Method of trial distribution function for quantum turbulence
Studying quantum turbulence the necessity of calculation the various characteristics of the vortex tangle (VT) appears. Some of "crude" quantities can be expressed directly via the total length of vortex lines (per unit of volume) or the vortex line density L(t) and the structure paramet...
Збережено в:
Дата: | 2012 |
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Автор: | |
Формат: | Стаття |
Мова: | English |
Опубліковано: |
Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
2012
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Назва видання: | Физика низких температур |
Теми: | |
Онлайн доступ: | http://dspace.nbuv.gov.ua/handle/123456789/117922 |
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Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
Цитувати: | Method of trial distribution function for quantum turbulence / S.K. Nemirovskii // Физика низких температур. — 2012. — Т. 38, № 11. — С. 1306–1312. — Бібліогр.: 28 назв. — англ. |
Репозиторії
Digital Library of Periodicals of National Academy of Sciences of UkraineРезюме: | Studying quantum turbulence the necessity of calculation the various characteristics of the vortex tangle (VT)
appears. Some of "crude" quantities can be expressed directly via the total length of vortex lines (per unit of volume)
or the vortex line density L(t) and the structure parameters of the VT. Other more “subtle” quantities require
knowledge of the vortex line configurations {s(ξ,t)}. Usually, the corresponding calculations are carried
out with the use of more or less truthful speculations concerning arrangement of the VT. In this paper we review
other way to solution of this problem. It is based on the trial distribution functional (TDF) in space of vortex
loop configurations. The TDF is constructed on the basis of well established properties of the vortex tangle. It is
designed to calculate various averages taken over stochastic vortex loop configurations. In this paper we also review
several applications of the use this model to calculate some important characteristics of the vortex tangle.
In particular we discussed the average superfluid mass current J induced by vortices and its dynamics. We also
describe the diffusion-like processes in the nonuniform vortex tangle and propagation of turbulent fronts. |
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