vanesch said:
Let us model this crudely. With a velocity (wrt ground) v_cart corresponds:
a force by the air on the cart: F_air = A x v_cart + B x (v_wind-v_cart)
a force on the wheels: F_wheel = - C x v_cart
Positive signs are "downwind". A, B and C are model constants. The term with A is the propeller acting as a propeller and it is driven by the speed of the cart. The term with B is the drag of the wind, and also the effect of the difference between wind velocity and propeller. The term with C is the force excerted through the gearing mechanism of the propeller (reaction from the fact that the wheels drive the propeller).
crude model
This isn't a good model of the DDWFTTW cart. The force from the prop is a function of v_wind as well as v_cart.
If A is very large compared to B and C, which means a high gearing ratio, the cart will move upwind
Except that large A doesn't mean high gearing ratio, but instead high force, such as a larger diameter. A is defined to be a force here, so it would have to be negative to create an upwind cart.
atyy said:
A>C
which I hope is equivalent to Jeff Reid's two regimes.
Sort of, this "crude model" doesn't quite describe the DDWFTTW cart as I just mentioned.
Forward force from the prop is a function of prop diameter, prop pitch, prop angular speed, and apparent wind. Prop angular speed = wheel angular speed x gear reduction factor (currently the two gear reduction ratios are 1/1 or 13/16). Prop geometric forward speed = prop angular speed x prop pitch. Actual speed of air through the prop is a function of prop geometric forward speed and apparent wind (slip ratio).
It mostly boils down to two requirements:
One requirement for a DDWFTTW cart is that the forward force from the prop + air interface is larger than the opposing backwards force from the wheel + ground interface that powers the propeller, so that the net forward force (prop force - wheel force) accelerates the cart or maintains a DDWFTTW speed against the opposing drag related forces. The other requirement is that the forward force > opposing force is achieved while the power output is less than the power input.
Since power = force times speed, the DDWFTTW cart can take advantage of the fact that apparent headwind speed is < ground headwind speed, because advancing the air through the prop at a lower speed than ground speed allows the force from the prop to be greater than the opposing force from the ground, without consuming more power than is generated by the ground + wheel interface.
It's my guess that the prop parameters aren't that critical if maximum speed isn't the goal, just any speed DDWFTTW, as long at the prop pitch and any gearing reduce the advance rate of the prop versus the wheels sufficiently. Once some miminal prop diameter is reached, the prop will generate enough force for the cart to operate. If the diameter is increased beyond the minimum, then the forward force increases due to the larger diameter, and the opposing force increases due to the increase in torque required to drive the larger diameter propeller. Generally a larger diameter prop is more efficient than a smaller diameter prop, so it's my guess again that a larger diameter prop will result in better forward force versus torque ratio (for a given prop pitch), so increasing the diameter of the prop beyond minimum will probably improve the cart's speed. There's some point of diminishing returns, but I don't know what that limit is.