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The Handbook of FMA, Inc. Section 2 – Evaluating and Selecting Cells July 2005
This document is a work in progress. Latest revision:
Distributor for Kokam Lithium Polymer Cells 5716A
Evaluating and Selecting
Cells How
to determine the propulsion your airplane needs A look
at performance parameters in greater depth It
all begins with the discharge curve The
first real indicator: voltage depression Lower
temp and HDR capability = long service
life Capacity
depression mirrors voltage depression A design
example illustrates the effectiveness of the method Energy
density (specific energy) normalizes the weight of cells Understanding
the Ragone Chart The
payoff for High Discharge Rate (HDR) capability
Important definitions 1. Ohm’s law: E = IR where E = volts, I = amperes of current, and R = resistance in ohms. 2. R/C models require watts to fly. If you know the wattage required, you have a leg up. 3. Power = watts. For reference, one HP = 750 watts. 1 V X 1 amp = 1 watt. 4.
5. Amperage is determined by the voltage a cell can maintain at a given discharge rate and the resistance of the circuit. 6. An important part of the resistance of the circuit is the internal resistance of the cell. 7. The wiring, motor, and ESC add resistance to current flow. 8. We are concerned only with cell internal resistance. 9. The length of time a cell can deliver a given wattage is called watt-hours 10. 11. Ampere-hours X volts = watt-hours. 12. Discharge curves are used to display the voltage of a cell as a function of elapsed time or capacity delivered. 13. Capacity is defined as the mAh or AH a cell can deliver when depleted from full capacity to a specific cut-off voltage at increasing current draw (amps). 14. Dividing the capacity in mAh or AH that a cell can deliver at a given average current gives the run time the cell can deliver. 1.
What distinguishes one cell from another •
Life cycle cost •
Performance and reliability •
Pack weight, not cell weight
•
Pack complexity and reliability •
Vendor knowledge and service •
Backing of a major supplier
and a dealer network •
Safety 2. What should not distinguish one cell from
another •
Old - wives tales •
Unsubstantiated vendor claims;
if data isn’t available, it may not be good or he may not have it •
Anonymous claims and critiques from someone you do not know Your ultimate success and enjoyment of electric
models can be enhanced by taking the time to study and understand the
principles discussed below. If a model builder elects to try to start and
run a glow engine with no understanding of the engine or the fact that he can
ruin a new engine with one lean run or by loading it with too big a prop, then
he can well expect to ruin a perfectly good engine that may have cost him
upwards of $150.00. By the same token,
if one refuses to learn how to use Li Pos properly, then we can expect to see
people report in forums that they ran a 3S1P pack 1020 mAh cells in a Belchfire
Heli and the cells swelled after two runs.
They don’t know that that heli draws 25 amps. Same thing. 1.
Basic cell performance
is defined by internal resistance. 2. Internal resistance determines cell voltage depression. Voltage depression is directly proportional to internal resistance per Ohm’s law. E = IR Where E = voltage drop (depression) I = current flow in amps R = cell internal resistance
As an illustration: if a specific
cell has internal resistance of 3 milliohms (.003 ohms), For a 60 amp load, E = 60 X .003 = 0.18 volt. Another cell that has internal resistance of 30 milliohms would have depression of E = 60 X 0.03= 1.8 V at the same current. 3. The amount of heat that the cell must dissipate is also directly proportional to the internal resistance of the cell but is proportional to the square of current flow; i.e., P = I X I X R Where P = power dissipation in watts
For the same illustration, the low R cell has to dissipate 60 X 60 X .003 = 10.8 watts while the 30 milliohm cell has to dissipate 60X60 X .03 = 108 watts. This is significant. 4. If a dead short were placed across a cell and the voltage measured across the cell, voltage would drop per the above equation. The drop is called voltage depression. The practical measurement is to load the cell in a square wave at 1 KHz. The data is recorded as AC impedance at 1 KHz. 5. A discharge curve will be illustrated a bit later. Because voltage depresses with increasing load, the cell reaches cut-off voltage earlier as load increases, thus, reflects capacity depression proportional to voltage depression. 6. The amount of wattage a cell can deliver per unit weight is labeled specific power or power density. 7. The watt-hours a cell can deliver is labeled specific energy or energy density and defines how long a cell can sustain a load. 8. Discharge curves plot cell voltage against either time or capacity delivered. 9. Voltage Vs. time can be converted to capacity by multiplying by the time elapsed at constant current drain. (Amps X time in hours = AH) 10. Capacity can be converted to run time by dividing capacity by amps. (AH/Amps = Hours) 11. Cell temperature is driven by internal resistance as described earlier. Cell life is greatly shortened by high temperature. How to determine the propulsion
your airplane needs 1.
Determine the
wattage needed to fly the aircraft intended. The detailed aerodynamic analysis required is
not within the scope of this document. However,
if Electrocalc or Motocalc can be accessed, those programs will help.
If the designer or a review has defined the wattage required, you are
half way there. Rest assured; this is a question our service
and sales departments receive many times a day! 2.
If you have
little information, at least find the weight of the airplane, use the table
below for a ball-park figure, then refine the results later. - Indoor and micro flyers 25
w/lb - Park and backyard flyers for Speed 280 to
Speed 400 25 to 50 w/lb - Speed 400 up to brushless sport-scale
trainers 50 to
75 w/lb - Maneuverable, higher performance sport-scale
& 3D 75 to 150 w/lb - AMA/FAI pattern competition & F5A
gliders 150 to
250 w/lb 3.
The low end
of each category is flyable and sedate. 4.
The higher end
of each category is much hotter and demands skill. 5.
Within each
category, wing loading has an effect. Wing
loading is the weight divided by wing area, usually lbs per square foot.
Higher wing loading imposes higher power loading to fly properly and
pushes the requirement toward the upper end of the scale. 6.
Once the power
loading (w/lb) is known, determine what motor and ESC can deliver the needed
wattage. Both motor and ESC specs will
give a range of voltage, usually as cell count. Take care not to mistake Ni Cd cell count for
Li PO. One Li Po cell = three Ni Cd
or Ni MH cells. CAUTION: Some ESCs specify upper voltage limits and upper
amperage limits. In some cases both
may not be permitted simultaneously. Check the specifications and demand to know.
7.
Pack requirements
are by peak wattage that may be demanded only for a few seconds each flight,
while overall pack capacity sets flight time. Li Pos are almost never run at peak load for
a whole flight. If they are, the pack
is under-designed and may be damaged. 8.
A rule of thumb
for success and long life is to allow for a 30% margin. Because Li Pos are so light, this is not really
a burden. 9.
Divide peak
watts by planned nominal voltage of 3.7V X the number of cells in series,
e.g. a 3S pack is 11.1 V, nominal to determine peak amps.. 10.
If you can,
measure the amperage in a short static run using a watt - meter or an ammeter
to confirm the estimate. NOTE:
This can save you the cost of a pack and is well worth - while. 11.
The capacity
required depends on desired flight time per charge. You may elect to have a pack with a lot of
capacity and fly multiple flights per charge or use a smaller pack and recharge
between flights. 12.
The standard
most recommend with modern 4th generation cells is the “ten minute
flight”. Ten minutes is about the average
flight time for glow or electric. Most
club fields have some limit on flight time after which one must relinquish
the frequency pin. 13.
FMA/Kokam HDR
packs charged with our cell balancing chargers may be recharged in 20 minutes
and this makes the “10 minute pack” very practical. Two packs then allow almost continual flying. 14.
The capacity
required = desired flight time in hours X average current drain in amps. 15.
The capacity
for the 10-minute flight = 0.167 X average current in amps. 16.
You may enter
peak current and voltage in LI POCALC II, available in the Li Po Compendium
at www.fmadirect.com. LI POCALC II
will provide the specification for the pack you need. Then reduce throttle setting to approximate
the average current anticipated to see what flight time will be. The chart below summarizes the above step-by-step procedure.
It all begins with the discharge curve. 2. There are some things on the curve itself that can be interpreted directly: a. The amount that the average voltage drops as load is increased is called voltage depression. It is the difference in average voltage from, e.g. the red to the yellow curve to the green, etc. A better way of displaying will be described later. Most casual students of Li Pos have a sense of the importance of voltage depression. b. The “flatness” of a given curve is an indicator that pack voltage will not keep falling rapidly so that throttle adjustments are needed continually. By the same token, when voltage does drop, it is rapid and cut - off can occur abruptly. c. Capacity depression is reflected in the spread between end points at the right end as current load increases The KOK 3200 illustrated is a particularly “stiff” battery, i.e. it loses little voltage or capacity as load is increased. d. Note that casual observation of the curves above as a standalone bring little sense of how good the cell is. Comparison with other cells in its family below will illustrate the importance of being more thorough. 3. The four key data points listed form the basis for a great deal more analysis that can be done if one is interested in knowing how to do a true evaluation. The key data may be entered in the spreadsheet below for analysis.
The data
presented in this handbook are as of June 2005. Li Po performance changes almost daily and
new cells and suppliers are arriving. Careful
study of this section will permit you to incorporate and evaluate claims made.
Simple math for calculating performance The following equations are built in to the EXCEL spreadsheet to calculate performance parameters once the basic data are entered. 1.
Run time in hours = capacity
in AH/amps discharge (X 60 to get minutes). 2.
Average watts delivered =
discharge rates in amps X average volts. 3.
Watt-hours delivered = average
watts X run time in hours (X 60 for watt-minutes). 4.
Specific energy (energy density)
= watt-hours/kilogram = watt-hours/weight in kilos (multiply kilos by 1000
for grams). 5.
Power density = watts/ weight
in kilograms (multiply kilos X 1000 for grams) 6.
%-capacity delivered = capacity
measured in AH or mAh at lowest discharge rate divided by capacity at
discharge rate of interest. Note: If the manufacturers rated capacity is used,
the % may exceed 100% at the lowest discharge rate measured. For best results, use the international
standard 0.2C as the initial discharge rate. 7.
Number of cells required in
each parallel pack = maximum expected discharge rate / C - rating for the
cell of interest, e.g. a 10C, 2100 mAh cell would have to be paralleled 3
times to carry a peak load of 63 amps. 8.
# of cells in series desired = voltage permitted
by the motor and ESC of interest/ 3.7 V per cell. 9.
Total # of cells in the pack
= Eq 7 X Eq 8. 10.
Pack weight = cell weight X # of cells in the pack X 1.05
(Estimate 5% for wiring, interconnects, and heat shrink or protective covering) Note: If the cell has high voltage depression, you may want to use capacity delivered at the expected peak discharge rate instead of the manufacturer’s nominal capacity. Using EXCEL CHART WIZARD,
any of the columns may be plotted against each other as desired. Some key curves are illustrated in the sections
that follow.
The
first real indicator: voltage depression 1. From the spread - sheet: Plot cell average voltage as a function of discharge amps. 2. More depression means that the cell gets hotter as amps increase. See discussion below. 3. High voltage depression precludes achieving high discharge rate. 4. Voltage depression impacts other parameters as shown in charts below. 5. The only way to go to higher current drain is by paralleling packs. The cost of light - weight is high
internal resistance and overheating Rather
than clutter the chart of voltage depression, a separate chart shows that the
final discriminator is the temperature rise in cells. Thus, it is important to know what the
temperature curve for any cell is and that sometimes is not shown in test
data. Data from tests made in April
2005 of a number of cells in the 2AH range by a test lab in the Experience accrued as the FMA Li Po systems described earlier were developed has shown that the determinant of cell life and performance is the temperature the cells reach during discharge. A cell run continuously at the maximum C rate will lose capacity to 80% in as little as 25 cycles. Properly managed, the same cells run with bursts of < 10 sec and average current of half the maximum allowable discharge rate can last 500 cycles. 1. The impact of light - weight and high internal resistance limit cell performance severely. 2. Cycle life may be very short for light - weight and high internal resistance cells. 3. While some light - weight cells are claimed to be capable of 10 to 12C discharge rate, it is clear that they cannot be used safely above 10 amps continuous. Lower temp and HDR capability = long service life 1. The race car current profile is tougher than for airplanes. 2. That profile was recorded for a number of races. 3. Kokam is cycling cells to validate life cycle. 4. The results after 200 cycles shows 92% of capacity. 5. 80% is international standard cell life. 6. The projection is for 500 to 600 cycles. 7. Packs that run at high temperatures won’t do that. 8. Kokam packs now in use in F3A airplanes at up to 60 amps run < 125 deg F. Capacity depression mirrors voltage depression 1. Plot the data from the spread-sheet capacity Vs discharge amps to see the effects on capacity depression. Now, it is much easier to see and to compare when all are on one plot with little extraneous information. 2. Just because a cell is heavier does not mean anything by itself. 3. If a light - weight cell is loaded lightly, performance can look good. 4. Paralleling packs curtails any advantage of lighter weight. 5. Paralleling adds pack weight and cost and reduces reliability. For example, a 3S 8P pack for larger airplanes has 24 cells and 48 solder joints compared to an 8S1P pack. Reliability of such a parallel pack is, by definition, going to be 1/3 that of the 8S1P pack that can do the same job. A design example illustrates the effectiveness of the
method 1. This is the example of an 11 - Lb F3A pattern airplane such as Icepoint illustrated earlier. The method is equally applicable to any example. 2. The givens: · F3A Airplane weight can - not exceed 12 lbs, battery and all. · The usual 1.8 cubic inch glow engine produces a stated 3 HP when the pilot can get it to run and peak out reliably, so that is the target. · 3 HP = 3 X 746 watts = 2238 watts. · It is desired to produce a minimum of 2238/11 = 203 watts / Lb of airplane · Airplane weight sans the battery pack is 8.5 lbs. · The brushless motor and speed control are able to handle up to 10S = 37V nominal and up to 60 amps. NOTE: The motor manufacturer limits voltage to 10S, so that sets the upper design limit. Thus, the 12S1P design proposed could not be used to reduce current draw and extend flight time for practice. · The pack voltage was chosen to be as high as permissible to keep current consumption as low as possible. · Average current consumption was estimated at 25 amps, including short bursts of 60 amps or more during acceleration from vertical maneuvers. 3. Primary analysis: ·
· 2236 watts is the peak design point that will be demanded of the propulsion package. This is the “burst capability” that is demanded for but a few seconds periodically. · The pack is sized by the wattage demanded. · Peak amperage is 2236/37 = 60 amps. · The KOK 3200/20C can deliver up to 64 amps continuously with adequate cooling and can deliver short bursts up to 100 amps as it does in the FMA Scorpion packs for race cars. · A 10S1P pack of KOK 3200/20C meets the peak power requirement. · The KOK 3200/20C delivers 98% capacity at 29 amps, the average current draw. Thus, flight time = 3.136 AH/ 25 amps ~ = 7.5 minutes and enough to complete an efficient flight pattern. · Weight of the pack is 1.88 lb. Thus; total airplane weight is 10.4 Lbs. He savings in current by reducing all-up weight by 0.6 lbs was not estimated. It was preferred to make an empirical determination by test flying. 4. Alternatives · Three alternative pack configurations are examined in the Watts Available chart above. · The results are self - explanatory. · It takes a 2P pack of KOK 2000/15C to deliver the peak 60 amps. · It takes a 3P pack of TANIC or TP cells to meet that requirement. · The two latter cells will be operating too close to the temperature limit to have long life. · The lightest weight pack is the KOK 3200 followed by the KOK 2000/15C, the TANIC, then the TP. · Note that voltage depression, even at 20 amps, drives the 2000 mAh packs below the reference KOK 34200 line. See discussion below. 5. How to do an analysis · Find out the wattage or horsepower needed · Define the voltage planned · Determine how many packs in parallel are required to meet the peak amps · Calculate the weight and cost of the pack required · The data in this curve can be replicated for any range of cells desired, using the spread - sheet and plotting from Chart Wizard. Energy density (specific energy) normalizes the weight of cells 1.
Energy density is watt-hours/kg. 2. When voltage is depressed, so also is the W-H available. Were this not so, a cell would deliver full energy density no matter the discharge rate. 3. Using energy density as a parameter of merit, the lighter a cell for a given discharge rate, the better. However, the lighter cell is almost certain to have greater voltage depression. 4. The chart below reflects these facts but also shows the impact of technological advance to the 4th generation HDR cells. 5. The 1st generation cells introduced in 2000 such as the KOK 3270 had maximum permissible discharge rates of < 5C. As the cell approached the limit, voltage dropped precipitously and, of course, energy density plummeted too. Yet, those cells were very light. 6. By 2003, Kokam had begun to introduce a 2nd and a 3rd generation of cells. The KOK 1500 is a 2nd generation cell with 10C burst capability. That cell begins to show a bit more “stiffness” and allows burst discharge rates that did not begin to see as much depression at 10 amps but fell as 10C was approached. 7. The new 3rd and 4th generation cells, starting with the prototype KOK 340 mAh cell, took on a whole new dimension in “stiffness”. Scaled up to the KOK 2000 to 3200 mAh cells produced the curves sweeping up and to the right, which is where we want to be. 8. At some point, weight does begin to have a stronger bearing as shown by the KOK 2100/20C cell that is extremely “stiff”. The KOK 2100 is a very sturdy cell with 10 mm wide tabs and beefy construction. It is an extremely rugged cell, but it is relatively heavy. Later, it will be shown that such a cell still enjoys an advantage in overall evaluation. Understanding the Ragone Chart 1. The Ragone Chart shows relative performance of any source of power from nuclear power to batteries. 2. The data comes from the discharge curves. 3. The method permits display of relative performance of many cells on one chart. 4. The method takes weight into consideration so that basic energy density and power density rule. 5. The Ragone Chart is not too useful except to see relative performance clearly. 6. With study, the Ragone Chart can be used to design packs and calculate run time. 7.
Watt-hour / KG / 8. The lines of constant run time radiate up and to the right. 9. Below is a Ragone plot for R/C cells from 2 AH to 3.2 AH. 10. When cells are paralleled, weight goes up on both scales, but pack weight and cost go up too. 11. A light - weight cell such as the KOK 1500 exhibits excellent energy density so long as discharge current is kept low. Note that all except the KOK 4th generation HDR cells have a fairly steep slope and that the HDR cells are not as high energy density when current drain is low. This trend now permits several parallel packs to be replaced with a single pack.
The payoff for High Discharge Rate (HDR) capability 1. A pack is sized by the maximum power it can deliver. 2. The data in the chart come from manufacturers data. 3. The baseline chart below is for a 1S pack. Multiply by the # in series to get weight and cost. 4. Total watts is determined by the airplane. 5. Once you decide the voltage to use from specifications for the motor and ESC, calculate the amps from watts required (or desired) / volts. 6. When amps required is known, the chart below tells how many parallel sets of a particular cell are required. 7. Note: The KOK 3200 is the only one that handles 60 amps in 1P. 8. Estimated pack weight = # of parallel packs x weight per cell x operating volts / 3.7V per cell. Example: 1P x 85 GM per KOK 32.2 x 37V / 3.7V = 1x85x10 = 850 GM / 453 GM / lb = 1.88 lb. 9. Cost is based on average $ / GM for all suppliers and varies with time and supplier. 10. Plug in your own numbers. The weight and cost are relative. 11. LI POCALC II does the calculations for you.
After peer review, people still want a simple one-shot figure of merit! 1. The things that have the most impact are voltage depression brought about by internal resistance, and the capacity depression with increasing amperage 2. Voltage depression is represented by Delta V per amp. Look at that chart and see the relative sensitivity. The slope of the curve is change in voltage per unit change in discharge amps. 3. A simple figure of merit (FOM) = V loss / amp of discharge. 4. An example used as the baseline is the KOK 3200, the top line in the chart. Delta V is 0.00995 volt per amp so the max 64 amps creates 0.5564 volts depression. 5. At a lower performance level, the 2nd generation KOK 1500 / 10C has a Delta V of 0.04702 / amp. 6. The slope on the curve is, of course, negative and the lower the slope, the lower the number. .It is more professional to have the best item appear first, so FOM = 1 / Delta V per amp. After peer review, people still want a simple one-shot figure of merit! 7. The ranking by this FOM is Column 3, below. 8. However, some cells are lighter than others and should benefit from that “lightness”, so a modifier was developed that credits lighter weight. The lighter weight cell yields more MAH per unit weight. More MAH equates to longer flight time. 9. Note how the ranking changes as weight is normalized: The KOK 2100 / 20C loses from 93 to 69 from Col 3 to Col 4. The TP 2P 2200 gains because it is a light cell. Likewise, the KOK 2000 / 5C that was a very light 1st generation cell gains. 10. This FOM is
for individual cells. Remember that,
if you want to parallel to meet current draw, the advantage of
Once the pack is assembled, the last connection for electric-powered aircraft is to the speed control (ESC). The ESC controls the speed of a brushed or brushless motor from full - off to full-throttle. The ESC also provides what is known as BEC voltage; that is, it outputs a regulated 5 to 6V DC level to the receiver to power the receiver and servos. The primary concern regarding Li Po batteries is the ESC’s cut-off voltage. Most ESCs sense battery voltage and cut-off the motor drive when battery voltage drops to about 5.2V. Li Po cells have a nominal 3.6V operating voltage under normal load. This happens to be 3 times that of a NiCd or NiMH cell. Li Po cells must not be permitted to go below 2.5V/cell. If the pack is a 2s pack, then 2 x 2.5 = 5V, and a cut-off of 5.2V is fine. However, if the pack is 3s, a 5.2V cut-off would mean each cell would have to go to 5.2V ÷ 3 = 1.733V and the cells might not recharge. Low Voltage Cut - off or LVC is the term used to describe what happens when an ESC determines that there is no longer sufficient battery voltage to continue running the motor on an aircraft. The ESC shuts off the motor to prevent the battery from discharging to the point where it will no longer power the receiver and servos. This provides the pilot adequate time to continue controlling the aircraft until it can be safely landed. Most ESCs have a fixed cut - off point of around 5 to 5.5V. This has not created a problem for most installations using NiCd or NiMH batteries, particularly lower cell count battery packs of 6 to 8 cells. Those battery technologies are fairly forgiving in this regard. Although it really isn’t good to deep-discharge any battery, NiCd/NiMH cells usually continue to operate even after deep discharge. If lithium batteries are allowed to discharge below about 2.5V per cell under load, there is a chance they will not recharge. There are a few ESCs available with programmable cut - off points, but programming these products is often difficult and time-consuming. FMA stocks a series of electronic speed controllers (ESCs) designed specifically to operate with Li Po as well as NiCd and NiMH batteries. The first of these, the FMA Direct SUPER 30, is a 30A miniature aircraft speed controller with several unique features. First, it was designed to prevent damage to Lithium battery packs. The SUPER 30 is a radical approach to LVC. This computer-controlled ESC detects the unloaded battery pack voltage on power up. In less than 1 second, it characterizes the battery pack, determining the number of cells in the pack, and stores in memory the proper cut - off voltage for the particular battery. Then it continuously measures the battery pack voltage as you fly. When the measured pack voltage reaches the stored cut - off point, power is cut - off to the motor. The SUPER 30 also provides two motor restarts, assuming your battery pack is in good condition. Based on requests from our customers, the latest computer code for the SUPER series controllers includes a user-programmable, fixed LVC that can be set at any level within valid operating voltage parameters of the controller. This feature does not eliminate the auto-cell detect feature—it is a new option that can be selected. The unit includes a battery eliminator circuit (BEC)
which is composed of a 1A, low dropout,
5V regulator. This enables the ESC to
power the receiver without a separate receiver battery pack. At 1A, the unit can easily power from 3 to 4
standard or micro servos. In addition, several functions can be controlled by a
bank of tiny switches. For example, the
brake can be disabled for use in electric helicopters. Also, the LVC circuit can be disabled,
allowing the ESC to operate reliably with NiCd/NiMH packs with as few as 3
cells in series. Finally, the SUPER 30 includes a one-time end point
adjustment (EPA) procedure that custom tailors throttle response to a specific
transmitter. The first time you use the
SUPER 30, you will go through a simple series of steps to teach the computer
about your transmitter throttle channel.
After the procedure is complete, you move one of the switches. From then on, the custom end points are
stored in permanent memory and recalled each time you turn power on. If you change transmitters, simply return the
EPA setup switch back to ON and perform the setup again. Speed controllers under development
by FMA will allow the cut-off to be programmed at an optimum 2.8V. Most brushless controllers offer the same
capability. Most other ESCs have a 5.3 V
cut-off that will work with 2s Li A Kokam radio flight pack is a 2s1p
pack equipped with the standard RC 3-pin, polarized battery connector. The output of a fully charged 2 - cell series lithium polymer
battery is 8.4V. Currently the FMA DS
300 is the only servo on the market that can operate at this high voltage. Other servos require a voltage regulator to
reduce pack voltage to a level the receiver and servos can handle. The SPORT VRLI voltage regulator connects between the
switch harness and the receiver. It
powers the receiver and up to five standard to medium torque servos (2A
continuous current draw). The unit
includes a low dropout (0.5V) regulator which provides a constant 5V output to
the receiver/servos. Three super-bright LED voltage indicators (green, yellow
and red) help prevent deep discharge of Lithium battery packs. The VRLI continuously measures battery pack
voltage and provides a clear warning of battery condition. For example, a fully - charged battery pack
in good condition will show green. As
the pack becomes discharged, or when the pack is under load, the yellow and red
LEDs may light. When the yellow LED stays
on and the unit won’t recover to green, it’s time to recharge the battery. The SPORT VRLI is also a great tool for
identifying power problems such as an under-rated or failing battery pack or
sticky linkages. Simple, effective and necessary to protect a Li Po pack
from deep discharge, the SPORT VRLI is the perfect match for Li Po powered
on-board electronics in trainers and sport models. (The SPORT VRLI is not recommended for
aircraft installations using digital or high torque standard servos.) | ||||||||||||||||||||||