The present paper gives a review of the major problems associated with the use of hydrocarbon-a ir combustion gases as an aerodynamic test medium. Condensation of water vapor is identified as the major problem, and actual experience is offered as evidence of its effects on aerodynamic flow parameters. Aerodynamic data obtained from tests in methane-air combustion gases are compared with theory and with data obtained on the same shapes in other test facilities using other test media. The comparisons indicate that data obtained in combustion gas compare well with data obtained in other test media. Nomenclature A = cross-sectional area CA = axial-force coefficient, axial force/g S CD = drag coefficient, drag/# S CL(t = slope of the lift curve at a = 0 Cm = pitching-moment coefficient, pitching moment/^ SI CN = normal-force coefficient, normal force/g S Cp = specific heat at constant pressure d = model diameter, cm / = characteristic length (model length) M = Mach number
[1]
A. J. Hodges.
The Drag Coefficient of Very High Velocity Spheres
,
1957
.
[2]
Dean R Chapman,et al.
Some possibilities of using gas mixtures other than air in aerodynamic research
,
1956
.
[3]
Peter H. Rose,et al.
Laminar Heat Transfer Around Blunt Bodies in Dissociated Air
,
1959
.
[4]
J. Leith Potter,et al.
THE DRAG OF SPHERES IN RAREFIED HYPERVELOCITY FLOW
,
1963
.
[5]
F. R. Riddell,et al.
Theory of Stagnation Point Heat Transfer in Dissociated Air
,
1958
.
[6]
J. Aroesty.
SPHERE DRAG IN A LOW DENSITY SUPERSONIC FLOW
,
1962
.
[7]
R. Howell,et al.
CALCULATION PROCEDURE FOR THERMODYNAMIC, TRANSPORT, AND FLOW PROPERTIES OF THE COMBUSTION PRODUCTS OF A HYDROCARBON FUEL MIXTURE BURNED IN AIR WITH RESULTS FOR ETHYLENE-AIR AND METHANE-AIR MIXTURES
,
1962
.