Solving a Puzzling Motor-Wheel Problem

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The discussion revolves around the dynamics of a motorized wheel attached to a pole and the resulting motion when torque is applied. The user grapples with understanding the direction of movement of the pole's top in relation to the wheel's clockwise rotation. They analyze the torque exerted by the motor and the corresponding effects on both the pole and the wheel, concluding that the pole will move to the right while falling counter-clockwise if certain conditions are met. The user also questions how to determine if the wheel will turn when the pole is shorter than the wheel's radius, highlighting concerns about the motor potentially spinning without moving the wheel. The conversation emphasizes the complexities of torque, inertia, and the relationship between the components in motion.
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Homework Statement


A motor with wheel is attached to the end of a pole. The device is initially vertical and at rest when the motor is switch on and supplies torque τ to the axle. As the wheel begins to roll clockwise, does the top of the pole moves to the left or to the right?

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The Attempt at a Solution


I am confused by this problem, because as the motor exert the torque to the wheel, doesn't the wheel exert the same torque to the motor? So if I take off the wheel and look at only the free body diagram of the rod&motor, then torque acting on it would be counter-clockwise, so the rod would move to the left. But the wheel is turning clockwise, so it should be moving to the right also (?).

How should I consider the problem?

- Thanks
 
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The motor is attached to the pole. So shouldn't the pole reflect the rotational motion of the motor in producing the torque. (That action/reaction thing?)
 
So the pole will fall to the left with respect to the axle, while the axle will be translating to the right?
 
That's what it looks like to me.
 
To calculate the translation acceleration at the axle, I would related the clockwise τ to α by

α = τ/I ... (1)

Then if the wheel rolls without slipping, then a = r α. In (1), what I should I be using? Is it just the moment of inertia of the wheel? Does the mass of the pole have an effect? I am thinking that since τ is given, whatever effect the mass has must be taken care of by τ, so I would be that of the wheel only.

atransx = r τ/I = 2 τ/mr

Then I use the counterclockwise τ to get the acceleration at the top of the rod by using the moment of inertial of the rod.

atangx = -r τ/I = - 3τ/m(2d) = -1.5τ/md ... (3)

Summing them up:

atopx = ( 2/r - 1.5/d ) τ/m ... (4)

This means that whether the rod fall to the left or the right depends on r and d. In particular when:

(2d - 1.5r)/(rd) > 0
d > 0.75 r

The top of the rod would be moving forward. According to the drawing, since d is longer than r (not to mention 2 times d, which is the length of the rod), the rod will be moving to the right (while falling counter-clockwise).

Is this interpretation correct?

But now I have another question:

Suppose the rod is shorter than r, how do I know that the wheel would turn at all? How do I know that the motor is not just spinning itself about the axle, while the wheel does not move?
 
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