Issue |
EPJ Web Conf.
Volume 173, 2018
Mathematical Modeling and Computational Physics 2017 (MMCP 2017)
|
|
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Article Number | 02009 | |
Number of page(s) | 4 | |
Section | Mathematical Modeling and Methods | |
DOI | https://doi.org/10.1051/epjconf/201817302009 | |
Published online | 14 February 2018 |
https://doi.org/10.1051/epjconf/201817302009
Diffusion Processes in the A-Model of Vector Admixture: Turbulent Prandtl Number
1 Institute of Experimental Physics, SAS, Košice, Slovakia
2 Bogoliubov Laboratory of Theoretical Physics, JINR, Dubna, Russian Federation
3 Dep. of Theoretical Physics and Astrophysics, Faculty of Science, P.J. Šafárik University, Košice, Slovakia
* e-mail: jurcisine@saske.sk
** e-mail: jurcisin@saske.sk
*** e-mail: remecky@saske.sk
Published online: 14 February 2018
Using analytical approach of the field theoretic renormalization-group technique in two-loop approximation we model a fully developed turbulent system with vector characteristics driven by stochastic Navier-Stokes equation. The behaviour of the turbulent Prandtl number PrA,t is investigated as a function of parameter A and spatial dimension d > 2 for three cases, namely, kinematic MHD turbulence (A = 1), the admixture of a vector impurity by the Navier-Stokes turbulent flow (A = 0) and the model of linearized Navier-Stokes equation (A = −1). It is shown that for A = −1 the turbulent Prandtl number is given already in the one-loop approximation and does not depend on d while turbulent Prandt numbers in first two cases show very similar behaviour as functions of dimension d in the two-loop approximation.
© The Authors, published by EDP Sciences, 2018
This is an Open Access article distributed under the terms of the Creative Commons Attribution License 4.0, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. (http://creativecommons.org/licenses/by/4.0/).
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