An electric field with circular field lines is induced as the magnetic field is turned on.
Suppose the magnetic field increases linearly from zero to B in time t. According to Eq.
31-27, the magnitude of the electric field at the orbit is given by
$$E=\Bigg(\dfrac{r}{2}\Bigg)\dfrac{dB}{dt}=\Bigg(\dfrac{r}{2}\Bigg)\dfrac{B}{t}$$,
where r is the radius of the orbit. The induced electric field is tangent to the orbit and
changes the speed of the electron, the change in speed being given by
$$\Delta v=at=\dfrac{eE}{m_e}t=\Bigg(\dfrac{e}{m_e}\Bigg)\Bigg(\dfrac{r}{2}\Bigg)\Bigg(\dfrac{B}{t}\Bigg)t=\dfrac{erB}{2m_e}$$
The average current associated with the circulating electron is $$i = ev/2πr$$ and the dipole
moment is
$$\mu=Ai=(\pi r^2)\Bigg(\dfrac{ev}{2\pi r}\Bigg)\dfrac{1}{2}evr$$
The change in the dipole moment is
$$\mu=\dfrac{1}{2}er\Delta v =\dfrac{1}{2}er\Bigg(\dfrac{erB}{2m_e}\Bigg)=\Bigg(\dfrac{e^2r^2B}{4m_e}\Bigg)$$