a. 100 rev/min
Initial angular velocity, \(\omega_1\)= \(40 \,rev/min\)
Final angular velocity = \(\omega_2\)
The moment of inertia of the boy with stretched hands = \(\text I_1\)
The moment of inertia of the boy with folded hands = \(\text I_2\)
The two moments of inertia are related as :
\(\text I_2\) = \(\frac{2}{5}\text I_1\)
Since no external force acts on the boy, the angular momentum L is a constant. Hence, for the two situations, we can write :
\(\text I_2\omega_2\)= \(\text I_1\omega_1\)
\(\omega_2\) = \(\frac{\text I_1}{\text I_2}\omega_1\)
=\(\frac{\text I_1}{\frac{2}{5}I_1}\times40\) = \(\frac{5}{2}\times 40\)
= \(100 \,rev/min\)
(b) Final K.E. = 2.5 Initial K.E.
Final kinetic rotation, \(E_F\) = \(\frac{1}{2}\text I_2\omega^2_2\)
Initial kinetic rotation, \(E_I\)= \(\frac{1}{2}\text I_1\omega^2_1\)
\(\frac{E_F}{E_I}\) = \(\frac{\frac{1}{2}\text I_2\omega^2_2}{\frac{1}{2}\text I_1\omega^2_1}\)
= \(\frac{2}{5}\)\(\frac{\text I(100)^2}{\text I_1(40)^2}\)
= \(\frac{2}{5}\times \frac{100\times 100}{40\times 40}\)
= \(\frac{5}{2}\) = 2.5
∴ \(E_F\) = 2.5 \(E_1\)
The increase in the rotational kinetic energy is attributed to the internal energy of the boy.
The oxygen molecule has a mass of 5.30 × 10-26 kg and a moment of inertia of 1.94 ×10-46 kg m2 about an axis through its centre perpendicular to the lines joining the two atoms. Suppose the mean speed of such a molecule in a gas is 500 m/s and that its kinetic energy of rotation is two thirds of its kinetic energy of translation. Find the average angular velocity of the molecule.
From a uniform disk of radius R, a circular hole of radius \(\frac{R}{2}\) is cut out. The centre of the hole is at \(\frac{R}{2}\) from the centre of the original disc. Locate the centre of gravity of the resulting flat body.