Rigorous proof about the nature of rolling motion

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SUMMARY

The discussion focuses on the nature of rolling motion as described in Resnick/Halliday, emphasizing the relationship between rotational and translational motion. It establishes that rolling can be analyzed through two frameworks: one centered at the center of mass and another at the bottom of the wheel. The velocities derived from both perspectives are equivalent, as demonstrated by the concept of relative velocity, specifically V(particle/ground) = V(particle/com) + V(com/ground). A rigorous proof is sought to clarify this equivalence and address the intuitive challenges associated with it.

PREREQUISITES
  • Understanding of rotational motion and translational motion
  • Familiarity with the concept of center of mass
  • Knowledge of relative velocity principles
  • Basic grasp of kinematics in physics
NEXT STEPS
  • Study the derivation of velocities in rolling motion using the center of mass approach
  • Explore the concept of relative velocity in different frames of reference
  • Learn about the implications of rotational motion on the bottom point of a rolling object
  • Investigate rigorous proofs related to rolling motion in classical mechanics
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Physics students, educators, and anyone interested in the mathematical foundations of motion, particularly in understanding rolling dynamics and relative velocity concepts.

quincyboy7
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In Resnick/Halliday, they describe how rolling can be described as the sum of a rotational force centered at the center of mass (for a wheel, say) and translational motion. The next part involves them saying that the motion can also be described as a completely rotational motion centered at the bottom of the wheel, pointing to how the velocities work in this framework for the bottom, center of mass, and top of the wheel as a "proof".

How does one generalize this into a complete proof however, that the velocities obtained by summing rotational motion from the center of the wheel plus translational motion is equal to the velocities by a rotational motion from the bottom of the wheel? It just doesn't seem very intuitive to me and a rigorous proof might clear up some doubts. Thanks as always!
 
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Since in rotational motion the velocity of the bottom most point is zero, there is no change in frame of reference. It is same as ground.
When we take rotational velocity from center of mass and add velocity of center of mass we are basically applying:
V(particle/ground) = V(particle/com) + V(com/ground)---> concept of relative velocity
In case of the bottom most point its velocity is zero, hence normal velocity is considered.
 

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