No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
Experiments on radiatively driven harmonic acoustic waves in a confined gas
1.G. T. Chapman, D. L. Compton, and W. G. Vincenti, Phys. Fluids 16, 1232 (1973).
2.D. L. Compton, Ph.D. thesis, Stanford University, 1969.
3.G. T. Chapman, Ph.D. thesis, Stanford University, 1970.
4.R. B. McQuistan, J. Opt. Soc. Am. 48, 63 (1958).
5.W. G. Vincenti, Astronaut. Acta 15, 559 (1970).
6.W. M. Brandenberg and O. W. Clausen, in Symposium on Thermal Radiation of Solids, edited by S. Katzoff, NASA SP 55 (1965).
7.J. C. Richmond, W. N. Harrison, and F. J. Shorten, in Measurement of Thermal Radiation Properties of Solids, edited by J. C. Richmond, NASA SP 31 (1963).
8.F. D. Shields and R. T. Lageman, J. Acoust. Soc. Am. 29, 470 (1957).
9.R. D. Fay, J. Acoust. Soc. Am. 12, 62 (1940).
10.T. L. Cottrell and M. A. Day, in Molecular Relaxation Processes (Academic, New York, 1966), p. 253.
11.B. J. Lavercombe, Nature (Lond.) 211, 63 (1966).
12.Use of these data to deduce values of the vibrational relaxation time for the mixtures would not be justified, since small amounts of impurities must inevitably have been present and the effect of impurities on can be substantial.
13.Argon, being infrared‐inactive, does not participate in the radiative energy exchange.
14.D. K. Edwards, J. Opt. Soc. Am. 50, 617 (1960).
15.W. Malkmus, J. Opt. Soc. Am. 53, 951 (1963).
16.W. Malkmus, J. Opt. Soc. Am. 54, 751 (1964).
17.L. D. Gray, J. Quant. Spectrosc. Radiat. Transfer 5, 569 (1965).
18.R. P. Madden, J. Chem. Phys. 35, 2083 (1961).
19.L. D. Kaplan and D. F. Eggers, J. Chem. Phys. 25, 876 (1956).
20.S. S. Penner and D. Weber, J. Chem. Phys. 19, 1351 (1951).
21.L. A. Young, J. Quant. Spectrosc. Radiat. Transfer 8, 693 (1968).
22.D. K. Edwards and W. A. Menard, Appl. Opt. 3, 847 (1964).
23.M. M. Abu‐Romia and C. L. Tien, J. Quant. Spectrosc. Radiat. Transfer 6, 143 (1966).
24.There was, however, appreciable low‐frequency noise apparently caused by mechanical vibrations of the modulator drive system. This noise changed somewhat in intensity, but not frequency, as the modulator frequency was changed.
25.Lord Rayleigh, The Theory of Sound (Dover, New York, 1945), 2nd ed., Vol. 2, Sec. 339.
26.W. Chester, J. Fluid Mech. 18, 44 (1964).
27.R. A. Saenger and G. E. Hudson, J. Acoust. Soc. Am. 32, 961 (1960).
28.The rms deviation between the measurements and the vector sum is 0.07, while that between the measurements and modified‐classical wave is 0.13.
29.R. Kaiser, Can. J. Phys. 37, 1499 (1959).
30.This factor is needed when is not small compared with unity. It accounts for energy that is radiated from the vibrational states before collisional equilibration can occur between vibration and rotation‐translation. It cannot be derived within the framework of the theory presented in Ref. 1. This factor deviates negligibly from unity in the and tests.
31.R. C. Lind, Ph.D. thesis, Stanford University, 1971.
32.S. E. Gilles and W. G. Vincenti, J. Quant. Spectrosc. Radiat. Transfer 10, 71 (1970).
33.W. E. Woodmansee and J. C. Decius, J. Chem. Phys. 36, 1831 (1962).
34.A. D. Wood, Ph.D. thesis, Purdue University, 1963.
35.It is possible, of course, that some of the present observed pressure response was due to absorption by infrared‐active impurities. We believe, however, that any such response was negligibly small.
36.R. Tripodi and W. G. Vincenti, J. Chem. Phys. 55, 2207 (1971).
Article metrics loading...
Full text loading...