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On the theory of the liquid state

III. The hole theory of the viscous flow of liquids

Published online by Cambridge University Press:  24 October 2008

R. Fürth
Affiliation:
The University Edinburgh

Extract

It is assumed that the viscosity of a liquid is due to the transfer of momentum by the irregular movement of the holes (see part I of this paper). A formula for the absolute value of the viscosity and its dependence on the temperature can be derived by the theory and is in agreement with its experiments.

Type
Research Article
Copyright
Copyright © Cambridge Philosophical Society 1941

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References

REFERENCES

(1)Fürth, R.Proc. Cambridge Phil. Soc. 37 (1941), 252.CrossRefGoogle Scholar
(2)Fürth, R., Ornstein, L. S. and Milatz, J. M. W.Proc. Amsterdam Acad. Sci. 42, (1939), 107.Google Scholar
(3)Landolt-Börnstein, . Physikalisch Chemische Tabellen, 5 Aufl. (Berlin, 1923); 1. Erg. Band 1927, 2. Erg. Band 1931, 3. Erg. Band 1935/36.Google Scholar
(4)Chiong, Y. S.Proc. Roy. Soc. A, 157 (1936), 264.Google Scholar
(5)Born, M.Proc. Cambridge Phil. Soc. 36 (1940), 160.CrossRefGoogle Scholar
(6)‘A discussion on viscosity of liquids’, Proc. Roy. Soc. A, 163 (1937), 319.CrossRefGoogle Scholar
(7)Mott, N. F. and Gurney, R. W.Rep. Progress Phys. 5 (1939), 46.CrossRefGoogle Scholar
(8)Andrade, E. N.da, C.Phil. Mag. (7), 17 (1934), 497.CrossRefGoogle Scholar
(9)Andrade, E. N.da, C.Phil. Mag. (7), 17 (1934), 698.CrossRefGoogle Scholar
(10)Ewell, R. H. and Eyring, H.J. Chem. Phys. 5 (1937), 726.CrossRefGoogle Scholar