A one-dimensional energy equation, with constant pressure and area, was used to model the LSC wave. This equation balances convection, conduction, laser energy absorption, radiation energy loss and radiation energy transport. Solutions of this energy equation were obtained to give profiles of temperature and other properties, as well as the relation between laser intensity and mass flux through the wave. The flow through the LSC wave was then conducted through a variable pressure, variable area streamtube to accelerate it to high speed, with the propulsion application in mind. A numerical method for coupling the LSC wave model to the streamtube flow was developed, and a sample calculation was performed. The result shows that 42% of the laser power has been radiated away by the time the gas reaches the throat. It was concluded that in the radially confined flows of interest for propulsion applications, transverse velocities would be less important than in the unconfined flows where air experiments have been conducted.
[1]
A. Boni,et al.
Propagation of laser supported deflagration waves
,
1974
.
[2]
J. Jackson,et al.
Role of Radiative Transport in the Propagation of Laser Supported Combustion Waves
,
1974
.
[3]
David C. Smith,et al.
Ignition and maintenance of subsonic plasma waves in atmospheric pressure air by cw CO2 laser radiation and their effect on laser beam propagation
,
1975
.
[4]
R. Patch.
Absorption coefficients for hydrogen. I.
,
1969
.
[5]
A. Boni,et al.
Nonlinear model of laser supported deflagration waves
,
1976
.
[6]
E. Klosterman,et al.
Measurement of subsonic laser absorption wave propagation characteristics at 10.6 μm
,
1974
.