Difference between a spinning sphere and rolling one

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The discussion centers on the kinetic energy of a rolling sphere as it transitions from a slant to a loop. It highlights the conversion of potential energy into both translational and rotational kinetic energy. The conversation explores the distinction between the sphere's rotation around its center and its motion along the loop's trajectory. Participants clarify that while both types of rotation contribute to kinetic energy, they should not be counted twice in calculations. The exchange emphasizes the importance of accurately accounting for different moments of inertia in kinetic energy equations.
Gabriel Maia
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Consider this: We have a sphere rolling down a slant, released from some height h with null velocity. At the end of the slant its potential energy will have been fully converted to kinetic energy, part translational and part rotational.

Now consider this: at the end of the slant the ball enters a loop. As it travels around the loop reaching its top it will have a potential energy, alright, but more importantly for our present problem, it will have again a translational and a rotational kinetic energy. The rotational part is due to the ball spinning around its center (as it rolls along its path) or is it due to the rotation around the loop's center? Shouldn't be 2 rotationa kinetic energies?

Thank you
 
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Gabriel Maia said:
The rotational part is due to the ball spinning around its center
This is how it's usually defined, but you can decompose the KE any way you like. Note that the moment of inertia will depend on the center you chose.
 
I see...

But the moment of inertia of a particle on a circular trajectory is I = m R^2 (where R is the trajectory radius) and the moment of inertia of a sphere spinning around its own center is I = \frac{2}{5} m r^2(where r is the sphere radius). So the total kinetic energy will be

K = \frac{1}{2} mv^2 + \frac{1}{2} mR^2 \omega^2 + \frac{1}{2}\left[\frac{2}{5}mr^2\right]\omega'^2?

(where \omega is the angular speed of the ball around the loop and \omega'^2 around itself)
 
Gabriel Maia said:
I see...

But the moment of inertia of a particle on a circular trajectory is I = m R^2 (where R is the trajectory radius) and the moment of inertia of a sphere spinning around its own center is I = \frac{2}{5} m r^2(where r is the sphere radius). So the total kinetic energy will be

K = \frac{1}{2} mv^2 + \frac{1}{2} mR^2 \omega^2 + \frac{1}{2}\left[\frac{2}{5}mr^2\right]\omega'^2?
No, you are accounting twice for the movement along the circular path. The first two terms are identical, and represent the same thing.
 
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Splendid, how foolish of me. Thank you very much.
 

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