The potential energy of a particle possessing a magnetic (dipole) moment and interacting with a uniform magnetic field can be obtained as follows:
where \mu is the magnetic moment of a particle which is parallel to spin. Hence, the difference between the potential energies of particles whose spin is parallel and antiparallel to the field is
 In case of an electron
where \mu_B is the Bohr magneton.
Substituting the numerical values, we obtain:
Answer: 1) 1.74×10-4 eV.
Comments
Leave a comment