| 1. | \(x=0 \) | 2. | \(x= \pm A \) |
| 3. | \(x= \pm \dfrac{A}{\sqrt{2}}\) | 4. | \(x=\dfrac{A}{2}\) |
| 1. | \( { K.E. }=\dfrac{k A^2}{8} \\ { P.E. }=\dfrac{3 k A^2}{8} \\ v=\dfrac{A}{3} \sqrt{\dfrac{k}{m}} \) | 2. | \({ K.E. }=\dfrac{3 k A^2}{8} \\ { P.E. }=\dfrac{k A^2}{8} \\ v=\dfrac{A}{2} \sqrt{\dfrac{3 k}{m}} \) |
| 3. | \({ K.E. }=\dfrac{3 k A^2}{8} \\ { P.E. }=\dfrac{k A^2}{4} \\ v=A \sqrt{\dfrac{3 k}{m}} \) | 4. | \({ K.E. }=\dfrac{k A^2}{4} \\ { P.E. }=\dfrac{3 k A^2}{8} \\ v=\dfrac{A}{4} \sqrt{\dfrac{3 k}{m}} \) |
| 1. | \(2\) | 2. | \(4\) |
| 3. | \(-2\) | 4. | \(-4\) |
| 1. | \(\dfrac{A}{\sqrt{2}}, \dfrac{A}{\sqrt{2}} \omega\) | 2. | \(\dfrac{A}{2}, \dfrac{A}{2} \omega\) |
| 3. | \(\sqrt2A, 2A \omega\) | 4. | \(\sqrt2A, \sqrt2A \omega\) |
| 1. | \((TE)\) is zero when \(x = 0.\) |
| 2. | \((PE)\) is maximum when \(x = 0.\) |
| 3. | \((KE)\) is maximum when \(x = 0.\) |
| 4. | \((KE)\) is maximum when \(x\) is maximum. |
| 1. | \(\left({{{A}\over{2}}}\right)\) | 2. | \(\left({{{A}\over{\sqrt{2}}}}\right)\) |
| 3. | \(\left({{{A}\over{2\sqrt{2}}}}\right)\) | 4. | \(\left({{{A}\over{4}}}\right)\) |
A particle executes simple harmonic motion with a frequency of \(2\) Hz. The frequency with which its potential energy oscillates is:
1. \(4\) Hz
2. \(2\) Hz
3. \(6\) Hz
4. \(8\) Hz
| 1. | \(\dfrac{A}2\) | 2. | \(\dfrac{A}{\sqrt{2}}\) |
| 3. | \(\dfrac{A \sqrt{2}}{3}\) | 4. | \(A \sqrt{2} \) |
| 1. | \(2\sqrt{A}\) | 2. | \(\dfrac{A}{2}\) |
| 3. | \(\dfrac{\mathrm{A}}{\sqrt{2}}\) | 4. | \(A\sqrt{2}\) |