In this schlieren system the probing laser beam is attenuated by a neutral density wedge (instead of the usual knife edge) so that the intensity is proportional to the deflection angle, which in turn is proportional to the density gradient. Time integration of the attenuated probe beam intensity yields the absolute refractive index variation across moving objects. The device is tested by measuring the density jump across a Mach 9 shock wave.
REFERENCES
1.
2.
3.
A. G. Gaydon and I. R. Hurle, The Shock Tube in High Temperature Chemical Physics (Chapman and Hall, London, 1961).
4.
M.
Yasuhara
, K.
Yoneda
, and S.
Sato
, J. Phys. Soc. Jpn.
36
, 555
(1974
).5.
6.
B.
Ahlborn
and A. J.
Barnard
, AIAA J. (Am. Inst. Aeronaut. Astronaut.)
4
, 1136
(1966
).7.
B.
Ahlborn
and R.
Morris
, J. Quant. Spectrosc. Radiat. Transfer
9
, 1519
(1969
).8.
9.
10.
P. C. T. de Boer, Ph.D. thesis, University of Maryland, 1962 (University Microfilm, 313 First St., Ann Arbor, MI, Order No. 63‐7137).
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© 1976 American Institute of Physics.
1976
American Institute of Physics
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