A solid cylinder of radius \(R\) is at rest at a height \(h\) on an inclined plane. If it rolls down, then its velocity on reaching the ground is
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For rolling bodies, always include both translational and rotational kinetic energies:
\[
K=\frac12 mv^2+\frac12 I\omega^2
\]
and use the rolling condition
\[
v=R\omega.
\]
Step 1: Apply conservation of mechanical energy. The solid cylinder starts from rest at height $h$. All potential energy converts to kinetic energy (translational + rotational): \[ mgh = \frac{1}{2}mv^2 + \frac{1}{2}I\omega^2 \] where $v$ is the translational speed at the bottom and $\omega$ is the angular velocity. Step 2: Use the moment of inertia of a solid cylinder. For a solid cylinder: \[ I = \frac{1}{2}mR^2 \] Step 3: Apply the rolling without slipping condition. For rolling without slipping: \[ v = R\omega \implies \omega = \frac{v}{R} \] Substituting: \[ \frac{1}{2}I\omega^2 = \frac{1}{2} \cdot \frac{1}{2}mR^2 \cdot \frac{v^2}{R^2} = \frac{1}{4}mv^2 \] Step 4: Substitute back into the energy equation. \[ mgh = \frac{1}{2}mv^2 + \frac{1}{4}mv^2 = \frac{3}{4}mv^2 \] Cancelling $m$: \[ gh = \frac{3}{4}v^2 \] \[ v^2 = \frac{4gh}{3} \] \[ v = \sqrt{\frac{4gh}{3}} \] Step 5: Compare with the options. $v = \sqrt{\frac{4gh}{3}}$ matches option 4. Note how the rotational kinetic energy reduces the final translational speed compared to a sliding object (which would give $v = \sqrt{2gh}$). Step 6: State the final answer. The velocity of the solid cylinder on reaching the ground is $\sqrt{\dfrac{4gh}{3}}$. \[ \boxed{\sqrt{\dfrac{4gh}{3}}} \]