Question:medium

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

Show Hint

For rolling bodies, always include both translational and rotational kinetic energies: \[ K=\frac12 mv^2+\frac12 I\omega^2 \] and use the rolling condition \[ v=R\omega. \]
Updated On: Jun 22, 2026
  • \(\sqrt{\frac{5gh}{3}}\)
  • \(\sqrt{\frac{2h}{3g}}\)
  • \(\sqrt{\frac{2gh}{3}}\)
  • \(\sqrt{\frac{4gh}{3}}\)
Show Solution

The Correct Option is D

Solution and Explanation

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 $\sqrt{\dfrac{4gh}{3}}$. \[ \boxed{\sqrt{\dfrac{4gh}{3}}} \]
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