A solid cylinder of mass \(M\) and radius \(R\) rolls down an inclined plane of length \(L\) and height…
- \(\sqrt{2 g h}\)
- \(\sqrt{\frac{3 g h}{4}}\)
- \(\sqrt{\frac{4 g h}{3}}\)
- \(\sqrt{4 g h}\)
Solution

When cylinder reaches at bottom, then its whole potential energy is converted into its rotational kinetic energy and linear kinetic energy of its centre of mass. $\begin{aligned} \text{Hence, } & M g h=\frac{1}{2} I \omega^{2}+\frac{1}{2} M v_{\text{COM}}^{2} \\ &=\frac{1}{2} \times \frac{M R^{2}}{2} \times\left(\frac{v_{\text{COM}}}{R}\right)^{2}+\frac{1}{2} M v_{\text{COM}}^{2} \\ & \quad\left[\because I=\frac{M R^{2}}{2} \text{ and } \omega=\frac{v_{\text{COM}}}{R}\right] \\ &=\frac{M v_{\text{COM}}^{2}}{4}+\frac{M v_{\text{COM}}^{2}}{2} \\ & \Rightarrow \quad M g h=\frac{3}{4} M v_{\text{COM}}^{2} \end{aligned}$ $\begin{aligned} \Rightarrow & v_{\text{COM}}^{2}=\frac{4 g h}{3} \\ \Rightarrow & v_{\text{COM}}=\sqrt{\frac{4 g h}{3}} \end{aligned}$
Asked in: AP EAMCET 2020 (21 Sep Shift 1)