Finding angular velocity after block is moved from middle to outside of disc

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The discussion centers on calculating the angular velocity of a turntable after a block is moved from the center to the edge. Initially, the user attempted to use energy conservation principles, calculating the final rotational inertia and energy, but arrived at an incorrect answer. A key insight shared is that conservation of angular momentum should be used instead of energy conservation in this scenario, as angular momentum is conserved when no net external forces or torques are acting. This approach simplifies the problem significantly and leads to the correct solution. The user expresses gratitude for this clarification, indicating a shift in understanding.
snoworskate
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Homework Statement



A 200 g, 42.0-cm-diameter turntable rotates on frictionless bearings at 56.0 rpm. A 20.0 g block sits at the center of the turntable. A compressed spring shoots the block radically outward along a frictionless groove in the surface of the turntable.

What is the turntable's rotation angular velocity when the block reaches the outer edge?

Homework Equations



Ei=Ef
.5Iw^2 (initial) = .5Iw^2 (final)

For finding the final rotational inertia:
I(final) = Icm + Md^2 = .5MR^2 + md^2

The Attempt at a Solution



I believe that energy is conserved in this process so the equation above is valid. I calculated the final rotational inertia to be (1/2)*(0.2kg)*(0.21m)^2 + (0.02kg)*(0.21m)^2 = 0.005292

The initial energy is (.5)*(.5*0.2kg*0.21m^2)*(56rpm)^2 = 6.915

The final energy is (.5)*(0.005292)*wfinal^2

Solving for wfinal I get 53.6 rpm. I've done the calculations repeatedly and I can't come up with an alternate way of doing it but this answer is not correct. Any ideas?

Thank you so much in advance!
 
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hi snoworskate! :smile:
snoworskate said:
… I believe that energy is conserved in this process so the equation above is valid

I can't come up with an alternate way of doing it but this answer is not correct. Any ideas?

never never never use conservation of energy if you can use conservation of momentum (or angular momentum).

Momentum (or angular momentum) is always conserved (if there is zero net force or torque, as in this case).

Energy usually isn't conserved, and virtually never is in exam questions unless the question gives a pretty clear hint that it is. :wink:
 
Wow, that was MUCH easier. Thanks so much, I'll remember that!
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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