Hostname: page-component-5c6d5d7d68-xq9c7 Total loading time: 0 Render date: 2024-08-11T13:27:21.248Z Has data issue: false hasContentIssue false

VIII.—Theoretical Expressions for Relaxation Effects in the Thermal Conductivity of Gases as Measured in the Modified Co-axial Cylinder Apparatus of Callear and Robb

Published online by Cambridge University Press:  14 February 2012

P. G. Wright
Affiliation:
Department of Chemistry, Queen's College, Dundee.

Synopsis

The apparent thermal conductivity of a polyatomic or isomerizing gas (as measured in a given apparatus) may decrease at low pressures for two distinct reasons. There may be accommodation effects at boundary surfaces, and there may be relaxation effects arising because molecules with excess energy do not yield it up fast enough to maintain local “chemical” equilibrium. If the apparatus is such that the temperature measured at points in the gas and not in the walls, relaxation effects may be observed directly, and accommodation effects are (in theabsence of relaxation effects) absent.

A detailed analysis is made of the apparent thermal conductivity measured in such an apparatus with cylindrical symmetry. Expressions are obtained in closed form. Numerical calculations show that, for a gas of relatively long relaxation time in an apparatus of reasonable dimensions, the apparent thermal conductivity would decrease appreciably at readily-attained pressures.

Type
Research Article
Copyright
Copyright © Royal Society of Edinburgh 1962

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

References to Literature

Brokaw, R. S., 1961. J. Chem. Phys., 35, 1569.CrossRefGoogle Scholar
Callear, A. B., and Robb, J. C, 1955. Trans. Faraday Soc, 51, 630.CrossRefGoogle Scholar
Chapman, S., and Cowling, T. G., 1939. Mathematical Theory of Non-Uniform Gases, p. 238. Cambridge.Google Scholar
Franck, E. U., and Spalthoff, W., 1954. Z. Elektrochem., 58, 374.Google Scholar
Fuchs, N. A., 1934. Phys. Z. Sowjet., 6, 225.Google Scholar
Hirschfelder, J. O., 1957. J. Chem. Phys., 26, 282.CrossRefGoogle Scholar
Kennard, E. H., 1938. Kinetic Theory of Gases, p. 312. New York.Google Scholar
Schäfer, K., Rating, W., and Eucken, A., 1942.Ann. Phys., 42, 176.CrossRefGoogle Scholar
Srivastava, B. N., and Barua, A. K., 1961. Proc. Phys. Soc. Lond., 77, 677.CrossRefGoogle Scholar
Ubbelohde, A. R. J. P., 1935. J. Chem. Phys., 3, 219.CrossRefGoogle Scholar
Waelbroeck, F. G., and Zuckerbrot, P., 1958. J. Chem. Phys., 28, 524.CrossRefGoogle Scholar
Whittaker, E. T., and Watson, G. N., 1920. Modern Analysis, 3rd ed., p. 373. Cambridge.Google Scholar
Wright, P. G., 1960. Disc. Faraday Soc, 30, 100.CrossRefGoogle Scholar
Wright, P. G., 1962. Proc. Roy. Soc. Edin., A, 66, 6580.Google Scholar
Wright, P. G., and Gray, P., 1961. Trans. Faraday Soc, 57, 657.CrossRefGoogle Scholar