To find the radius of the circular orbit for a particle with mass \( m \) and angular momentum \( L \) moving under the potential energy \( U(r) = kr^2 \), we proceed as follows:
The force acting on the particle due to the potential energy is given by the negative gradient of \( U(r) \):
\(F(r) = -\frac{dU}{dr} = -\frac{d}{dr}(kr^2) = -2kr\)
For circular motion, the centripetal force required is provided by this force, and is given by \( \frac{L^2}{mr^3} \), the expression for centripetal force considering angular momentum:
\(\frac{L^2}{mr^3} = 2kr\)
Solve for \( r \) to determine the radius of the circular orbit:
\(L^2 = 2kmr^4\)
Rearranging gives:
\(r^4 = \frac{L^2}{2km}\)
Taking the fourth root on both sides:
\(r = \left(\frac{L^2}{2km}\right)^{\frac{1}{4}}\)
This matches the given option \((\frac{L^2}{2mk})^{\frac{1}{4}}\), thereby confirming it as the correct choice.
In order to achieve the static equilibrium of the see-saw about the fulcrum \( P \), shown in the figure, the weight of Box B should be _________ kg, if the weight of Box A is 50 kg.

A particle of mass 1kg, initially at rest, starts sliding down from the top of a frictionless inclined plane of angle \(\frac{𝜋}{6}\)\(\frac{\pi}{6}\) (as schematically shown in the figure). The magnitude of the torque on the particle about the point O after a time 2seconds is ______N-m. (Rounded off to nearest integer) 
(Take g = 10m/s2)

