(b) If \( \vec{L} \) is the angular momentum of the electron, show that:
\[ \vec{\mu} = -\frac{e}{2m} \vec{L} \]
μ = I · A
where:Step 1: Electron-induced current
For an electron moving in a circular orbit, the current is defined as the charge passing a point per unit time. If T is the time period of revolution, then:
f = 1 / T = v / (2πr)
Hence, the current I is:
I = e / T = e · (v / 2πr) = ev / (2πr)
Step 2: Orbital area
The area enclosed by the circular orbit is:
A = πr²
Step 3: Magnetic dipole moment
μ = I · A = (ev / 2πr) · (πr²)
μ = evr / 2
Thus, the magnetic dipole moment of an atom is:
μ = evr / 2
(b) To show: μ⃗ = −(e / 2m) L⃗
Solution:
The angular momentum of the electron is:
L⃗ = mvr
Substituting vr from this expression into μ:
μ = (e / 2) · (vr) = (e / 2m) · (mvr)
Since the electron carries negative charge, the direction of μ⃗ is opposite to L⃗:
μ⃗ = −(e / 2m) L⃗