Two identical masses are connected to a spring of spring constant \(k.\) The two masses are slowly moved symmetrically so that the spring is stretched by \(x.\) The work done by the spring on each mass is:
1. \(\dfrac12 kx^2\)
2. \(\dfrac14kx^2\)
3. \(-\dfrac12 kx^2\)
4. \(-\dfrac14kx^2\)
A small block of mass '\(m\)' is placed against a compressed spring, of spring constant \(k\). The initial compression in the spring is '\(d\)'. The block is released and the spring relaxes, while the block is projected up to a height \(H\) relative to its initial position. Then, \(H\) =
1. | \(\dfrac{kd^2}{2mg}\) | 2. | \(\dfrac{kd^2}{2mg}+d \) |
3. | \(\dfrac{kd^2}{2mg}-d\) | 4. | \(\dfrac{kd^2}{mg}+d\) |
1. | \(x_{1}+x_{2}=\dfrac{\mu m g}{k}\) |
2. | \(x_{1}-x_{2}=\dfrac{\mu m g}{k}\) |
3. | \(x_{1}+x_{2}=\dfrac{2\mu m g}{k}\) |
4. | \(x_{1}-x_{2}=\dfrac{2\mu m g}{k}\) |
1. | \(\sqrt{\dfrac{kh^2}{m}} \) | 2. | \(\sqrt{\dfrac{k(\sqrt2-1)h^2}{m}} \) |
3. | \((\sqrt2+1)\sqrt{\dfrac{kh^2}{m}} \) | 4. | \((\sqrt2-1)\sqrt{\dfrac{kh^2}{m}}\) |