the neutral carries current. It might seem like this would make the entire equipment grounding system live. It does quite the opposite. Let’s look at why this is.
When a source of electrical power is completely isolated from system or earth ground (not to be confused with equipment ground in this case), the only fixed quantity is the voltage potential created between the wires coming out of the alternator of the generator. The voltage potential from any
part of the circuit to ground is not defined. With no reference to ground, it is as if the phases are floating. To use an analogy: it is like a ship floating on a gentle sea – even though the
ship rises and falls with the swells of the ocean, the relationship of the keel (a phase leg) to the deck (the neutral) doesn’t change. In such an arrangement, we know the phase potential is 120V higher, but we don’t
really know higher than what? Like the ship, the relation to the ground is floating (called a Floating Ground arrangement), changing slightly as the waves gently ungulate up and down. And, just like a ship navigating the open sea, this arrangement (an
isolated power source) can function just fine, as long as nothing comes along to make a connection to earth ground.
“Generators mounted on trucks or trailers shall be completely insulated from earth by means of rubber tires, rubber mats around metal stairways and rubber mats under any type of lift gate or jacking device. Metal supports for trailers shall be insulated by means of wooden blocks. Safety tow chains shall be secured so as to not touch the ground. If complete insulation is not possible, a grounding electrode system shall be installed per the National Electrical Code, Article 250.52.”
In fact, it is the preferred set up for power that is distributed from a generator according to the guidelines (see excert from safety bulletin #23 above) established by the Safety Committee of the
Contract Service Administration Trust Fund (CSATF), an industry wide administrative body (governed by the collective bargaining agreement by and between the Producers, The International Alliance of
Theatrical Stage Employees ("I.A.T.S.E."), the Moving Picture Technicians Artists and Allied Crafts of the United States, its Territories, and Canada ("M.P.T.A.A.C."); as well as the collective
bargaining agreements by and between the Producers and the Basic Crafts Locals (Article 18)).

But as specified in the OSHA Guidelines for Grounding of Portable Generators (above), isolating the generator from ground is only permissible when the equipment grounding system, consisitng
of the non-current carrying metal parts of
equipment and the equipment grounding conductor terminals of the receptacles, is bonded to the generator frame and the Neutral conductor is also bonded to the frame as illustrated above (use this link for the
complete guidelines). If the generator is
mounted on a vehicle, the frame of the generator must also be bonded to the frame of the vehicle.
When this is the case, the figure below, illustrates how a Floating Ground arrangement offers protection against ground faults.

1) A fault in a metal fixture energizes the entire housing as soon as the circuit is turned on.
2) Since, electricity seeks the path of least resistance back to its’ source, the bulk of the
fault current will travel through the equipment grounding wire, instead of the individual making contact
with the housing, because it is of a much lower resistance than the individual.
3) Because the ground wire and the neutral wire are bonded at the generator bus with a grounding
jumper, the current carried by the ground wire back to the generator bus creates a dead short
(over-current situation).
4) If enough current flows through the ground wire, the fuse or circuit breaker pops in response.
Even with their ground floating, Bonded Neutral generators offer a high degree of protection. With the generator winding connected to the equipment grounding conductor, a low resistance path is established to carry fault current back to the generator winding to create an over-current situation and trip the breaker. Since, electricity seeks the path of least resistance back to its’ source, the bulk of the fault current will travel through the grounding wire, instead of the individual making contact with the housing.
While a Floating Ground configuration of a Bonded Neutral generator offers a high degree of protection against ground faults in equipment, it is less than ideal. For instance, if someone were to touch a grounded part of the equipment housing while making good
contact to ground (while holding a metal railing), then they could receive a slight shock equal to the difference in potential between the arbitrary floating power source and ground.
For this reason, the AHJ (Authority Having Jurisdiction) may none-the-less require the system be grounded by attaching the neutral bus of the generator to earth ground via a grounding
electrode (ground rod.) Connecting a
grounding electrode to the neutral bus of a power source gives the source a relation to ground – it establishes zero-potential between neutral and ground. The phase and neutral wires are
not just 120V from one another, the phase is now 120V above ground. It is like draining the ocean, with the boat resting on the bottom the relationship between the keel and deck are fixed
relative to the ground. With the difference in potential between the arbitrary floating power source and ground eliminated there is no potential difference between the lamp housing and hand
railing to cause a shock. No appreciable current needs to flow through the grounding electrode conductor to establish this relationship, but once it is established, all equipment connected
to the power source has the same zero-potential relation to ground - the system is grounded.
Whether a generator may be run as an isolated system without grounding electrode, or may be required to be grounded via a grounding electrode, depends ultimately on the AHJ (Authority Having
Jurisdiction).
Floating Neutral Generators:
There is no question that a generator system with a Floating Neutral requires grounding with a grounding electrode. As we saw above, OSHA guidelines for the grounding of portable
generators does not allow for isolating the generator from ground when the Neutral conductor is not bonded to the frame along with the equipment
grounding conductors. The reason being, that when the Neutral is not bonded to the
equipment grounding system, over-current breakers offer no protection in the event of a double ground fault and GFCIs will not operate reliably. To understand why this is the case, it helps to understand
first why technicians are not endangered by electrocution from current going to ground if there is only one fault in the system.
In a Floating Neutral system, technicians are not endangered by electrocution from current going to ground
as long as there is only one fault in the system. Since the ground wire and the neutral wire are not bonded at the generator bus, the equipmet grounding wire does not offer a path for the
fault current to complete the circuit back to the generator windings. In effect an open circuit, current will not travel it and so the fault current does not even go to ground. The figure below, illustrates why that is the case.

1) A fault in a metal fixture energizes the entire housing as soon as the circuit is turned on.
2) Since the ground wire and the neutral wire are not bonded at the generator bus, and
the generator is not grounded to earth by an grounding electrode, the equipmet grounding wire
does not offer a path for the fault current to complete the circuit back to the generator windings.
Therefore, the fault current does not go to the equipment ground wire
3) If the generator frame is completely insulated from the ground (a Floating Ground),
an individual making contact with the energized housing does not present an alternate path
for fault current back to the generator windings. An open circuit, the fault current does not go
through the individual and ground back to its source.
But, in the event of a double ground fault - one on the Hot, and a second in the Neutral - a path (circuit) can be created for fault
current to return to the generator windings through an individual making contact with the energized housing and through the ground if the generator frame becomes grounded
(either through moisture or contact with the ground.) Since the equipmet ground wire is not bonded to
the generator windings, it does not offer in the event of a double fault an alternate path of lower resistance. Where the individual/ground route is now the path of least resistance,
the fault current travels through the individual and the ground back to the generator windings through the second fault - delivering a shock to the individual. If either
of the faults is high resistance, the current will not be high enough to open the breaker, and the individual will receive a sustained shock that can be potentially fatal. The
Figure below illustrates why an individual receives a shock when there are two faults.

1) Current goes out on the hot (black conductor) to the light housing fault.
2) Even though current travels on the ground wire (if it is in good condition), current also
travels through the worker's body into the earth back to the generator windings, because there
is no clear return path because of the un-bonded condition.
3) Current enters the generator frame and goes back to the generator winding through the second Fault
on the Neutral side. If either of the faults is high resistance, the current will not be high enough to
open the breaker. However, the currrent will be high enough if the equipment grounding conductor is faulty (the grounding
pin is broken or there is a bad connection) to give the individual touching the housing a shock.
4) The generator’s circuit breaker may trip in response, but only if enough current flows through the
second fault to create an over-current situation.
5) The worker, however, is exposed to electrical shock until the breaker operates because no GFCI is present.
The inherent risk in using Floating Neutral generators lies in the fact that the neutral of the generator winding is neither grounded to the generator frame nor
to the grounding pin of the receptacle. This deficiency makes operation of the protective device (breaker or fuse) unreliable because in a two Fault situation, fault current has no definite
path as it does in a Bonded Neutral generator. For example, a fault current that, under these circumstances, is too low to trip a breaker or blow a fuse will also travel through an
individual making contact with the energized housing and deliver a potentially life threatening shock.

To isolate a portable generator from earth requires insulation between all metal points and the ground.
Since all equipment leaks some current, it is not uncommon to have two Faults in a system. A defect in the generator, a poorly insulated or defective extension cord, defective insulation
in a lamp housing, or defective plug, can all produce Faults - to name just a few causes. And, since it is difficult to completely insulate a portable generator from ground (wet ground, rain, or even
high humidity can cause a generator to be inadvertantly grounded) the risks of shock greatly increases (see the study by The Construction Safety Association of Ontario (CSAO) below). Floating Neutral
generators are deceptive because they give the appearance of a safely grounded system when, in fact, they are not. Their receptacles accept a plug with a grounding pin, but in
the receptacle the grounding pin is connected only to the generator frame and not to the generator winding (neutral). The user is given a false sense of security.
How dangerous are shocks?
Most people think that high voltage causes fatal shocks, this is not necessarily so. The amount of current flowing through the body determines the effect of a shock. A mili-ampere (1 mA) is 1/1000th of an amp; a current of 1 mA through the body is just barely perceptible. Up to 8 mA causes mild to strong surprise. Current from 8 to 15 mA are unpleasant, but usually the victim is able to free himself or to “let-go” of the object that is causing the shock. Currents over 15 mA are likely to lead to “muscular freeze” which prevents the victim from letting go and often leads to death. Currents over 75 mA are almost always fatal; much depends on the individual involved; how much muscle mass, body condition and condition of the heart.

If the fault is high resistance (making only loose contact with the housing) the current will create a lot of heat, but it may not be high enough to open an over-current breaker. And, if the grounding conductor is faulty (the grounding pin broken or bad connection) the current may be high enough to cause cardiac arrest.
To protect against serious harm from electrical shock, the circuit must be monitored by a Class A GFCI (Ground Fault Circuit Interrupter). This type of device will interrupt the circuit if it detects current leakage that is greater than 6 mA. At 6 mA, almost all adults and children can let go of the source of the shock. At higher currents, people are progressively less able to overcome muscle contractions caused by the shock, and therefore less able to disconnect themselves from the fault source. A GFCI will de-energize the circuit in less time than it takes to receive a harmful amount of current.

A GFCI works by monitoring the current between the hot conductor and the neutral conductor. When it senses a very small difference in current between the two, typically three to six milliamps (0.003+/-mA - 0.006mA), it trips by opening internal current conducting contacts. It will typically perform this function in the event of either a hot-to-ground fault where current takes a path to ground other than through the neutral or in the event of a grounded neutral fault caused by the neutral and the equipment grounding conductors being electrically connected by a low resistance path between them somewhere downstream of the GFCI device. When a grounded neutral fault condition exists, the GFCI device will trip the instant current is introduced on the circuit whether or not anything is connected to the GFCI device.

Normally, the difference in current between the hot and neutral conductors is zero. The component in a GFCI device that monitors current and senses an imbalance or difference between the current flowing out on the hot conductor and the current flowing back to ground on the neutral conductor is referred to as a differential current transformer. In the event that some of the current returning to ground is passing through you instead of the neutral conductor, the transformer will sense the imbalance and open the internal contacts to stop the flow of current through the GFCI device and through you.

A GFCI will not prevent a person who is part of a ground fault circuit from receiving a shock, but it will open the circuit so quickly that the shock will be below levels which will inhibit
breathing or heart action, or the ability to “let-go” of the circuit. A GFCI will not protect against short circuits or overloads. The circuit breaker or circuit protector in the control panel, which supplies power to the circuit, provides that protection. A GFCI is not a substitute for grounding or over-current protection – it should be considered a supplemental part of the circuit.
To ground or not to ground is a complicated issue. On the one hand, if you have a Bonded Neutral system, and you can effectively isolate it from ground, there is good reason not to ground it.
It is a common misconception that circuit breakers and ground rods are there to protect you. A circuit breaker is there to prevent fire created by heat from an over-current or short-circuit
and protect the equipment. The amount of current it takes to electrocute a person is much smaller than the amount needed to trip a circuit breaker. Add the fact that a ground rod will never
pass enough fault current to trip an over current device and you realize that they are not there for personal safety. Where this is so contrary to popular belief, allow me to explain.

As the Figure of a Utility Line-men above clearly demonstrates, even though there will be current traveling on the grounding electrode, because of the high impedance of the
rod, not enough will travel on it to open a breaker. Using Ohm's law, if we calculate how much current a ground rod will fault to the source through the earth at 25 Ohm's
(the prescribed impedance of a grounding device according to the NEC) at 120 volts, we find that a ground rod will only allow for 4.8 amps to flow through it. 4.8 amps will not open any breaker save a GFCI.
An electrical shock current of one hundred milliamps (100mA or 0.1A) is a very serious shock capable of causing paralysis of the lungs and heart muscle. The smallest circuit breaker we use is 20A –
that’s about two hundred times more current than is needed to kill you. So in the final analysis, a ground round will not pass enough fault current to trip an over current device, that is the job of the grounded circuit conductor (Bonded Neutral.) As Article 250.4 (5) of the NEC explains, bonding is to provide a path for fault current:
“Article 250.4 (5) Effective Ground-Fault Current Path. Electrical equipment and wiring and other electrically conductive material likely to become energized shall be installed in a manner that creates a permanent, low-impedance circuit capable of safely carrying the maximum ground-fault current likely to be imposed on it from any point on the wiring system where a ground fault may occur to the electrical supply source. The earth shall not be used as the sole equipment grounding conductor or effective ground-fault current path.”
In short, ground rods and circuit breakers provide almost no increase in safety for people. They do not provide equal potential nor do they clear faults. Installing a rod for a generator with
bonded Neutral will only provide a path for a person to get in between the source and return. In fact, a case can be made that the installation of a ground rod decreases safety. Without the rod,
there is no potential to the earth, but as soon as you bond the system to the earth there is potential to earth. Why then does OSHA require a grounding electrode be used with Floating Neutral
Generators?
The only possible explanation is that, absent a Neutral/Ground bond (as in a Floating Neutral generator like the Honda EU6500is), a ground rod, even though it is not sufficient to activate
over-current devices, is the only means of establishing a ground fault circuit for electricity to travel back to its source – creating the imbalance required to trip a GFCI device. Without the
ground rod, the GFCI will not operate on a Floating Neutral generator for reasons that we will explore next.
Simply using a GFCI on an ungrounded Floating Neutral generator will not ensure a safe system, and can in fact be misleading. A GFCI will not operate reliably if one side of the winding is not grounded to the generator frame because fault
current has no path back to the winding to complete the circuit. Only when Neutral is bonded to ground, will current go to ground to complete the circuit when there is a current leak. In other
words, a complete circuit is required to create an imbalance and cause the GFCI to trip. GFCI test circuits can also be misleading when they are used on Floating Neutral
generators. On a Floating Neutral generator, the test button will draw power from the Hot through the toroid and back to the neutral without going through the toroid again
and the sensor will initiate the GFCI to trip. The false positive received by GFCI test circuits on ungrounded Floating Neutral generators does nothing to eliminate faulty
equipment.

Tests recently conducted by The Construction Safety Association of Ontario (CSAO) uncovered significant problems in using GFCIs on ungrounded portable generators with
Floating Neutrals.
While the CSAO conducted their tests to determine the effectiveness of GFCIs used on portable generators in typical construction scenarios, their findings are equally applicable to motion picture production applications.
The GFCIs used in the CSAO tests were of both the extension cord and receptacle type (pictured above.) A rheostat was used to simulate the current leak to ground (ground fault).
Generators connected to GFCIs were tested on wet ground, dry surfaces, and an isolated surface (the back of a pickup truck). In addition, tests covered variable grounding conditions: proper ground, ground with some resistance, no ground.
Based upon their tests, the CSAO report drew the following conclusions (the complete report is available on-line at http://www.csao.org/home.cfm):
1) In the case of ungrounded Floating Neutral generators, where the neutral is not bonded or grounded but "floating", GFCIs failed to trip even when the current leak
reached higher than acceptable levels. Without a Neutral bond, electricity did not leak to the equipment grounding conductor to trip the GFCI.
2) GFCI test buttons functioned regardless of the generator's grounding property. The buttons cannot be used to test the effectiveness of GFCIs or grounding. The test button should only be
used to test GFCIs after grounding has been established.
3) Grounding can vary from one place to another, even when both are relatively close. In one test the GFCI tripped when the generator was grounded in wet earth but failed to trip when the
generator was grounded 1OO feet away in soil that was drier and better drained.
4) Testing also proved that wet surfaces can create grounding for generators in Floating Ground arrangements.
The results of the CSAO’s test support what we determined earlier. First, that simply grounding one side of the winding of a generator without also adding
GFCI protection is inadequate. Although grounding the winding would increase the probability that the circuit breaker would trip on a ground fault, current
levels could still not be high enough for a breaker to protect personnel from a shock. A combination of grounding the generator winding and adding a GFCI is
necessary. Second, ungrounded Floating Neutral generators did not present a ground path for Fault current to travel to create an imbalance sufficient enough
to trip a GFCI when a Fault existed. GFCIs only operated reliably when the generator was earth grounded. Finally, absent a Neutral/ground bond, a ground rod
is the only means of establishing a ground fault circuit for electricity to travel back to its source – creating the imbalance required for a GFCI to trip.
For these reason OSHA requires that Floating Neutral generators be earth grounded.
Before we explore the implications of OSHA’s Guidelines for the use of portable generators in motion picture production, I would first like to highlight one other problem inherent in Floating
Neutral Generators. As illustrated in the Figure below, the accidental reversing of Ground Conductor and Neutral Conductor in an extension cord or lamp cord can lead to a potentially hazardous
condition when used on a generator with a Floating Neutral and no GFCI protection.

1. Current goes out on the hot conductor (black) to light. Note: The grounding conductor
is not co
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