Conservation of angular momentum and energy

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SUMMARY

The discussion centers on the conservation of angular momentum and energy in a spinning body when its shape changes, specifically addressing the relationship between moment of inertia and angular velocity. It is established that if angular velocity is conserved due to no net torque, the body will spin at a different speed but maintain the same direction. The rotational kinetic energy does change, necessitating that the excess kinetic energy manifests as translational motion. The example of two weights connected by a cord illustrates that work is required to change their configuration, affecting both energy and angular momentum, which remain conserved despite changes in angular velocity.

PREREQUISITES
  • Understanding of angular momentum conservation principles
  • Familiarity with rotational kinetic energy concepts
  • Knowledge of moment of inertia and its impact on rotational motion
  • Basic grasp of non-inertial reference frames and centrifugal force
NEXT STEPS
  • Study the relationship between moment of inertia and angular velocity in rotating systems
  • Explore the implications of energy conservation in non-inertial frames
  • Investigate the effects of shape changes on the inertial tensor
  • Learn about practical applications of angular momentum conservation in engineering
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Physics students, mechanical engineers, and anyone interested in the principles of rotational dynamics and energy conservation in physical systems.

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if you have a spinning body, and then its shape changes so that the moment of inertia changes, what happens? If angular velocity is conserved, since there's no net torque, then it spins a different speed, but the same direction. But then has the rotational kinetic energy changed? And if so, does this mean the excess kinetic energy must take the form of translational motion? Does it matter if the change in shape was symmetrical?
 
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Consider a very simple example - two weights connected by a cord spinning around their common center.

If you pull the weights in, it will require work to do so. (The easiest way to see this is to go to a non-inertial frame that's corotating with the weights, and consider the centrifugal force). Similarly, if you let the weights go out, work will be generated and must be dissipated (perhaps by friction).

Energy and angular momentum will both be conserved.
 
The (instantaneous) angular velocity may well change its direction, since (for one) we cannot assume that the shapechange does not affect the inertial tensor (with respect to the C.M).
The angular momentum, remains, however, constant.
 

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