Now since the only force acting on the particle is T and us always acting radially inwards, there is no torque acting on the disc as seen from the center of rotation (the hole). In other words the angular momentum as seen from the hole will always be conserved. Hence we have,
Sunday, June 29, 2008
Irodov Problem 1.193
Now since the only force acting on the particle is T and us always acting radially inwards, there is no torque acting on the disc as seen from the center of rotation (the hole). In other words the angular momentum as seen from the hole will always be conserved. Hence we have,
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