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Journal ArticleDOI

Exact solutions of the Navier-Stokes equations with the linear dependence of velocity components on two space variables

TLDR
In this article, a wide class of two-dimensional and three-dimensional steady-state and non-steady-state flows of a viscous incompressible fluid is considered, where the components of the velocity of a fluid linearly depend on two spatial coordinates.
Abstract
A wide class of two-dimensional and three-dimensional steady-state and non-steady-state flows of a viscous incompressible fluid is considered. It is assumed that the components of the velocity of a fluid linearly depend on two spatial coordinates. The three-dimensional Navier-Stokes equations in this case are reduced to a closed determining system that consists of six equations with partial derivatives of the third and second orders. A brief review of the known exact solutions of this system and the respective flows of a fluid (Couette-Poiseuille, Ekman, Stokes, Karman, and other flows) is given. The cases of reducing a determining system to one or two equations are described. Many new exact solutions of two-dimensional and three-dimensional nonstationary Navier-Stokes equations containing arbitrary functions and arbitrary parameters are derived. Periodic (both in spatial coordinates and in time) and some other solutions that are expressed in terms of elementary functions are described. The problems of the nonlinear stability of solutions are studied. A number of new hydrodynamic problems are considered. A general interpretation of the solutions as the main terms of the Taylor series expansion in terms of radial coordinates is given.

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Citations
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Journal ArticleDOI

A new class of exact solutions for three-dimensional thermal diffusion equations

TL;DR: In this paper, a new class of exact solutions has been obtained for three-dimensional equations of themal diffusion in a viscous incompressible liquid, which enables the description of the temperature and concentration distribution at the boundaries of a liquid layer by a quadratic law.
Journal ArticleDOI

Exact solutions of non-linear differential-difference equations of a viscous fluid with finite relaxation time

TL;DR: In this paper, the authors describe a one-dimensional flow arising from longitudinal periodic oscillations of a rigid plane and a two-dimensional periodic flow with pressure gradient near a fixed porous plate.
Journal ArticleDOI

New Class of Exact Solutions of Navier–Stokes Equations with Exponential Dependence of Velocity on Two Spatial Coordinates

TL;DR: In this article, a new class of exact solutions of nonlinear and linearized Navier-Stokes equations has been proposed, which generalize the well-known family of exact solution in which the velocity is linear in some coordinates.
Journal ArticleDOI

Towards understanding the algorithms for solving the Navier-Stokes equations

TL;DR: In this article, the authors present a review of featured works in the field of hydrodynamics with the main aim to clarify the ways of understanding the algorithms for solving the Navier-Stokes equations.
Journal ArticleDOI

Large-scale flows of viscous incompressible vortical fluid

TL;DR: In this article, an exact solution of the Navier-Stokes equations is given that describes the vorticity of a viscous incompressible liquid or gas, dissipative mediums, stationary shear counter-current of continuous vortical medium in the absence of the Coriolis field.
References
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Book

Boundary layer theory

TL;DR: The flow laws of the actual flows at high Reynolds numbers differ considerably from those of the laminar flows treated in the preceding part, denoted as turbulence as discussed by the authors, and the actual flow is very different from that of the Poiseuille flow.
Journal ArticleDOI

Flow past a stretching plate

TL;DR: In this paper, a plastischem material fliesst aus einem Spalt with einer Geschwindigkeit, die proportional zum Abstand vom Spalt ist.
Book ChapterDOI

On the Effect of the Internal Friction of Fluids on the Motion of Pendulums

TL;DR: In this paper, the reduction to a vacuum correction is considered, which is the only correction that is necessary for a simple pendulum to swing in a vacuum environment, due to the buoyancy of the fluid.
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