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Transcript
The total free energy of a
magnetic substance
LL8 Section 32
Magnetizable body
Magnetic field
For given currents j in some conductors, the
thermodynamic potential with respect to T and j is
For constant T and j, irreversible processes occur until
is minimized.
In equilibrium
is a minimum with respect to changes
in state occurring at constant T and j.
For given j and constant T, the change in
is the work done by the field on the
conductors.
In the absence of the body,
where
is the magnetic field produced by the given j
without contribution from the magnetized body.
Thing to remember: H is not the same as
they are often almost the same.
, but for non-ferromagnetic bodies,
With the body present,
includes the energy of
the external field that magnetizes the body.
Free energy density
of body without field.
New definition
The difference in old and new definitions does not affect the
differential thermodynamic relations of the body.
,
Field part of the
energy density,
which includes the
contribution from M
For a reversible change in
at constant T
HW
Magnetization of the body
Change in the original external
field that created M
For spatially uniform
Total magnetic moment
of the body
When temperature is not constant
By analogy with dielectrics (section 11)
Absolute, not differential
Usually the magnetic susceptibility is small for non ferromagnetic
bodies, so that their magnetization does not affect the currents
that create the field that magnetizes the body. Then the free
energy is linearly proportional to the susceptibility.
This is found from the original current distribution
(e.g. an electromagnet) without any magnetizable
material around.