Rotational kinetic energy explaination

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SUMMARY

The discussion centers on the principles of rotational dynamics, specifically the conservation of angular momentum and its implications for kinetic energy. A classroom demonstration involving a person on a rotating stool illustrates how pulling weights inward decreases the moment of inertia, doubling the angular speed and kinetic energy. A contrasting scenario with a tethered volleyball raises questions about energy sources when the moment of inertia decreases without additional energy input. The resolution lies in understanding that the tension in the string, which is influenced by external forces, does work on the system, thereby accounting for the increase in kinetic energy.

PREREQUISITES
  • Understanding of rotational dynamics and angular momentum
  • Familiarity with kinetic energy concepts in physics
  • Knowledge of forces and work in mechanical systems
  • Basic principles of energy conservation and transformation
NEXT STEPS
  • Explore the mathematical derivation of rotational kinetic energy formulas
  • Study the implications of the conservation of angular momentum in various systems
  • Investigate the role of tension in mechanical systems and its effects on energy transfer
  • Examine real-world applications of rotational dynamics in engineering and physics
USEFUL FOR

Students and educators in physics, mechanical engineers, and anyone interested in understanding the principles of rotational dynamics and energy conservation.

  • #91
aaaa202 said:
hmm it's just that when you see the ball for the point of contact between string and pole it makes a uniform circular motion. So can't you say that the angular momentum is conserved in this frame for the ball? And why does that not qualify to the ball's angular momentum being conserved like if the rotation was around the center of mass? :)

The point of contact is changing all the time: it's turning in a circle around the pole, so (as Philip pointed out) it's constantly accelerating. If we fix one point on the surface of the pole and measure the angular momentum around this point, we'll see that the momentum of the ball must be changing, since there is only one instant when the ball exerts no torque in this frame: the instant when the centre of rotation is at the point we have fixed. For the rest of the time, the centre of rotation is not at the point we have fixed, so there is torque around this point.
 
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  • #92
yes okay, I should have realized that. But doesn't there exist conservation laws in non inertial reference frames?
 
  • #93
I expect so. Indeed I expect we could easily find such a frame in which angular momentum is conserved for the ball. But that would not be anything to be especially pleased about. The ball's angular momentum would be conserved simply because we've chosen a special frame in which it is conserved. In this frame, things whose angular momentum we'd normally expect to be conserved won't have it conserved... The laws of Physics are usually easier in inertial frames.
 

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