A student stands on a horizontal platform that is free to rotate around a vertical axis. He holds two weights in his outstretched hands. Another student gives him a push and starts the platform rotating at 0.500 rev/s. The student then pulls the weights in close to his chest. The moment of inertia with the weights extended is 2.40 kgrn2; the moment of inertia with the weights close to the axis is 0.904 kgm2. Ignore any frictional effects. What is his new rate of rotation?

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Answer:

1327.43362 rev/s

Explanation:

[tex]I_i[/tex] = Initial moment of inertia = 2.4 kgm² (arms outstretched)

[tex]I_f[/tex] = Final moment of inertia = 0.904 kgm² (arms close)

[tex]\omega_f[/tex] = Final angular velocity

[tex]\omega_i[/tex] = Initial angular velocity = 0.5 rev/s

Here the angular momentum is conserved

[tex]I_i\omega_i=I_f\omega_f\\\Rightarrow \omega_f=\frac{I_i\omega_i}{I_f}\\\Rightarrow \omega_f=\frac{2.4\times 500}{0.904}\\\Rightarrow \omega_f=1327.43362\ rev/s[/tex]

The new rate of rotation is 1327.43362 rev/s

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