The magnetic dipole moment of a revolving electron: The electron of change (–e) performs uniforms circular motion around a stationary heavy nucleus of charge +Ze. This constitutes a current I.
∴I=Te ...(i)
Where, T is the time period of revolution. Let r be the orbital radius of electron and v the orbital speed. Then T=υ2πr ...(ii)
Substituting the value of T in (i), we get I=υ2πre=2πreυ
The magnetic moment (m) associated with this circular current is m=Iπr2[∵m→=IA→] ∴m=2πreυ⋅πr2=2eυr