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I. Multiple Choice Questions · Q13

Q.The speed of a solid sphere after rolling down from rest without sliding on an inclined plane of vertical height hh is,

(a) 4gh3\sqrt{\dfrac{4gh}{3}}
(b) 10gh7\sqrt{\dfrac{10gh}{7}}
(c) 2gh\sqrt{2gh}
(d) gh2\sqrt{\dfrac{gh}{2}}
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Step 1. Set up energy conservation.

The sphere starts from rest at height hh and rolls without slipping to the bottom. No energy is lost to friction (static friction does no work when there's no slipping at the contact point), so all the lost gravitational PE converts into kinetic energy — both translational (of the center of mass) and rotational (spin about the center):

mgh=12mv2+12Iω2.mgh = \dfrac12 mv^2 + \dfrac12 I\omega^2.

Step 2. Substitute the solid sphere's moment of inertia and the rolling condition.

For a solid sphere, I=25mR2I = \dfrac25 mR^2, and pure rolling means ω=v/R\omega = v/R. Substituting:

mgh=12mv2+12(25mR2)(vR)2=12mv2+15mv2.mgh = \dfrac12 mv^2 + \dfrac12\left(\dfrac25 mR^2\right)\left(\dfrac{v}{R}\right)^2 = \dfrac12mv^2 + \dfrac15 mv^2.

Step 3. Combine the kinetic-energy terms.

mgh=(12+15)mv2=5+210mv2=710mv2.mgh = \left(\dfrac12+\dfrac15\right)mv^2 = \dfrac{5+2}{10}mv^2 = \dfrac{7}{10}mv^2.

Step 4. Solve for vv.

The mass mm cancels from both sides:

gh=710v2⇒v2=10gh7⇒v=10gh7.gh = \dfrac{7}{10}v^2 \quad\Rightarrow\quad v^2 = \dfrac{10gh}{7} \quad\Rightarrow\quad v = \sqrt{\dfrac{10gh}{7}}.

Step 5. Match against the printed options.

Among the four choices — 4gh/3\sqrt{4gh/3}, 10gh/7\sqrt{10gh/7}, 2gh\sqrt{2gh}, gh/2\sqrt{gh/2} — the derivation above lands exactly on 10gh/7\sqrt{10gh/7}, i.e. option (b).

Step 6. Rule out the other options physically. …

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