I think zut did the best job pointing out that the original statement of the problem makes little sense, but if anyone’s trying to figure out details, simplifying and looking at similar cases may help.
We have either a treadmill or an infinite and movable strip, which I’ll call “the belt”. The part we want to move relative to will be “the ground”.
Since we don’t really care about lift so much as whether we can move a certain speed (or at all) relative to the ground, these may as well be carts. Simple vehicles moving in a straight line.
Consider these cases :
(A) Rocket Sled : No wheels; has some means of thrust controlled by the pilot (e.g. jet engine, tow rope, child pushing it).
(B) Auto Cart : Has wheels; moves by turning its own wheels (e.g. bicycle, car, locomotive).
© Rocket Car : Has wheels, but moves by some other force as in (A).
Think about these questions for each vehicle. Start with (A), it’s easiest. Consider how much © is like (A).
What happens if there is no friction on the belt?
Now add friction (to the belt). What happens when the belt moves at a constant, low speed (no slippage) in any direction? Why?
Imagine the vehicle is moving, applying just enough throttle to keep a constant forward speed v[sub]0[/sub].
What happens to the vehicle’s speed if the belt moves at constant speed in the opposite direction (-v[sub]0[/sub] )
-relative to the belt?
-relative to the ground?
What can the belt do to slow or stop the vehicle relative to the ground?
When you are finished, please return your blue books to the proctor. If you need to cheat, look off treis’s paper.