Question:

When a solid sphere rolls without slipping down an inclined plane making an angle $\theta$ with the horizontal, the acceleration of its centre of mass is $a$. If the same sphere slides without friction, its acceleration $a'$ will be

Updated On: Jul 28, 2023
  • $\frac{7}{2}a$
  • $\frac{5}{7}a$
  • $\frac{7}{5}a$
  • $\frac{5}{2}a$
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The Correct Option is C

Solution and Explanation

Acceleration of the solid sphere when it rolls without slipping down an inclined plane is $ a= \frac{g\, sin \,\theta}{1+\frac{I}{MR^{2}}} $ For a solid sphere, $I= \frac{2}{5}MR^{2}$ $\therefore a = \frac{g \,sin \,\theta}{1+\frac{2}{5}} = \frac{5}{7} g \,sin\, \theta\quad...\left(i\right)$ Acceleration of the same sphere when it slides without friction down an same inclined plane is $a'= g \,sin \,\theta\quad...\left(ii\right) $ Divide $\left(ii\right)$ by $\left(i\right)$, we get $ \frac{a'}{a} = \frac{7}{5}$ or $a' = \frac{7}{5}a$
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System of Particles and Rotational Motion

  1. The system of particles refers to the extended body which is considered a rigid body most of the time for simple or easy understanding. A rigid body is a body with a perfectly definite and unchangeable shape.
  2. The distance between the pair of particles in such a body does not replace or alter. Rotational motion can be described as the motion of a rigid body originates in such a manner that all of its particles move in a circle about an axis with a common angular velocity.
  3. The few common examples of rotational motion are the motion of the blade of a windmill and periodic motion.