Magnetic susceptibility
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In electrical engineering, the magnetic susceptibility is the degree of magnetization of a material in response to a magnetic field. The dimensionless mass magnetic susceptibility is represented by the symbol χ (lowercase Greek letter chi).
- <math>
\chi = \frac {M} {H} <math>
where
M is the magnetization of the material (the magnetic dipole moment per unit mass), measured in A/m (i.e. Amperes per metre)
H is the applied field, measured in A/m (where the magnetic induction B is related to H by the relationship <math>B = \mu_0(H + J)<math> where μ0 is the permeability of vacuum (see table of physical constants).)
If χ is positive the material is called paramagnetic, and the magnetic field is strengthened by the presence of the material. If χ is negative then the material is diamagnetic and the magnetic field is weakened in the presence of the material.
The magnetic susceptibility of a ferromagnetic substance is not linear. Response is dependent upon the state of sample and can occur in directions other than that of the applied field. To accommodate this, a more general definition using a tensor derived from derivatives of components of M with respect to components of H
- <math>\chi_{ij} = \frac{\part M_j}{\part H_i}<math>
called the differential susceptibility describes ferromagnetic materials. When the coercivity of the material parallel to an applied field is the smaller of the two, the differential susceptibility is merely a function of the applied field.
The magnetic susceptibility and the magnetic permeability (μ) are related by the following formula:
- <math>\mu = \mu_0(1+\chi) \,<math>de:Suszeptibilität