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Orifice flow at high Knudsen numbers

Published online by Cambridge University Press:  28 March 2006

Roddam Narasimha
Affiliation:
Guggenheim Aeronautical Laboratory, California Institute of Technology, Pasadena, California

Abstract

Several interesting features of the flow field in free-molecule flow through an orifice are discussed. An estimate is then made of the deviation of the mass flow $\dot{m}$ through the orifice from its limiting free-molecule value $\dot{m}$ for small departures from the limit. Using an iteration method proposed by Willis, it is shown that this deviation is of the first order in ε, the inverse Knudsen number, defined as the ratio of the radius of the hole to the mean free path in the gas at upstream infinity. An estimate of the coefficient is obtained making some reasonable assumptions about the three-dimensional nature of the flow, and the value so derived, giving $\dot{m}=\dot{m}(1+0.25\epsi)$, shows fair agreement with the measurements of Liepmann. It appears that ‘nearly’ free-molecular conditions prevail up to ε ∼ 1.0.

Type
Research Article
Copyright
© 1961 Cambridge University Press

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References

Bhatnagar, P. L., Gross, E. P. & Krook, M. 1954 Phys. Rev. 94, 511.
Bromwich, T. J. I'A 1926 Introduction to the Theory of Infinite Series. London: Macmillan.
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Narasimha, R. 1960 Phys. Fluids, 3, 476.
Present, R. D. 1958 Kinetic Theory of Gases. New York: McGraw-Hill.
Sadowsky, M. A. & Sternberg, E. 1950 Quart. Appl. Math. 8, 113.
Willis, D. R. 1958 Princeton Univ. Rep. no. 442.
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