Question:

A uniform solid cylinder of mass \( m \) and radius \( r \) rolls along an inclined rough plane of inclination \( 45^\circ \). If it starts to roll from rest from the top of the plane, then the linear acceleration of the cylinder axis will be:

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For rolling motion without slipping, use both the translational and rotational equations of motion. The frictional force causes the rotation, and the rolling condition \( a = r\alpha \) relates the linear and angular accelerations.
Updated On: Apr 30, 2025
  • \( \frac{1}{\sqrt{2}} g \)
  • \( \frac{1}{3\sqrt{2}} g \)
  • \( \frac{\sqrt{2} g}{3} \)
  • \( \sqrt{2} g \)
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The Correct Option is C

Solution and Explanation

Step 1: Find the acceleration of the cylinder. For a solid cylinder rolling down an incline without slipping, the acceleration \(a\) is given by the formula:

\[ a = \frac{g \sin \theta}{1 + \frac{I}{mr^2}}, \] where: - \(I\) is the moment of inertia of the cylinder about its axis of rotation, - \(m\) is the mass, - \(r\) is the radius, and - \(\theta\) is the angle of inclination. For a solid cylinder, the moment of inertia \(I\) is given by: \[ I = \frac{1}{2}mr^2. \] Substituting this into the formula for acceleration: \[ a = \frac{g \sin \theta}{1 + \frac{\frac{1}{2}mr^2}{mr^2}} = \frac{g \sin \theta}{1 + \frac{1}{2}} = \frac{2}{3}g \sin \theta. \]

Step 2:

Substitute the given values. In this case, \(\theta = 45^\circ\), so \(\sin \theta = \sin 45^\circ = \frac{1}{\sqrt{2}}\). \[ a = \frac{2}{3}g \left( \frac{1}{\sqrt{2}} \right) = \frac{2}{3\sqrt{2}}g = \frac{2\sqrt{2}}{3 \cdot 2}g = \frac{\sqrt{2}}{3}g. \]

Final Answer:

The linear acceleration of the cylinder's axis is \( \frac{\sqrt{2}}{3}g \). The correct answer is option (3).

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