Experimental studies of shock modification in weakly ionized supersonic gas
flows are discussed. In these experiments, a supersonic nonequilibrium pla
sma wind tunnel which produces a highly nonequilibrium plasma flow with the
low gas kinetic temperature at M = 2, is used. Supersonic flow is maintain
ed at complete steady state. The flow is ionized by a high-pressure aerodyn
amically stabilized do discharge in the tunnel plenum and by a transverse r
f discharge in the supersonic test section. The do discharge is primarily u
sed for the supersonic flow visualization, whereas the rf discharge provide
s high electron density in the supersonic test section. High-pressure flow
visualization produced by the plasma makes all features of the supersonic f
low, including shocks, boundary layers, expansion waves, and wakes, clearly
visible. Attached oblique shock structure on the nose of a 35-deg wedge wi
th and without rf ionization in a If = 2 flow is studied in various nitroge
n-helium mixtures. It is Found that the use of the rf discharge increases t
he shock angle by 14 deg, from 99 to 113 deg, which corresponds to a Mach n
umber reduction from M=2.0 to 1.8. Time-dependent measurements of the obliq
ue shock angle show that the time for the shock weakening by the rf plasma,
as well as the shock recovery time after the plasma is turned off, is of t
he order of seconds. Because the flow residence time in the test section is
of the order of 10 mus, this result suggests a purely thermal mechanism of
shock weakening due to heating of the boundary layers and the nozzle walls
by the rf discharge. Gas flow temperature measurements in the test section
using infrared emission spectroscopy, with carbon monoxide as a thermometr
ic element, are consistent with the observed shock angle change. This shows
that shock weakening by the plasma is a purely thermal effect. The results
demonstrate the feasibility of both sustaining uniform ionization in cold
supersonic nitrogen and airflows and the use of nonequilibrium plasmas For
supersonic flow control. This opens a possibility for the use of transverse
stable rf discharges for magnetohydrodynamic energy extraction and/or acce
leration of supersonic airflows.