Gyromagnetism
For gyromagnetic media (see Faraday rotation)
the magnetic permeability response to an
alternating electromagnetic field in the
microwave frequency domain is treated as a
non-diagonal tensor expressed by: [5]
Values for some common
materials
The following table should be used with caution
as the permeability of ferromagnetic materials
varies greatly with field strength. For example
4% Si steel has an initial relative permeability
(at or near 0T) of 2,000 and a maximum of
35,000 [6] and, indeed, the relative permeability
of any material at a sufficiently high field
strength trends toward 1.
Magnetic susceptibility and permeability data for
selected materials
For gyromagnetic media (see Faraday rotation)
the magnetic permeability response to an
alternating electromagnetic field in the
microwave frequency domain is treated as a
non-diagonal tensor expressed by: [5]
Values for some common
materials
The following table should be used with caution
as the permeability of ferromagnetic materials
varies greatly with field strength. For example
4% Si steel has an initial relative permeability
(at or near 0T) of 2,000 and a maximum of
35,000 [6] and, indeed, the relative permeability
of any material at a sufficiently high field
strength trends toward 1.
Magnetic susceptibility and permeability data for
selected materials
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