Hyperenthalpic flows are encountered when spatial vehicules reenter the atm
osphere (Anderson 1989) or in some astrophysical situations as in envelopes
of cool pulsating stars (Lafon 1991). In reentry applications, a bow shock
is created at the front of the vehicule. The plasma in the shock layer is
highly collisional and the radiative heat flux is of the same order of magn
itude as the convective heat flux. It is then necessary to take into accoun
t the coupling between aerodynamics and radiation.
For high mach numbers, electronic collisional processes are out of equilibr
ium, and each atomic electronic level has to be considered as a distinct ch
emical species. The structure of the system is globally non-linear and the
coupling is taken into account by mass conservation, energy exchange, and r
adiation-matter interaction. The radiative transfer also depends on atomic
and molecular spectra in conditions of nonequilibrium for which cross secti
ons and reaction rates are not well known and difficult to calculate.