Magnetohydrodynamics of a → plasma
with very large (infinite) → conductivity.
In this condition, → Ohm’s law reduces
to E = -v × B, where E
represents → electric field,
B → magnetic field,
and v the → fluid velocity.
Ideal MHD is the simplest model to describe the dynamics of
plasmas immersed in a magnetic field. It is concerned with
→ one-fluid magnetohydrodynamics and neglects
→ resistivity.
This theory treats the plasma composed of many
charged particles with locally neutral charge as a continuous single
→ fluid.
Ideal MHD does not provide information on the velocity distribution
and neglects the physics relating to wave-particle interactions, as
does the two-fluid theory as well. It does have the advantage that the
macroscopic dynamics of the → magnetized plasma
can be analyzed in realistic three-dimensional geometries
(K. Nishikawa & M. Wakatani, 2000, Plasma Physics, Springer).
See also → non-ideal magnetohydrodynamics.
See also: → ideal;
→ magnetohydrodynamics.