Let an electron move in a circular orbit of radius r = ℏ2/me2 around a proton.
Assume that the z-component of the angular momentum is Lz = ℏ. Equating Lz to the classical angular momentum
Lz = ℏ = mer2ω ....(1)
An electron orbiting the proton with frequency v = ω/2π constitutes a current
i = ωe/2π
The magnetic moment μ0 produced is equal to this current multiplied by the area enclosed.
μB = i A = ωe. (πr2/2π) ......(2)
Using (1) in (2)
μB = eℏ/2me ....(3)
μB is known as Bohr magneton.
Electron with total angular momentum [j(j + 1)]1/2ℏ has a magnetic moment μ = [j(j + 1)]1/2μB
The z-component of the magnetic moment is μJ = mJμB where mJℏ is the z-component of the angular momentum.