We present a cold plasma, two-fluid electromagnetic theory of the norm
al modes of a plasma shell expanding, at sub-Alfvenic velocities, into
a magnetic field. A two-fluid approach is used in order that the spec
ific effects of plasma and magnetic field geometry can be considered.
Three main results are obtained. First, a general normal mode equation
for lower-hybrid frequency range oscillations is derived which is mor
e accurate in its treatment of the plasma and magnetic field geometry
than previous published normal mode equations. The higher accuracy acc
rues because no a priori assumptions are made about the ratio of pertu
rbation and equilibrium scale lengths. The second set of results is th
e establishment of specific criteria for the existence of localized so
lutions of the lower-hybrid drift normal mode equation and the develop
ment of analytical formulae which describe the dispersive properties o
f this instability. These are useful because results concerning lower-
hybrid drift instability growth rates and maximal growing wave numbers
are usually given in the context of the local approximation without s
pecifying where the normal modes are localized within the highly inhom
ogeneous plasma profile. The third result is a cautionary one. Two equ
ilibrium models are constructed with identical magnetic field profiles
, similar density profiles, but distinctive electron cross-field veloc
ity profiles. The localization criteria and analytical formulae for lo
wer-hybrid drift dispersive properties are found to be quite accurate
for one equilibrium model but to be inappropriate for the other.