Morin classical mechanics page 326 example

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SUMMARY

The discussion focuses on a problem from Morin's classical mechanics regarding the acceleration of a mass connected to a uniform cylinder on an inclined plane. It establishes that the accelerations of the two masses are not equal, specifically that the acceleration of mass m (a2) is twice that of the cylinder (a1), expressed as a2 = 2a1. This relationship arises from the rolling motion of the cylinder without slipping, where the topmost point's velocity is twice that of the center of mass. The confusion stems from assuming equal accelerations, which leads to incorrect results.

PREREQUISITES
  • Understanding of classical mechanics principles, specifically rotational dynamics.
  • Familiarity with the concept of rolling without slipping.
  • Knowledge of kinematic relationships between linear and angular motion.
  • Basic grasp of pulley systems and tension in strings.
NEXT STEPS
  • Study the derivation of the relationship between linear acceleration and angular acceleration in rolling objects.
  • Explore the conservation of string length in pulley systems, as discussed in the Kleppner-Kolenkow textbook.
  • Investigate the dynamics of inclined planes and the forces acting on objects in motion.
  • Review examples of similar problems in classical mechanics to reinforce understanding of acceleration relationships.
USEFUL FOR

Students of classical mechanics, physics educators, and anyone seeking to deepen their understanding of dynamics involving rolling objects and pulley systems.

almarpa
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Homework Statement


A string wraps around a uniform cylinder of mass M, which rests on a fixed plane with angle θ. The string passes up over a massless pulley and is connected to a mass m. Assume that the cylinder rolls without slipping on the plane, and that the string is parallel to the plane. What is the acceleration of the mass m?

Homework Equations



In the solucion, Morin claims that the masses acceleratins are not the same, and they are related by a2=2 a1, where a1 is the acceleratin for M, and a2 the acceleration for m

The Attempt at a Solution



When solving the problem, I used the same value for both accelerations, that is, a1=a2=a, so my result was wrong. Why are the accelerations different, if the pulley is at rest? Where does the a2=2 a1 equation come from?

Regrads.
 
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almarpa said:

Homework Statement


A string wraps around a uniform cylinder of mass M, which rests on a fixed plane with angle θ. The string passes up over a massless pulley and is connected to a mass m. Assume that the cylinder rolls without slipping on the plane, and that the string is parallel to the plane. What is the acceleration of the mass m?

Homework Equations



In the solucion, Morin claims that the masses acceleratin are not the same, and they are related by a2=2 a1, where a1 is the acceleratin for M, and a2 the acceleration for m

The Attempt at a Solution



When solving the problem, I used the same value for both accelerations, that is, a1=a2=a, so my result was wrong. Why are the accelerations different, if the pulley is at rest? Where does the a2=2 a1 equation come from?

Regrads.

When a cylinder/sphere rolls without slipping on a surface ,what is the relationship between velocity of topmost point and velocity of the Center of Mass ?
 
Last edited:
Yes, I know that the speed in the top is twice the speed of the center of mass, so the accelerations must obey the same relation . This is what Morin suggest to get this equation, altought I have not found the proof for this relation, so I would have never tought of this possibility. I was wondering if this constraint equation can be derived from the "conservation" of the length of the string, as Kleppner - Kolenkow textbook usually does.
 

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