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[FONT=Verdana, sans-serif]If the propeller and air only interact in an equal and opposite manner . . .[/FONT]
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[FONT=Verdana, sans-serif]The only advantage a cart travelling at wind speed has over a cart pushed up to the same speed in still air is that it doesn't have a headwind.
Otherwise all other frictional losses are essentially the same for both carts. At wind speed the cart is effectively in still air. How does a propeller spinning in still air develop extra energy to sustain and increase the cart's speed ONLY from an equal and oposite reaction with that air? [/FONT]
It can't in principle, but the cart is special. Even allowing for that, and using Dodge69's numbers:
"Ok, I did it for 28 mph in a 10 mph wind. Again, ignoring friction.
If the cart moves at 28 mph, the propeller spins at 133.7 RPM or 2.228 rev/s. The airspeed of the cart is 18 mph, or 26.4 ft/s. And the diameter of the propeller is 16 ft. So, the advance ratio (jj) is 26.4/[(2.228)(16)] = 0.7406.
To get values for the coefficients ct and cq, I interpolated linearly between the two nearest values of jj given (0.7073 and 0.8252), and ended up with ct = 0.0834 and cq = 0.0120.
Then, the forward thrust of the propeller works out to be 61.32 lb, the torque driving the propeller is 141.2 ft-lb, and the backward force of the ground on the wheels is 48.11 lb.
That leaves 13.21 lb to overcome friction and accelerate the cart."
Air power at prop = 18mph*61.3lb = 26.4ft/s*61.3lb = 8.0m/s*272N = 2176W =2.92HP
Power at wheel = 28mph*48.11lb = 41ft/s*48.11lb = 12.5m/s*214 = 2675W =3.58HP
The wheel is somehow generating more power than the prop, but the net is 0.66HP.
Using rider and bike weights of 200lbs and 450lbs respectively, and a mechanical efficiency of 85%, the losses are 1.1HP.
It is unlikely that a cart on dirt will have less rolling losses, and certainly more drag. Spork was going to give some numbers for the pylon drag. When he does that, we can include them in the calculation.