Linear Isotropic Non-Ferromagnetic Materials
| (06-13) |
is the magnetic susceptibility, is relates the local microscopic alignment
of the individual magnetic moments to the applied field.
If
, the magnetic moments align with the field--this is called a paramagnetic
material
If
, the magnetic moments align anti-parallel
with the field--this is called a diamagnetic material
Combining Eq. 6-11 with Eq. 6-13, we get the definition
of magnetic permeability
for an isotropic magnetic material:
| (06-14) |
And from this follows the associated magnetic work for this model: