Hostname: page-component-78c5997874-m6dg7 Total loading time: 0 Render date: 2024-11-19T13:43:17.503Z Has data issue: false hasContentIssue false

A quantum theory for non-viscous fluids in the Lagrange variables

Published online by Cambridge University Press:  24 October 2008

S. F. B. Tyabji
Affiliation:
Christ's CollegeCambridge

Extract

1. Introduction. A number of authors (2,3,7) have recently quantized the motion of an inviscid fluid. The starting point has been the variational principle of Bateman which uses the Clebsch variables. The density turns out to be the canonical conjugate to the velocity potential, and the transition to the quantum theory is then made in the usual way. If the fluid is making small vibrations, ‘phonons’, which are scalar, appear as a result of the quantization.

Type
Research Article
Copyright
Copyright © Cambridge Philosophical Society 1954

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

(1)Dirac, P. A. M.Principles of quantum mechanics (Oxford, 1947).Google Scholar
(2)Itö, H.Progr. theor. Phys., Osaka, 9 (1953), 117.Google Scholar
(3)Kronig, R. and Thellung, A.Physica, 's Grav., 18 (1952), 749.Google Scholar
Thellung, A.Physica, 's Grav., 19 (1953), 217.Google Scholar
(4)Lichtbnstein, L.Qrundlagen der Hydromechanik (Berlin, 1929).Google Scholar
(5)Wentzel, G.Quantum theory of fields (New York, 1949).Google Scholar
(6)Whittakeb, E. T.Analytical dynamics (Cambridge, 1917).Google Scholar
(7)Ziman, J. M.Proc. roy. Soc. A, 219 (1953), 257.Google Scholar