A solid sphere of mass ' $m$ ' and radius ' $r$ ' is allowed to roll without slipping from the highest point of an inclined plane of length ' $L$ ' and makes an angle $30^{\circ}$ with the horizontal. The speed of the particle at the bottom of the plane is $v_1$. If the angle of inclination is increased to $45^{\circ}$ while keeping $L$ constant. Then the new speed of the sphere at the bottom of the plane is $v_2$. The ratio $v_1^2: v_2^2$ is
Solution
<p>Let's analyze the problem step-by-step.</p>
<p><p>Energy conservation: </p>
<p>When the sphere rolls without slipping, its gravitational potential energy converts into both translational and rotational kinetic energy. The energy conservation equation is given by: </p>
<p>$mgL\sin\theta = \frac{1}{2}mv^2 + \frac{1}{2}I\omega^2$ </p>
<p>where:</p></p>
<p><p>$L\sin\theta$ is the vertical height,</p></p>
<p><p>$I$ is the moment of inertia, and</p></p>
<p><p>$\omega$ is the angular speed.</p></p>
<p><p>Moment of Inertia and Rolling Condition: </p>
<p>For a solid sphere, the moment of inertia about its center is: </p>
<p>$I = \frac{2}{5}mr^2$ </p>
<p>Since the sphere rolls without slipping, the linear speed $v$ and the angular speed $\omega$ are related by: </p>
<p>$v = r\omega \quad \Rightarrow \quad \omega = \frac{v}{r}$</p></p>
<p><p>Total Kinetic Energy: </p>
<p>Substituting the rolling condition into the rotational kinetic energy gives: </p>
<p>$ \begin{aligned} K &= \frac{1}{2}mv^2 + \frac{1}{2}\left(\frac{2}{5}mr^2\right) \left(\frac{v}{r}\right)^2 \\ &= \frac{1}{2}mv^2 + \frac{1}{2}\left(\frac{2}{5}mr^2\right) \frac{v^2}{r^2} \\ &= \frac{1}{2}mv^2 + \frac{1}{5}mv^2 \\ &= \frac{7}{10}mv^2 \end{aligned} $</p></p>
<p><p>Finding $v^2$ in Terms of $L$ and $\sin\theta$: </p>
<p>Equate the initial potential energy to the final kinetic energy:</p>
<p>$mgL\sin\theta = \frac{7}{10}mv^2$ </p>
<p>Solving for $v^2$:</p>
<p>$v^2 = \frac{10}{7}gL\sin\theta$</p></p>
<p><p>Apply to the Two Cases: </p></p>
<p><p>For $\theta = 30^\circ$, since $\sin(30^\circ) = \frac{1}{2}$:</p>
<p>$v_1^2 = \frac{10}{7}gL\left(\frac{1}{2}\right) = \frac{5}{7}gL$ </p></p>
<p><p>For $\theta = 45^\circ$, since $\sin(45^\circ) = \frac{1}{\sqrt{2}}$:</p>
<p>$v_2^2 = \frac{10}{7}gL\left(\frac{1}{\sqrt{2}}\right)$</p></p>
<p><p>Calculate the Ratio $\frac{v_1^2}{v_2^2}$: </p>
<p>$ \begin{aligned} \frac{v_1^2}{v_2^2} &= \frac{\left(\frac{5}{7}gL\right)}{\left(\frac{10}{7}gL\frac{1}{\sqrt{2}}\right)} \\ &= \frac{5}{10}\sqrt{2} \\ &= \frac{\sqrt{2}}{2} \end{aligned} $</p>
<p>Expressing this ratio as $v_1^2 : v_2^2$, we have:</p>
<p>$v_1^2 : v_2^2 = 1 : \sqrt{2}$</p></p>
<p><p>Conclusion: </p>
<p>According to the options given, the correct answer is:</p>
<p>Option C: $1:\sqrt{2}$.</p></p>
About this question
Subject: Physics · Chapter: Rotational Motion · Topic: Centre of Mass
This question is part of PrepWiser's free JEE Main question bank. 158 more solved questions on Rotational Motion are available — start with the harder ones if your accuracy is >70%.