A uniformly thick wheel with moment of inertia


A uniformly thick wheel with moment of inertia I and radius $R$ is free to rotate about its centre of mass (see fig). A massless string is wrapped over its rim and two blocks of masses $m_{1}$ and $m_{2}\left(m_{1}>m_{2}\right)$ are attached to the ends of the string. The system is released from rest. The angular speed of the wheel when $m_{1}$ descents by a distance $h$ is:

  1. $\left[\frac{2\left(m_{1}-m_{2}\right) g h}{\left(m_{1}+m_{2}\right) \mathrm{R}^{2}+1}\right]^{1 / 2}$

  2. $\left[\frac{2\left(m_{1}+m_{2}\right) g h}{\left(m_{1}+m_{2}\right) \mathrm{R}^{2}+1}\right]^{1 / 2}$

  3. $\left[\frac{\left(m_{1}-m_{2}\right)}{\left(m_{1}+m_{2}\right) \mathrm{R}^{2}+1}\right]^{1 / 2} g h$

  4. $\left[\frac{m_{1}+m_{2}}{\left(m_{1}+m_{2}\right) \mathrm{R}^{2}+1}\right]^{1 / 2} g h$

Correct Option: 1


(1) Using principal of conservation of energy

$\left(m_{1}-m_{2}\right) g h=\frac{1}{2}\left(m_{1}+m_{2}\right) v^{2}+\frac{1}{2} I \omega^{2}$

$\Rightarrow \quad\left(m_{1}-m_{2}\right) g h=\frac{1}{2}\left(m_{1}+m_{2}\right)(\omega R)^{2}+\frac{1}{2} I \omega^{2}$

$(\because v=\omega R)$

$\Rightarrow \quad\left(m_{1}-m_{2}\right) g h=\frac{\omega^{2}}{2}\left[\left(m_{1}+m_{2}\right) R^{2}+I\right]$

$\Rightarrow \omega=\sqrt{\frac{2\left(m_{1}-m_{2}\right) g h}{\left(m_{1}+m_{2}\right) R^{2}+I}}$

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