Shock propagation into weakly ionized gases shows several features dif
fering markedly from conventional, nonionized-gas shock structure. Phe
nomenological analysis of general macroscopic features of the previous
ly observed plasma shock effects allows only two possible interpretati
ons: existence of an energy (momentum) flux toward the wave precursor
or volumetric energy release (exothermic phase transition! in the upst
ream portion of the wave !precursor) followed by reverse transition in
the downstream portion of the wave. It is shown that known microscopi
c mechanisms are not capable of producing such a flux or energy releas
e: Typical processes involving electrons, ions, and excited species do
not couple strongly to neutral atoms and molecules, and there is not
enough energy stored in these species because of the low ionization fr
action. The theoretical basis for phase transitions in low-density, we
akly ionized plasmas also is unknown. Analysis of the steady two-wave
system created by either of the two effects raises a question as to wh
ether the observed plasma shocks are stable objects. Another question
is whether there exists phase transition within the plasma shock. It a
lso remains unclear to what extent two-dimensional thermal inhomogenei
ty effects contribute to the observed phenomena. Answering these Funda
mental questions requires additional experimental studies of the probl
em.