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A much better result with a b
ELECTRIC FLI
Our first article in the February 2006 issue showed the
potential of the electric Piper Cub model aircraft. This
month we continue our investigation by converting the Cub
to a brushless motor to obtain a greatly improved result.
By BOB YOUNG
I
n the last article we recounted the trials and tribulations associated with using the original Speed 400 brush
motor supplied with the Cub kit.
In passing, I mentioned the possibility of fitting a brushless motor to the Cub at a later date. This is the story of
how a duckling was transformed into a swan. (For the
politically correct, there is of course nothing wrong with
being a duckling. Ducklings are nice too.)
For those who missed the previous article, the brush
Speed 400 motor supplied with the kit caused serious
radio interference, especially with FM receivers, resulting
in greatly reduced range.
This problem was eventually overcome by replacing
the FM radio with an AM radio (see box “AM & FM?”).
Therefore there was much interest in examining the outcome regarding radio range when the brushless motor
was fitted.
In addition there were several minor flaws in the aerodynamics of the Cub as originally supplied in the kit.
These included too little down-thrust and adverse yaw
during aileron turns. Even with these drawbacks, the Cub
flew very nicely in its original form and provided several
hours of very happy test flying. (To think I get paid for
doing this...)
However it was obvious that the Cub could stand some
improvement.
Aerodynamic improvement
Altering the down-thrust angle on the motor originally
supplied would have been very difficult. Luckily the decision to fit the brushless motor solved that problem as well.
The brushless motor chosen was a small LSE outrunner.
The outrunner style motors have the windings (stator) at the
78 Silicon Chip
centre, fixed to the motor mounting flange. The bell housing
holding the magnets (rotor) surrounds the windings and
the propeller is fastened to it. Thus the rotor and propeller
spin together.
Long-term audiophiles will recognise these brushless
motors as being very similar in construction to the highquality Papst motors used in reel-to-reel tape recorders.
Outrunners deliver more torque than the brushless inrunners but do not rev as fast. It is interesting to note that
the outrunner with no gearbox drove the same size prop
at approximately the same RPM as the brush motor fitted
with a 3:1 gearbox.
Mounting the outrunner required the removal of the
original front former and the construction of a small box
to move the motor/prop forward into the correct position
for the re-fitting of the engine cowling (see photo opposite).
The outrunner mounting flange was attached to a plywood
plate that was mounted on this small box.
Thus it was a simple matter to shape the box to tilt the
plate at the correct angle for the down-thrust and right
thrust required. As it turned out, I had set a fraction too
much down-thrust and the angle had to be adjusted after
the first test flight.
With the correct down-thrust and right thrust angles,
the aircraft will fly straight on full power and continue
on flying straight when power is suddenly reduced. If the
aircraft turns right, there is not enough right thrust and if
it dives, there is not enough down-thrust. Conversely, the
model needs less right thrust if it turns left and less downthrust if it climbs after reducing power.
This is a most important part of setting up an aircraft
correctly. A well set up aircraft is much easier to fly and
places a lot less strain on a tyro R/C pilot. Learning to fly
siliconchip.com.au
brushless motor
IGHT
Part
2
an R/C model is difficult enough without the additional
complication of a badly trimmed aircraft.
The adverse yaw was cured in a relatively simple manner. A small amount of rudder movement was mixed into
the aileron channel via the mixing function in the transmitter. Thus when the ailerons are moved, a smaller but
proportional amount of movement was programmed into
the rudder.
At full aileron deflection approximately 10° of rudder is
applied. This is sufficient to overcome the adverse yaw and
now the model does well-balanced turns with no sign of
adverse yaw. A switch was inserted into the mixer to switch
the coupled aileron/rudder (CAR) mixing on or off.
It is a good idea to switch the CAR off during take-offs
and landings, as the CAR will induce a heading change
each time the ailerons are moved to level the wings during the landing approach. This makes accurate landing
approaches more difficult and that is not a good thing
when learning.
The pilot that can land the aircraft well and from even the
most difficult of situations or emergencies will be rewarded
with models that live a long time. This is why I practise
landings and take-offs at every opportunity. Forget the loops
and rolls. They are easy. The landing is the manoeuvre that
separates the boy pilots from the men.
Electronic improvements
The difference in the electronic performance of the model
with the brushless motor was staggering. I expected an
improvement but not as much as was obtained.
First of all, the radio interference completely disappeared
and we could return to the original FM receivers without
the range problems previously encountered.
siliconchip.com.au
June 2006 79
Secondly, the performance of the
model was greatly improved. Where
take-offs were marginal even on tar
with the original Speed 400, take-offs
are now so brisk that short, tufted grass
is no longer a problem for the take-off
area. The model will also climb more
briskly and on a fully-charged battery,
loop from level flight.
This is a staggering improvement
from a motor that is smaller, lighter
and runs much cooler than the Speed
400.
In addition, the speed controller
supplied with the brushless motor
has some very natty features although
these had to be found the hard way
as the original instruction sheet was
a piece of paper approximately 75 x
25mm covered in Chinese or Korean
writing!
The first of these features is a programmable voltage cut-off to allow for
the use of two or 3-cell LiPO batteries.
As discussed in the first article, LiPO
batteries are very fussy to work with.
They need to be handled with great
care in both charging and discharging.
The point about discharging LiPOs is
that from about 2.7V per cell downward, irreversible chemical changes
begin to occur in the cells and by the
time the cell voltage falls to 2.4V or
lower, the cell is permanently damaged.
It is very difficult to obtain agreement on a definite voltage at which the
cell is destroyed, with figures quoted
from 2.7V down to 2.4V. However
what is almost universally agreed
upon is that speed controllers should
contain a voltage cut-off circuit that
will cut off power to the motor at a
minimum of 3V per cell.
The LSE electronic speed controller
(ESC) used in the Cub is fitted with a
lead ending in a 2-pin header plug.
If a micro-shunt is fitted to this plug,
the cut-off voltage is set for two LiPO
cells. If the shunt is removed, the ESC
is configured for 3-cell operation. The
nominal voltage of a LiPO cell is 3.7V
per cell, giving a total of 7.4V and
11.1V for two and 3-cell packs. Be
very careful with this because if you
run a 3-cell pack on a 2-cell cut-off,
terrible things are going to happen to
that 3-cell pack.
While we are on this point, it is
mandatory that LiPO batteries be unplugged from the model at the end of
each flying session. There is no ON/
OFF switch in this type of ESC, thus
there will be a small current drain on
the battery, eventually leading to cell
voltages falling below 3V and thereby
damaging or destroying the batteries
if the battery is left plugged into the
model for an extended time.
For the same reason, do not leave
LiPO cells lying around for extended
periods without recharging, as selfdischarge will eventually destroy the
battery, Voltage cut-off circuits will not
protect against the last two scenarios,
so make sure each battery pack is
recharged at least once every three
months to be on the safe side.
The second feature of the ESC is a
self-arming/calibration routine. The
ESC will not operate until the throttle is moved to low throttle and the
transmitter turned on. At this point
the ESC is armed and will now operate the motor via the throttle channel.
Another interesting point here is that
the ESC will set the low throttle point
when the transmitter is switched
on. It is also possible to program in
a dynamic brake during the switchon routine. The dynamic brake will
prevent the prop from wind-milling
in gliding flight.
Electric models can be a dangerous
to work around as the motor can start
suddenly when least expected and
low throttle arming is a great safety
feature. Having a model leap off a
bench, or worse still, inflict a nasty
cut from a prop is no fun. So be very
careful at all times when working with
electric-powered models, especially
with high-powered models!
Unplug the motor battery whenever possible, keep the transmitter
off as much as possible and if it must
be on, put it somewhere where the
throttle lever cannot be accidentally
bumped to high. The motor will not
start accidentally with the transmitter
switched off.
The scope grabs tell the story . . .
This first ’scope grab shows the output of the FM detector
on the bottom (magenta) trace, the supply rail is on the
middle (cyan) trace while the active lead on the motor is
shown on the top (yellow) trace. All ’scope grabs use the
same order for the traces. This grab was obtained with the
Speed 400 motor stopped.
80 Silicon Chip
The motor signal with the Speed 400 motor running. Note
the spikes on the supply rail. However, have a look at the
receiver detector trace. It has been obliterated and this was
with a moderately strong signal from the transmitter. Three
brands of FM receivers were tried and all gave much the
same result.
siliconchip.com.au
One of the things that I cannot get
used to with electric models is the lack
of a definite throttle-stop as I prefer to
land with the motor set at an idle of
approximately 1000 RPM. In IC motors the throttle barrel is pulled hard
against a mechanical stop so that the
idle RPM is constant at all times. In an
electric model the idle point will vary
a little with battery voltage, making
landing approaches less predictable.
If the throttle trim is pulled too far
back, then the motor stops completely
then restarts if the throttle is advanced.
All this takes some getting used too
after years of flying IC engines.
I also miss the noise and have been
toying with the idea of sticking a bit of
cardboard into the prop like we used to
do when we were kids on pushbikes.
Either that or perhaps I will fit an onboard tape recorder with speakers and
recorded motor sounds. The sight of a
Piper Cub roaring off the runway with
absolutely no sound is a little unnerving for those who cut their R/C teeth on
IC motors. Still I do appreciate being
able to go to a local cleared area and
not disturb the neighbours.
Another nice feature with the ESC
is a motor cut-off that is instantaneous
upon striking an object. The modern
brushless ESC uses back-EMF sensing
for its timing. These motors are wired
as 3-phase motors in either star or delta
configuration and therefore need to be
timed to sustain rotation. The timing
No, this isn’t the front of the motor or just a part of
the motor. It is THE motor – it’s an LSE Outrunner
and it gave a staggering improvement over the
original electric motor supplied with the
Piper Cub kit. Minor modifications
were required to fit it, though . . .
signal is derived from the motor
windings and no longer requires
extra wires for the timing signal.
If for any reason the shaft stops
rotating for even the briefest
period, the motor drive current
is cut off immediately. This is
also a great safety feature.
This type of sensing is extremely clever and calls for
a simple explanation. By summing
the two driven windings, a reference
voltage can be derived. The undriven
winding, which will have a voltage
induced into it because it is being
moved through a magnetic field, is
compared to the reference.
When a zero crossing is detected it
is time to rotate the magnetic field to
the next position. The above works
once the motor is spinning.
This shows the same order of traces but with a Silvertone
AM receiver fitted and the Speed 400 stopped. Note the
inverted detector signal and higher detector output.
The next grab (at right) shows the Speed 400 running with
the AM receiver and the same signal strength from the
transmitter.
siliconchip.com.au
However before it starts spinning
there is no zero crossing to detect so
the designer must resort to interesting
techniques such as ringing the windings to try to work out the position
of the motor so a clean start may be
performed. It is much easier to do
this if the controller knows the motor
characteristics. If they are not known,
the controller must learn them. Some
It was impossible to sync the ’scope due to noise but
the detector signal is clearly visible and at full strength.
However the audio filter must have been working its little
capacitors to the bone, filtering out the rubbish being passed
on from the detector. In spite of the noise the receiver still
had full control of the ESC at 80% of its normal range.
June 2006 81
controllers are so smart that they can
recognise brush or brushless motors
and configure themselves accordingly.
Incidentally, brushless motors may be
reversed by swapping any two of the
three motor wires.
If the ESC is disarmed after striking an object, the transmitter must be
switched off and left off for 10 seconds
or so and then turned back on, making sure that the throttle is correctly
set at the desired low throttle setting.
The most common cause of this type
of disarming is clipping the prop in a
bouncy landing.
Finally, the last feature is the low
voltage cut-off that will determine for
you when flying stops on that battery
pack. Once the pack hits 3V a cell, all
temptation to continue flying is removed. That pack is now out of bounds
until recharged. Do not be tempted to
let the pack rest and pick up a surface
charge and so continue flying. Go home
and recharge the pack.
With two 1800mAh LiPO packs and
an 8 x 6 slow-fly prop on the Cub, I
find I am gone from home for at least an
hour and a half, sometimes more. This
includes a five-minute walk each way
to the field and the rest is taken up with
non-stop take-offs and landings with
the occasional loop and roll thrown
in for good measure. I did say I bought
the Cub because it was a pretty aircraft
when taking off and landing!
How is this possible? At best, the
maths show 30 minutes flying time.
This is one of the most complex questions in aerodynamics so the following
answer is much simplified.
Take a look at Table 1. This shows
static (0km/h) current consumption
against RPM for the 8 x 6 slow-fly
prop.
The table shows a non-linear rise
in current for each 1000 RPM, with
the last 200 RPM requiring as much
current as the change from 3000 to
4000 RPM.
Why is this so? The ESC appears to
deliver a linear current with throttle
stick position, so what is happening?
The answer is found in the formula for
aerodynamic drag:
FD = 0.5 CD p A V2
The culprit is the V2 bit of the equation. As the prop speed increases the
power required follows a square law
and this is what makes selecting the
correct prop for any motor/model combination so difficult and so important.
The same applies to the model as well.
To double the flying speed requires
four times the power.
Do you want or need a Piper Cub
with a scale speed of 400km/h? Why
not opt for a Cub with a scale speed
of 140km/h and a battery life several
orders of magnitude greater?
Each branch of electric modelling
is different and the prop requirements
must be balanced for the task in hand
against the design of the model. A
slow-flying, high drag aircraft requires
a larger diameter, fine pitch prop
whereas a slick, fast-flying model
requires a smaller diameter, coarse
pitch prop. The choice of prop is one
of the most difficult parts of aircraft
Now have a look at these ’scope grabs. On the left, the
brushless motor is stopped while on the grab at right it is
running. The gain on the supply trace has been increased
tenfold to get a look at the noise on the supply rail. This
82 Silicon Chip
Table 1: static current consumption vs
RPM for the 8 x 6 slow-fly propellor.
design. Most modellers using 2-stroke
IC engines tend to over prop their motors (too large a diameter mainly) and
I suspect that electric flyers tend to
do the same.
For example, an increase of one inch
in prop diameter can increase current
consumption by 25%. However, electric flyers have a method of recognising prop efficiency in that flight times
will indicate an efficient or inefficient
prop/motor combination. Measuring
flight time in the absence of in-flight
telemetry is an important method of
determining motor/prop efficiency.
Propellers have many important
characteristics including blade shape,
blade section, pitch and diameter.
The latter two are the most easily
explained. Diameter is the length
of the prop from tip to tip and will
determine the mass flow through the
prop. The pitch is how far the prop
will pull the model in a single revolu-
is processor switching noise and is barely visible. The
FM receiver detector output is clean and stable with only
processor noise visible and the audio filter easily filters
this out.
siliconchip.com.au
tion. Broadly speaking, the prop is the
aircraft transmission and a fine pitch
gives great pulling power at low speed
whereas a coarse pitch prop will give
less pulling power.
However there is a complication in
that the faster a model flies the smaller
the effective pitch angle becomes due
to the angle that the air meets the prop
being reduced as a result of forward
motion. So once the aircraft gets moving the coarser prop becomes finer in
effective pitch; take-off being the big
problem for fixed-pitch propellers.
Full-size aircraft usually use variable pitch props or constant speed
props. Thus during take-off the pitch
is set to fine (low gear) and at high
speed the pitch is gradually increased
to keep the engine RPM constant.
Now this has important ramifications for electric flight models in that
current consumption drops as the
model gets up to flying speed. For
example a 9 x 7 Masters e-prop that
draws 11A at 5400 RPM at 0km/h
will draw only 7.5A and the revs will
increase to 6700 RPM at 60km/h. At
40km/h, the motor draws 8.5A and at
20km/h 9.5A.
Thus referring back to Table 1, at
anything less than 3,000 RPM in flight
the motor in the Cub would be drawing
fractions of an amp.
And this is precisely how the model
is flown when doing circuits and
bumps. Full power is only applied
during take-off and climb to altitude
(about 100 ft). From then on the model
is throttled back and cruises on approximately one-third throttle or less
for the rest of the circuit.
In conclusion then, where I began
flying the outrunner with the recommended 9 and 10-inch props (props
are still measured in inches) on the
Cub, I finally settled on an 8 x 6 inch
slow-fly prop, thereby reducing the
static current from 11A to 7A and thus
extending the flight time accordingly.
The aircraft also flies at a more realistic
speed – another nice touch.
REAL
VALUE
AT
$12.95
PLUS P
&
P
Radio performance
improvement
A major, staggering, improvement
was obtained upon fitting the brushless motor. It was impossible to obtain
a reliable range with an FM receiver
with the Speed 400 installed and we
had to resort to installing a Silvertone
AM receiver to obtain the desired
range.
The series of scope screen grabs tell
the story. Field-testing told the same
story. In hours of test flying there has
not been a single glitch from the FM
receiver, even with the model at extended range.
So there you have part two of the
electric flight story. I could say with
warts and all again but there were no
warts.
Was the effort and expense of the
change of motors worthwhile?
Too right!
SC
AM and FM?
For the technically-minded, scratching their heads and trying to make sense out of the
statement that the AM receiver out-performed the FM receiver in a high noise environment, fear not! The laws of physics have not been rewritten.
What the model trade refers to as FM is, in fact, Narrow Band Frequency Shift Keying
(NBFSK) and R/C-type AM is ON-OFF Keying (OOK).
NBFSK as applied to R/C equipment employs a ±1.5kHz frequency shift as against
the 70kHz frequency shift in a true FM broadcast system. The signal-to-noise ratio of
an NBFSK system when compared to an FM system is very poor.
OOK on the other hand is not AM as the data transmitted is carried in the position of
the OFF spikes (Pulse Position Modulation, PPM) and not the amplitude of the carrier.
This means that the carrier is either full ON (100%) or OFF (0%) for very brief periods –
about 350ms. The AGC time constant holds the AGC on during the 350ms OFF spikes.
Thus the receiver AGC clamps the receiver in the least sensitive state until the last
20% of the receiver range, at which point the AGC is almost useless and the receiver
is wide open to noise, as it is now at full sensitivity. This gives the OOK system a much
improved signal-to-noise ratio compared to the true AM system.
In practice, the signal-to-noise ratios of the two systems (OOK and NBFSK) are about
equal. However, in many cases the AGC provides superior protection against electric
motor and spark ignition noise than the limiters in the NBFSK receivers. This does not
always hold true but experience has shown that swapping an OOK receiver for an NBFSK
receiver will often give better results.
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