Step 1: The angular momentum \( L \) of a particle rotating with respect to a central force is given by: \[ L = r \times p, \] where \( r \) is the position vector, and \( p \) is the linear momentum of the particle.
Step 2: The rate of change of angular momentum is related to the torque \( \tau \) acting on the particle: \[ \frac{dL}{dt} = \tau. \]
Step 3: If the torque \( \tau \) is zero, then the angular momentum remains constant. This happens when there is no external torque acting on the particle.
Step 4: Since central forces always act along the line joining the particle and the center of rotation, they produce zero torque. Therefore, the angular momentum of the particle remains constant.
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :
