How does the Kv work in this rule of thumb? Such as Kv per ounce or Kv per pound?
1) commit aviation (very sedate slow flyer) you need at least 50W/lb
2) for a trainer 75W/lb
3) for sport plane 100W/lb
4) for pattern about 125W/lb
5) for full on 3D anything from 150W/lb upwards
From : Don Stackhouse
As is often the case, another simple question, with an answer that is
anything but.
First of all, that list is another one of those "rules of thumb", with all
the limitations inherent in them. In this case the numbers apply to only a
certain range of models, probably about the Speed 400 and up sizes of
outdoor models, with conventional propellers, and conventional wing
loadings and span loadings. If you get into things like sailplanes with
high efficiency, low drag and low flying speeds, you can get good
performance with less power. However, something with relatively poor
propulsive efficiency such as a ducted fan, you'd better have more power.
Likewise, something with a high wing loading (and therefore a higher than
"normal" flying speed) has a greater amount of parasite drag to deal with,
so it will need more power. OTOH, something that's designed to fly slower
will need less.
For example, the models typically cited for this rule probably operate in
the range of the high teens to the low thirties for airspeeds, and the 50
watts per pound number is appropriate in that context. However, a small
"park flier" such as our 3 ounce Curtiss-Wright "Junior" can get comparable
performance (within the context of its 10-15 mph typical cruising speed) on
only about 30 watts per pound, because the lower flying speed results in
considerably less parasite drag, and the low span loading helps the induced
drag.
Kv really addresses a different issue, the relationship between the motor
and the prop. Here it might help to draw an analogy with the common
automobile. If the motor of the model corresponds to the motor of the car,
then the prop (and anything between the prop and the motor, such as a
reduction drive) corresponds to the car's transmission, drivetrain and wheels.
The motor of the car generates mechanical energy, and the transmission,
drivetrain and wheels transfer that mechanical energy from the motor to the
road (which, through Newton's third law, the one about action and reaction,
applies an equal and opposite reaction to the car).
In an airplane, the motor generates mechanical energy, and the prop (plus
any reduction drive) transfers that mechanical energy from the motor to the
air, which (in accordance with Newton's third law) applies an equal and
opposite reaction to the airplane.
Now, the key item in both of those relationships is the ratios involved. In
the case of the car, we have a motor that is happiest when running at some
RPM when at some given power setting, and the car wants to move along the
road at some speed when at that same power setting. The drivetrain designer
has to come up with gear ratios and tire diameters for that set of
operating RPMs and operating speeds, that matches the desired RPM of the
motor to the desired speed of the car. Of course in the process the
designer also has to consider how big a patch of rubber is required between
the tires and the road to efficiently transfer the power without skidding,
and the tradeoffs between the rolling friction, the traction required, the
handling qualities, and a variety of other factors that constrain the tire
diameter and width. This then forces the decision on the ratios of the
gears in the rest of the drivetrain.
In an airplane we have constraints on the diameter and pitch required in
the prop to efficiently transfer power to the air, and the desired RPM that
results from that situation. In general this tends to be a relatively low
RPM. On the other hand we have the RPM desired by the motor, which in
general tends to be a fairly high RPM.
If we can come up with a way to reconcile these two conflicting
requirements, we can get away with a direct-drive system. Examples of this
are relatively low-powered airplanes with high Kv motors, where the power
is low enough that we can get away with a small prop that tolerates running
at a high RPM. Another example is the typical "outrunner" motor such as the
one I have in my electric 2-meter Chrysalis. The outrunners as a group tend
to have low Kv's, so they are happy when running at a relatively low RPM's,
which then allows for a large prop diameter and fairly high powers with
direct drive.
However, if we can't reconcile the needs of the motor for high RPM, with
the aerodynamic need for a large diameter prop (which therefore limits the
prop to relatively low RPM), then the solution may be to insert a reduction
drive between the prop and the motor to let each of them run at their
desired speed.
OK, that sounds great, but what about the case where we have to run at a
variety of power settings and speeds? For example, the typical
reciprocating car engine is only efficient over a relatively narrow range
of RPM's. If we have a wide range of speeds we want to drive at, wider than
the engine's range of useful RPM's, then we have to resort to a
transmission in the drivetrain that has more than one gear. If we want to
relieve the driver of the work of figuring out which gear to use for best
motor efficiency, we can even go to an automatic transmission.
The analogous situation in an airplane is the variable pitch propeller.
Changing the prop's pitch is like changing the gear ratio of the car's
transmission. If we really want to hold the motor precisely at its most
efficient RPM, and without relying on the pilot to readjust for every
little change in the airplane's speed, altitude and flight path, then we
automate the process by adding a governor, and making the prop a variable
pitch, constant speed prop. That's right, a variable pitch, constant speed
prop is the airplane equivalent of a car's automatic transmission.
Note, we only need that extra complexity if we have a wider range of
operating conditions than the motor can tolerate. In planes or cars with
only a narrow range of operating speeds, or with motors that tolerate wide
ranges of motor RPM's, we do not need the extra complexity, weight, cost,
and efficiency penalties of a variable speed transmission system. Most of
our model airplanes fall in this category, as do things like some types of
golf carts. Also, a free-turbine turboshaft engine typically has an
extremely wide range of efficient RPM's, so some of those turbine powered
cars and trucks that various companies were experimenting with back in the
60's and 70's only needed a one-speed transmission.
But I digress... Getting back to the original question, how does Kv relate
to the size or weight of the model? The short answer is, it doesn't. As is
typically the case where the relationship involves more than two variables
(a lot more than two in this case), any attempt at making a "rule of thumb"
quickly drowns itself in a veritable ocean of exceptions. However, we can
draw some general inferences:
Lower Kv (i.e.: a motor that naturally likes to run at low RPM and high
torque) increases the chances that we can successfully operate "direct
drive" needing no a gearbox between the prop and the motor.
Eliminating the reduction drive gets rid of the reduction drive's
efficiency losses, which could typically be anywhere from a 3% penalty to
15% or more, depending on the design details and the operating parameters.
However, generally a low Kv motor (such as a typical outrunner) pays a
penalty in the motor's electrical efficiency (I've heard that it's because
of increased "iron losses" in the motor, but I'll leave it to the electric
motor experts in this group to cover that issue). Which approach results in
the smallest efficiency losses depends on the individual case.
In addition, reducing the prop RPM typically allows for an increase in prop
diameter, which typically results in more prop efficiency. However, this is
not automatically true, there can indeed be such a thing as too much prop
diameter, just as there is such a thing as too many blades, or too few
blades. Once again, each individual case has to be evaluated on its own
merits.
One other thing that enters into this issue of prop efficiency is the range
of operating conditions. It's usually possible to design a prop with pretty
decent efficiency at one particular operating airspeed, altitude, RPM and
power setting. However, very few airplanes fly at only one flight
condition. Determining a basic Kv, gear ratio and set of prop parameters
becomes a far trickier problem if you have to operate efficiently at a
range of flight conditions. The prop that has extremely good efficiency at
one flight condition might be extremely "peaky", so that its performance
drops off very suddenly with even a small deviation from that design flight
condition. This is especially important for fixed pitch props.
There are references that can help find a better baseline design point.
Unfortunately these tend to be scarce as hen's teeth, and even if you have
one, you still need to know how to use it. The design of a prop, and the
matching of a prop to an airframe and engine, is one of the most complex
and difficult jobs in airplane design, but also one of the most
misunderstood and underestimated.
So, we come down to the one rule of thumb that does seem to hold up
consistently in engineering:
The design with the greatest probability of success is the one where the
designer did their homework thoroughly, and addressed all the interactions
of all the relevant details of that particular design, instead of relying
too much on oversimplified rules of thumb!
Don Stackhouse
DJ Aerotech
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