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In article ,
Don W wrote: Alan Baker wrote: Don W wrote: Can someone explain to me why 300HP applied to a large rotor at ~700 RPM is enough to lift a 2000lb helicopter straight up, but the same 300HP applied to a smaller diameter propellor at ~2600 RPM can not even come close to allowing a 2000 LB airplane to climb vertically? Don W. snip So if you go from rotor moving x mass per second at y speed to a propellor moving x/2 mass per second at 2y speed, then your power goes down by half from the change in mass, but *up* by four from the change in speed. IOW, move half the mass to achieve the same force and you need to use twice the power. Does that help? Yes Alan, it does. I had just not thought of it that way. Now that you point it out, it makes perfect sense. This is what I think you said: force = d (mv)/dt = force = d (m)/dt * d(v)/dt = force = d(m)/dt * (v1-v0) In English: force is equal to mass flow rate times the difference in velocity before and after the propellor. Ek= 1/2 (mv^2) -and- Power = d(Ek)/dt = Power = d(m)/dt * (v1-v0)^2 In English: Power is the rate of change of the kinetic energy of the airflow which is equal to the mass airflow times the square of the difference in velocity before and after the propellor. Is that correct? If so, it says that for fuel efficiency you want as big a prop as you can fit turning slow. That also makes sense because the parasitic drag on the prop goes up as the square of the blade velocity as well. big grin I think something fundamental just just clicked. Don W. Looks correct to me, Don. Glad to have helped. -- Alan Baker Vancouver, British Columbia "If you raise the ceiling 4 feet, move the fireplace from that wall to that wall, you'll still only get the full stereophonic effect if you sit in the bottom of that cupboard." |
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