\( \left( \frac{B}{2A} \right)^{\frac{1}{5}} \)
Step 1: The equilibrium position is obtained by differentiating the potential energy function with respect to \( r \) and setting the derivative equal to zero. \[ \frac{dU}{dr} = -\frac{10A}{r^{11}} + \frac{5B}{r^6} \] Setting \( \frac{dU}{dr} = 0 \) for equilibrium: \[ -\frac{10A}{r^{11}} + \frac{5B}{r^6} = 0 \] \[ \frac{10A}{r^{11}} = \frac{5B}{r^6} \] \[ \frac{2A}{r^5} = B \] \[ r^5 = \frac{2A}{B} \] \[ r = \left( \frac{2A}{B} \right)^{\frac{1}{5}} \]
Step 2: The equilibrium distance between the atoms is \( r = \left( \frac{2A}{B} \right)^{\frac{1}{5}} \).
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 :
