Slip condition for a pulled cylinder

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Homework Help Overview

The problem involves a massless string wrapped around a homogeneous cylinder being pulled to determine the maximum force that can be applied without causing the cylinder to slip on a horizontal surface. The context includes concepts from dynamics and friction, specifically focusing on the relationship between applied forces, friction, and rolling motion.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of symbolic representation versus numerical values to derive a general case for the maximum force. There are inquiries about the conditions under which slipping occurs and the relationship between acceleration and slipping.

Discussion Status

The discussion is ongoing, with participants exploring the implications of their analyses. Some guidance has been offered regarding the acceleration of the cylinder and its relationship to slipping, but no consensus has been reached on the generality of the maximum force condition.

Contextual Notes

Participants are considering the implications of their assumptions about the motion of the cylinder and the conditions for slipping, including the role of acceleration and the forces involved.

Helmholtz
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Homework Statement



Massless and inextensible string is wrapped around the periphery of a homogeneous cylinder of radius R = 0.5 m and mass m = 2 kg. The string is pulled straight away from the upper part of the periphery of the cylinder, without relative slipping. The cylinder moves on a horizontal floor, for which the friction coefficient (μ) is 0.4. What is most nearly the maximum force that can be exerted on the free end of the string so that the cylinder rolls without sliding?

(A) 24 N
(B) 12 N
(C) 8 N
(D) 6 N
(E) 8/3 N

Homework Equations



Your general rotational equations.

The Attempt at a Solution



I know the answer is A. My question is, is it a completely general case that the maximum force you can apply to a cylinder is 3 times the kinetic friction before it starts to slip?
 
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Hi, Helmholtz.

Did you try applying the same method that you used to find the answer (A), but using symbols rather than numbers? That way, you can get a general result and see if your conjecture is true.
 
Thanks for the response. I have done that, but I didn't like what I did and I was wonder if this was something someone could confirm.

Two forces directed in the same direction, one on top of the wheel, the other on the bottom. Forces add as such: F_1+F_2=ma (F_1 is the tension, F_2 is the friction), torques subtract such as F_1-F_2 = ma/2 (skipped a few steps hope it's followable). Then add them together (2*F_1 = 3/2 * ma), solve for a (a=4/3 * F_1/m), plug back into the force equation and find that 3*F_2 = F_1.

What I don't like is that the slip condition isn't obvious to me. Why is 'a' non-zero?

(Edit: I guess the slip condition was in the fact when I subtracted the torques and allowed \alpha = a/r)
(Edit: I suppose 'a' can be positive and there still is no slipping, not a condition I needed to impose. But when I thought about this in my mind, I assumed a cylinder of constant velocity, which is incorrect)
 
Last edited:
Right. The center of the cylinder is accelerating even though the cylinder is not slipping on the surface. Your analysis and comments look correct to me.
 

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