On the problem of the static helium film
Author:
Publisher
Springer Science and Business Media LLC
Subject
Astronomy and Astrophysics,Nuclear and High Energy Physics,Atomic and Molecular Physics, and Optics
Link
http://link.springer.com/content/pdf/10.1007/BF02731632.pdf
Reference11 articles.
1. S. Franchetti:Nuovo Cimento,4, 1504 (1956) and5, 183 (1957) (henceforth referred to as I and II).
2. Use of free energy is due to the assumption of negligible external pressure (See I, Sect.2). About condition (1) see also Appendix A of this paper.
3. K. R. Atkins andR. A. Stasior:Canad. Journ. of Phys.,31, 1156 (1953).
4. S. Franchetti:Nuovo Cimento,12, 749 (1954) and II, App. B.
5. In writing down eq. (19), the surface energy has been assumed to be thickness-independent. Indeed,C. G. Kuper [Physica,22, 1291 (1956)] has recently suggested that surface waves might be affected by the Van der Waals field of the wall. This would bring about at-dependent term, concerning mainly the zero point energy of these waves. An exact treatment of such an effect would be rather difficult. However, a rough evaluation of orders of magnitude leads to a contribution to eq. (19) which isnegligible in comparison of the Van der Waals term even for a thickness of 10−6 cm (corresponding to more than 1 dm height).
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1. Chapter 2 Third Sound;Progress in Low Temperature Physics;1970
2. Flowing Liquid He II: Critical Velocities and Dissipation Functions;Helium-3 and Helium-4;1969
3. The thickness of the moving helium II film;Proceedings of the Physical Society;1964-07
4. The thickness of the saturated helium film above and below the λ-point;Philosophical Magazine;1959-12
5. On the Thickness of Helium Films;Proceedings of the Physical Society;1959-08-01
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