Quote:
Originally Posted by James Critchley
Sorry Ether, I'm just not being clear. 
|
No, you were quite clear.
Quote:
|
The torque available "at the motor" and "by the motor" is the same for all wheel sizes.
|
check
Quote:
|
keeping the same top speed and low end torque requires a different gear box
|
check
Quote:
|
So the torque applied TO THE WHEEL must go through a different gearbox, and will then be a different torque.
|
check
Quote:
|
Having so designed all gearbox-wheel combinations, at stall the force at the exterior rim of any wheel will actually be the same (no losses). So the applied torque as indicated is actually F_stall * R which was used correctly.
|
If a wheel of mass M
w and moment I and radius R is sitting on the floor
and is free to accelerate, then the force F that it exerts on the floor when a torque tau is applied
is not equal to tau/R.
It is equal to tau*M
w*R / (M
w*R
2 + I). That approximately equals tau/R only if I is negligible compared to M
w*R
2.
That wasn't made clear in your post.
If four of the above wheels are on a vehicle of mass M
v which is free to accelerate, then the force F with which each wheel pushes against the floor is given by
F = tau*R*(4*M
w+M
v) / (R
2*(4*M
w+M
v)+4*I)
The above approximately equals tau/R only if I is negligible compared to R
2*(M
w+M
v/4).
...
The acceleration is given by a = 4*tau*R / (R
2*(4*M
w+M
v) + 4*I)
Letting I=K*M*R
2 this becomes:
a = 4*(tau/R) / (M
v+4*M
w*(K+1))
Compare the acceleration of two vehicles, one with wheels of mass M
w1, K= K
1, radius R
1, applied torque tau
1, and vehicle weight M
v1, and the other with wheels of mass M
w2, K= K
2, radius R
2=2*R
1, applied torque tau
2=2*tau
1, and vehicle weight M
v2. Then
a1/a2 = (M
v2+4*M
w2*(K
2+1)) / (M
v1+4*M
w1*(K
1+1))
... and R does not appear in the ratio, as you said.