Rotation qns which i am stuck for 2 hours

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The discussion centers on a physics problem involving a gymnast tossing a hoop with a backward spin. The key challenge is determining the minimum backward angular velocity required for the hoop to eventually spin back, considering the effects of friction. The net torque acting on the hoop is not zero due to friction, complicating the application of angular momentum conservation. The conversation highlights the relationship between translational and rotational kinetic energy, particularly when the hoop is on the verge of rolling backward. The participants emphasize the importance of understanding torque and energy conservation in solving the problem.
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I have been stuck at this qns for 2 hours.

A gymnast often toss a hoop forward while giving it a backward spin. the hoop has a radius R and mass M, and is thrown forward with speed V. Find the minimum backward angular velocity w the gymnast must give in order to make sure it spin back eventually . Take both its static and kinectic coefficent of friction to be #.

Since friction is acting , its nett torque is not 0. Hence conserv. of angular momentum cannot be applied.

if its nett torque is Mg#R, how should i relate this to the translational and rotational K.E.?

Please teach me how to solve this.
 
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if the torque is taken about contact point(bottum) then torque due to all three forces is zero and we can conserve angular momentum.
 
so 1/2 I w^2= 1/2 MV^2 ?
 
yes, the kinetic energy of a rolling object is, as you have stated:
KE_{rolling} = \frac{1}{2}mv^2 + \frac{1}{2}I{\omega}^2

if the object is on the veeeeeeerge of rolling backwards, or back to the thrower, the inequality you have stated works.

Regards,

Nenad
 
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