Given the importance of linear mode properties (e.g., characteristic s
peeds) in identification/classification of discontinuities, a detailed
comparison between the mode properties in fluid theory and kinetic th
eory in high beta plasmas is carried out. It is found that conventiona
l fluid theories of linear modes in both isotropic and anisotropic pla
smas do not yield the correct mode properties, even in the long-wavele
ngth Limit. In particular, fluid phase velocities are very sensitive t
o the model and parameters (polytropic indices) employed. Because of t
his, fluid theory loses its predictive power. In linear kinetic theory
, modes cannot be ordered according to their phase velocities. For ins
tance, at small and moderate propagation angles, the slow/sound (S/SO)
mode can have the fastest phase velocity. In such cases, a (quasipara
llel) fast shock would be associated with the S/SO mode rather than th
e usual fast/magnetosonic (F/MS) model. This has important implication
s for fast shocks. Since it is the F/MS rather than S/SO mode that con
nects to the whistler branch, low Mach number quasiparallel shocks ass
ociated with S/SO would not be expected to have a phase standing whist
ler wave train upstream, and their thickness is determined by dissipat
ion rather than dispersion. The consequences of the kinetic mode prope
rties are demonstrated via hybrid simulations (fluid electron, kinetic
ions) using the quasiparallel shock as an example. (C) 1995 American
Institute of Physics.