| Degrees C | |||||||||
| Battery | Upper | Lower | Ave Power (W) | Min 10s Power (W) | Mismatch (pwm) | Payload (kg) | Lower Temp | Upper Temp | ESC Temp |
| 3s | 10x3.8 | 10x4.7 | 233 | 221 | 170 | 0.82 | |||
| 3s | 10x4.7 | 10x4.7 | 230 | 218 | 187 | 0.87 | |||
| 3s | 10x4.7 | 10x7 | 243 | 231 | 66 | 0.77 | |||
| 3s | 10x4.7 | 11x4.7 | 220 | 207 | 116 | 1.00 | |||
| 3s | 11x4.7 | 10x7 | 241 | 235 | 138 | 1.00 | |||
| 3s | 11x4.7 | 11x4.7 | 222 | 210 | 173 | 1.18 | |||
| 3s | 11x4.7 | 11x7 | 232 | 218 | 73 | 1.10 | |||
| 4s | 10x3.8 | 10x4.7 | 243 | 228 | 154 | 1.63 | 50 | 35 | 60 |
| 4s | 10x4.7 | 10x4.7 | 246 | 235 | 158 | 1.69 | 43 | 31 | 46 |
| 4s | 10x3.8 | 11x4.7 | 238 | 222 | 163 | 1.58 | 43 | 32 | 49 |
| 4s | 10x4.7 | 11x4.7 | 240 | 220 | 108 | 1.73 | 50 | 33 | 56 |
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See if this helps clear up some of the questions. Here's a dissertation from Don Stackhouse:
OK, so we've learned that pushers are usually a detriment unless you really
do your homework, contra rotation is not generally worth the trouble on
models, but if we're going to do it anyway, we should try to keep the
airflow into both props as clean, smooth and uniform as possible. What's
that bit someone else mentioned about different diameters due to
"slipstream contraction", and what about the need for different pitches
and/or rpm's for the two props?
A prop makes thrust by grabbing chunks of air from in front of it, and
accelerating them out behind. About half the acceleration occurs in front
of the prop, and the other half behind. The reaction to the force required
to accelerate the air's mass shows up as thrust. Because the air has to be
accelerated to make thrust, the velocity of the air behind the prop is
faster than the velocity in front of the prop.
As the velocity changes, the roughly cylindrical stream of air flowing
through the prop has to obey Bernoulli's principle. If its airspeed
increases, then the cross-sectional area (and therefore the diameter) of
the stream has to decrease in proportion to that in order for the volume of
the flow to remain constant. If this were not so, the flow through the prop
would violate the law of conservation of mass and energy, which happens to
be one of the most inflexible laws in all of Newtonian physics. Thus, the
diameter of the inflow to the prop is actually larger than the prop at some
point upstream of it, then contracts during that first half of its
acceleration until it is equal in diameter to the prop when it reaches the
prop disk. It continues to contract after it passes through the prop,
during the second half of its acceleration. This is that "slipstream
contraction" that some other posters to this thread have mentioned. This
means that a second prop, aft of the first one, that is supposed to be
working with the slipstream of the first prop, needs to be a little smaller
in diameter in order to match the boundaries of the now-contracted
slipstream.
Just how much faster (and therefore how much smaller in diameter) depends
on a number of factors. For the ratio of slipstream dynamic pressure to
free-stream dynamic pressure, Daniel E. Dommasch's "Airplane Aerodynamics"
suggests an equation, which with a little algebraic juggling gives us:
Qt = Q + [(4 * T) / (D^2 * Pi)]
where:
Qt = dynamic pressure ("ram air pressure" minus the static pressure) in the
fully developed slipstream well aft of a prop
Q is the dynamic pressure in the freestream well ahead of the prop, and
outside of the propwash
T = thrust
D = prop diameter
and of course "Pi" is 3.141592...
Dynamic pressure ("Q") is equal to one-half the air density, times the
velocity squared. If we plug that back into the formula and do some more
algebra, we get:
Vt = SQRT [V^2 + (8T / rho * D^2 * Pi)]
where:
Vt = the velocity in the fully developed freestream in feet per second
"SQRT" means you take the square root of the result of the formula inside
the [ ]
V^2 = the freestream velocity squared (velocity in feet per second)
T = thrust in pounds
rho = air density in slugs/ft^3 (.00238 at sea level standard day
conditions)
D^2 = prop diameter in feet
Other units will work as well, just make sure that you use the same system
of units throughout (no fair mixing feet in one variable with inches in
another, or metric units with English, etc.!).
Ok, now that half of you are getting glassy-eyed and most of the rest are
running for cover in a mad panic, let's clarify that terrifying blast of
algebra with a practical example:
Suppose we have a twin-engined model that weighs 1 pound, and we're
planning to modify it into a twin contra-rotating arrangement. Let's also
assume that the L/D (essentially the same as the glide ratio) at our
expected cruise speed of about 25 mph ( multiply by 22 and divide by 15 to
get 36.67 fps) is about 4:1 (I know that sounds low, but remember, typical
cruise speeds are higher than best gliding speed, and besides, this
airplane has a bunch of extra stuff hanging out in the breeze). This means
our drag is equal to the weight divided by the L/D, or 0.25 pounds. In
level flight, that is also equal to the total thrust.
Let's also assume the front prop is doing about 55% of the work (0.138
pounds of thrust) to allow for the lower efficiency of the aft prop. We'll
define the prop as having a 6" diameter (0.5 feet).
Plugging all of that data into our formula:
Vt = SQRT [36.67^2 + (8 * 0.138 / .00238 * 0.5^2 * 3.1416)]
which is equal to 43.99 feet per second, or 30 mph. That's a velocity ratio
of 1.2, or 20% more than the freestream velocity.
This means that if the aft prop is far back enough to sit in the fully
developed slipstream from the forward prop, it will need either 20% more
pitch (the preferred solution) or 20% more rpm (which opens several other
cans of worms). In addition, the slipstream contraction will be SQRT
(1/1.2), or 0.913 . That means the aft prop should be 91.3% of the diameter
of the forward prop, or just a little less than 5.5" diameter. See, that
wasn't so hard, was it?
If you plan to do this a lot, I suggest coding these formulas into your
favorite spreadsheet program, such as Excel.
I helped advise a guy recently who scratch-built a VERY giant-scale
electric model of the Voyager. As I recall, his original setup used the
same size props on both ends. It flew much better when we put a prop with
more pitch on the aft motor.
So, that's all there is to it! Just correct for slipstream effects on the
rear prop, and keep the inflow into it as clean and undisturbed as
possible. You will probably not have as much prop efficiency as a pair of
tractor props with nice clean inflow, but it shouldn't be too bad."
Those pwm mismatches are huge! Going to have bad yaw performance etc... Maybe people should be steered towards an X8 if they don't have a very specific need for compactness?
Why is there still such a big pwm mismatch with a 10x7 on the bottom?