Vortex Stationary Karman Structures in Flows of a Rotating Incompressible Polymer Fluid

A. M. Blokhin; R. E. Semenko

doi:10.1134/S0015462820070034

Vortex Stationary Karman Structures in Flows of a Rotating Incompressible Polymer Fluid

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Аннотация

The paper considers stationary solutions for the motion problem of a finite layer of an incompressible polymer fluid over an infinite rotating disk. An approximate stationary solution representation is used, similar to the self-similar Karman solution for a viscous fluid. Examples of stationary numerical solutions are given for various values of the problem’s parameters.

Язык оригинала	английский
Страницы (с-по)	925-935
Число страниц	11
Журнал	Fluid Dynamics
Том	55
Номер выпуска	7
DOI	https://doi.org/10.1134/S0015462820070034
Состояние	Опубликовано - сен 2020

Доступ к документу

10.1134/S0015462820070034

Ссылка на публикацию в Scopus

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abstract = "The paper considers stationary solutions for the motion problem of a finite layer of an incompressible polymer fluid over an infinite rotating disk. An approximate stationary solution representation is used, similar to the self-similar Karman solution for a viscous fluid. Examples of stationary numerical solutions are given for various values of the problem{\textquoteright}s parameters.",

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N2 - The paper considers stationary solutions for the motion problem of a finite layer of an incompressible polymer fluid over an infinite rotating disk. An approximate stationary solution representation is used, similar to the self-similar Karman solution for a viscous fluid. Examples of stationary numerical solutions are given for various values of the problem’s parameters.

AB - The paper considers stationary solutions for the motion problem of a finite layer of an incompressible polymer fluid over an infinite rotating disk. An approximate stationary solution representation is used, similar to the self-similar Karman solution for a viscous fluid. Examples of stationary numerical solutions are given for various values of the problem’s parameters.

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KW - self-similar solution

KW - stationary solutions

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