For a circular loop of radius \( r \) with current \( I \), the magnetic field at its centre is given by: \[ B = \frac{\mu_0 I}{2r} \]
The area \( A \) of a circle with radius \( r \) is defined as: \[ A = \pi r^2 \]. Therefore, the radius can be expressed as: \[ r = \sqrt{\frac{A}{\pi}} \]
Rearranging the magnetic field formula \( B = \frac{\mu_0 I}{2r} \) to solve for the current \( I \): \[ I = \frac{2Br}{\mu_0} \]
The magnetic moment \( M \) of a current loop is calculated as the product of the current and the area: \[ M = I \cdot A \] Substitute the expression for \( I \) derived previously: \[ M = \left( \frac{2Br}{\mu_0} \right) \cdot A \] Now, substitute the expression for \( r \) in terms of \( A \): \[ M = \frac{2B}{\mu_0} \cdot A \cdot \sqrt{\frac{A}{\pi}} = \frac{2BA}{\mu_0} \sqrt{\frac{A}{\pi}} \]
The magnetic moment of the circular loop has been shown to be: \[ M = \frac{2BA}{\mu_0} \sqrt{\frac{A}{\pi}} \]
(b) If \( \vec{L} \) is the angular momentum of the electron, show that:
\[ \vec{\mu} = -\frac{e}{2m} \vec{L} \]