Cm Acceleration: Rolling Cylinder Movement Analysis

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Discussion Overview

The discussion revolves around the analysis of a rolling cylinder without slipping, specifically examining the motion of its center of mass (cm) and the implications of different approaches to understanding its acceleration. The scope includes theoretical considerations of motion, acceleration, and the application of different frames of reference.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose analyzing the motion of the rolling cylinder as a combination of translation of the cm and rotation about the cm, leading to the conclusion that the cm has no acceleration when moving at constant velocity.
  • Others argue that considering the motion as pure rotation about the instantaneous axis at the contact point suggests that the cm experiences centripetal acceleration, expressed as vcm^2/R.
  • A later reply questions the validity of using the instantaneous axis of rotation at the contact point, noting that this point is accelerating and thus does not represent an inertial frame.
  • Another participant mentions that while all points on the rim of the cylinder have centripetal acceleration relative to the cm, the force acting on them is perpendicular to the velocity, indicating that no work is done in this context.

Areas of Agreement / Disagreement

Participants express differing views on the appropriate frame of reference for analyzing the motion of the rolling cylinder, with no consensus reached on the implications of these approaches for understanding acceleration.

Contextual Notes

The discussion highlights the limitations of using the instantaneous axis of rotation, particularly regarding its non-inertial nature and the assumptions involved in approximating the motion of the cylinder.

enippeas
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hello and sorry for my english
Let us consider a rolling whithout slipping cylinder. We can work in two different ways. First considering the motion as a pure translation of the cm plus a rotation about the cm. Second, considering the motion as a pure rotation about the instantaneous axis from the contact point with the ground.
The cylinder is moving with constant velocity. In the first way, the cm has no acceleration. But in the second way, the cm has a centripetal acceleration vcm^2/R.
What is going wrong here?
 
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enippeas said:
hello and sorry for my english
Let us consider a rolling whithout slipping cylinder. We can work in two different ways. First considering the motion as a pure translation of the cm plus a rotation about the cm. Second, considering the motion as a pure rotation about the instantaneous axis from the contact point with the ground.
The cylinder is moving with constant velocity. In the first way, the cm has no acceleration. But in the second way, the cm has a centripetal acceleration vcm^2/R.
What is going wrong here?

Well, in the second picture, the cylinder really doesn't have a rotational motion about the axis at the contact point. This is only a lowest order approximation to the actual motion. The approximation is so bad that it will only give you the correct result for the velocity of the motion, not the acceleration.

Torquil
 
While using an instantaneous axis of rotation at the contact point is OK for some purposes, realize that the contact point is itself accelerating so it is not an inertial frame.
 
Although all points on the rim of the cylinder have centripetal acceleration relative to the cm, the force is perpendicular to the velocity, so no work is done.

Bob S
 

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