Cylinder rolling thanks to external torque.

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Homework Help Overview

The problem involves a cylinder of mass m and radius R rolling on a plane with a constant torque applied about its center of mass. The discussion centers on determining the acceleration of the center of mass while ensuring rolling without slipping.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore different methods to calculate the angular and linear accelerations, considering the effects of torque and friction. Questions arise regarding the application of torque equations and the role of friction in the calculations.

Discussion Status

Some participants have provided guidance on setting up the torque equation relative to the center of mass, including the torque due to friction. There appears to be a productive exchange of ideas as one participant confirms their understanding and resolves discrepancies in their calculations.

Contextual Notes

Participants discuss the implications of using different reference points for calculating moments of inertia and the resulting effects on the equations of motion. The conversation reflects an ongoing examination of the assumptions related to torque and friction in the context of rolling motion.

bobon123
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Homework Statement



A cylinder of mass m and radius R is set on a plane, with large enough friction coefficient to ensure at any moment rolling without slipping. A constant torque is applied along the axis passing through the center of mass (G) of the cylinder and perpendicular to the basis of the cylinder.
What is the acceleration of the center of mass G?

Homework Equations



The central equation in this problem is
I dw / dt = M
This equation should be valid if w (angular velocity) and I are referred to either an axis passing through the center of mass of the system (I_G) or through a point that is fixed along the motion.

I will also need to compute I for the cylinder,
I_G=1/2 mR^2,
while remembering that, if I need I for a different axis,
I_O=I_G+ m (GO)^2

The Attempt at a Solution



To find a solution is easy, I have two! I can set myself either in the center of mass, or in the contact point between the cylinder and the plane, since it is fixed.

In the second case, I have I_O = 3/2 mR^2 and therefore the angular acceleration is 2 M/(3 mR^2), and the linear acceleration should be 2M/(3 mR)
In the first case, I have I_G=1/2 mR^2, and therefore the angular acceleration is 2 M/(mR^2) and the linear acceleration would be 2 M/(mR).

I am pretty sure the proper solution is the first, but I am not able to understand why I can't solve it easily in the center of mass... I think I am missing in this case the additional torque caused by the attrition force, but I don't understand how that would bring the total to 2M/(3 mR)
 
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Welcome to PF!
bobon123 said:
... I am not able to understand why I can't solve it easily in the center of mass... I think I am missing in this case the additional torque caused by the attrition force
Yes.
but I don't understand how that would bring the total to 2M/(3 mR)
Try setting up the torque equation relative to the center of mass with the torque due to friction included. Don't forget that you also have Fnet = M aG.
 
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Thanks a lot! I think I am there:

In the center of mass, I have
1) M_T = M - F_a R
2) F_a = m a_G
3) M_T= I_G dw/dt
where M_T is the total torque and the friction is the only force parallel to the plane. I also have
4) a_G = dw / dt R,
since the cylinder is rolling without slipping.

Therefore, from 1) and 2),
5) M_T=M-m a_G R

While from 3) and 4),
6) M_T=1/2 m R a_g

Therefore, from 5) and 6),
7) M-m R a_G = 1/2 m R a_g,
from which a_g = 2 M / (3 m R)

Perfect! Finally the two solutions are only one!
 
Looks great. Good work!
 

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