An electron orbiting the nucleus in a circular path generates a loop current.
The current \( I \) is defined as:
\[ I = \frac{\text{Charge per revolution}}{\text{Time for one revolution}} \]
With the electron's charge being \( e \) and its time period \( T \):
\[ T = \frac{2\pi r}{v} \]
Consequently,
\[ I = \frac{e}{T} = \frac{e}{\frac{2\pi r}{v}} = \frac{ev}{2\pi r} \]
The magnetic moment \( \mu \) is calculated using the formula:
\[ \mu = I \times A \]
For a circular orbit, the area \( A \) is:
\[ A = \pi r^2 \]
Therefore,
\[ \mu = \frac{ev}{2\pi r} \times \pi r^2 \]
This simplifies to:
\[ \mu = \frac{evr}{2} \]
The angular momentum \( L \) of the electron is given by:
\[ L = mvr \]
where \( m \) is the electron's mass.
Using the previously derived equation:
\[ \mu = \frac{evr}{2} \]
Substituting \( vr \) from the angular momentum equation:
\[ \mu = \frac{e}{2m} L \]
Thus, the magnetic moment associated with the orbiting electron is:
\[ \mu = \frac{e}{2m} L \]
(b) If \( \vec{L} \) is the angular momentum of the electron, show that:
\[ \vec{\mu} = -\frac{e}{2m} \vec{L} \]