Collisions in rotational dynamics

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SUMMARY

The discussion centers on the mechanics of collisions in rotational dynamics, specifically examining why a stationary rod rotates about the center of mass (CM) after being struck by a particle moving at speed v. It is established that the angular momentum of the system can be expressed as L=LCM+L', where LCM represents the angular momentum of the combined mass moving at the CM and L' is the angular momentum relative to the CM frame. The conversation also addresses the implications of elastic versus inelastic collisions on the rotational behavior of the rod and particle system.

PREREQUISITES
  • Understanding of angular momentum and its conservation principles
  • Familiarity with the concepts of center of mass (CM) in physics
  • Knowledge of elastic and inelastic collisions
  • Basic grasp of Newton's laws of motion, particularly F=ma
NEXT STEPS
  • Study the principles of angular momentum conservation in detail
  • Explore the differences between elastic and inelastic collisions
  • Learn about the dynamics of systems involving multiple bodies and their center of mass
  • Investigate real-world applications of rotational dynamics in engineering and physics
USEFUL FOR

This discussion is beneficial for physics students, educators, and professionals in engineering fields who are interested in understanding the principles of rotational dynamics and collision mechanics.

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If I have say a stationary rod, and a particle collides with the rod whilst moving at speed v at the top end, why does the rod then proceed to rotate about the centre of mass of the system (whether that be in an elastic or completely inelastic collision where they both stick together).

I believe it may have something to do with the fact the angular momentum can be written as
L=LCM+L'
with the first term that of a particle with the total mass of the system moving at the CM, and the second the angular momentum of the system relative to the CM (i.e in the CM frame). Thanks.
 
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Is that true? If the particle doesn't stick to the rod, why would the rod rotate about the center of mass of the system? Wouldn't it rotate about its own center of mass as it is not interacting with the particle anymore?

In the case where the two stick together, if they don't rotate about their center of mass, that means the center of mass is rotating about another point, so it is accelerating. Is that consistent with F=ma?
 

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