By A. A. Abrikosov (auth.), K. D. Timmerhaus, W. J. O’Sullivan, E. F. Hammel (eds.)
The thirteenth foreign convention on Low Temperature Physics, geared up by means of the nationwide Bureau of criteria, Los Alamos clinical Laboratory, and the college of Colorado, was once held in Boulder, Colorado, August 21 to twenty-five, 1972, and was once backed via the nationwide technology starting place, the U. S. military workplace of clinical examine, the U. S. Atomic strength fee, the U. S. army workplace of Naval learn, the foreign Institute of Refrigeration, and the Internation al Union of natural and utilized Physics. This overseas convention was once the newest in a sequence of biennial meetings on low temperature physics, the 1st of which was once held on the Massachusetts Institute of know-how in 1949. (For an entire checklist of earlier L T meetings see p. viii. a lot of those previous meetings were coordinated and backed by way of the fee on Very Low Temperatures of IUPAP. next LT meetings might be scheduled triennially starting in 1975. LT thirteen was once attended by way of nearly 1015 members from twenty 5 international locations. Eighteen plenary lectures and 550 contributed papers have been offered on the convention. The convention begun with short introductory and inviting comments via Dr. R. H. Kropschot on behalf of the Organizing Committee, Professor J. Bardeen on behalf of the fee on Very Low Temperatures of the IUP AP, and professional fessor O. V. Lounasmaa on behalf of the foreign Institute of Refrigeration. The 8th London Award was once then awarded by means of Professor E.
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Extra info for Low Temperature Physics-LT 13: Volume 1: Quantum Fluids
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Surely the main reason for interest in He II is that its macroscopic behavior or hydrodynamics is a direct consequence of the operation of quantum mechanics on a massive scale. In this paper we will discuss those aspects of the macroscopic behavior of He II that are most closely related to the quantum theory. The first advance in our understanding of the hydrodynamics of superfluid helium was provided by the Landau two-fluid hydrodynamics! · V) v. = - VJ1. - va (1) where V. is the local velocity of the superfluid, a is the external potential per unit mass, and J1.