A particle is moving along a circular path with a radius \(a,\) under the influence of an attractive force. The potential energy associated with the particle is given by: \(U=-\dfrac{k}{2r^2}.\)
The attractive force acting on the particle is:
1. | \(\dfrac{k}{4a^3}\) | 2. | \(\dfrac{k}{2a^3}\) |
3. | \(\dfrac{k}{a^3}\) | 4. | \(\dfrac{3k}{2a^3}\) |
If the potential energy between two molecules is given by \(U = -\dfrac{A}{r^6}+ \dfrac{B}{r^{12}}\),
then the potential energy at equilibrium separation between molecules is:
1. | \(\dfrac{-A^{2}}{2B}\) | 2. | \(\dfrac{-A^{2}}{4B}\) |
3. | \(0\) | 4. | \(\dfrac{-A^{2}}{3B}\) |
1. | \(\left ( \dfrac{{A}}{{B}}\right )^{1/5}\) | 2. | \(\left ( \dfrac{{B}}{{A}}\right )^{1/5}\) |
3. | \(\left ( \dfrac{{2A}}{{B}}\right )^{1/5}\) | 4. | \(\left ( \dfrac{{B}}{{2A}}\right )^{1/5}\) |