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A solid cylinder of mass m and radius R rolls down an inclined plane of height h without slipping. The speed of its centre of mass when it reaches the bottom is
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- √(2gh)
- √4gh/3
- √3gh/4
- √4g/h
Correct Option: B
| K.E. = | Iω² + | mv² | ||
| 2 | 2 |
| K.E. = | ![]() | mr² | ![]() | ω² + | mv² | |||
| 2 | 2 | 2 |
| = | mv² + | mv² = | mv² | |||
| 4 | 2 | 4 |
Now, gain in K.E. = Loss in P.E.
| mv² = mgh ⇒ v - √ | ![]() | ![]() | gh | ||
| 4 | 3 |

