scholarly journals Exact solution for the layered convection of a viscous incompressible fluid at specified temperature gradients and tangential forces on the free boundary

2017 ◽  
Author(s):  
N. V. Burmasheva ◽  
E. Yu. Prosviryakov
Keyword(s):  
Exact Solution ◽  
Free Boundary ◽  
Incompressible Fluid ◽  
Viscous Incompressible Fluid ◽  
Temperature Gradients ◽  
Tangential Forces

scholarly journals Waves in Two Coaxial Elastic Cubically Nonlinear Shells with Structural Damping and Viscous Fluid Between Them

Symmetry ◽  
2020 ◽  
Vol 12 (3) ◽  
pp. 335
Author(s):  
Lev Mogilevich ◽  
Sergey Ivanov
Keyword(s):  
Exact Solution ◽  
Incompressible Fluid ◽  
Difference Scheme ◽  
Viscous Incompressible Fluid ◽  
Initial Conditions ◽  
Numerical Study ◽  
Fluid Motion ◽  
Structural Damping ◽  
The Difference ◽  
The Mathematical Model

This article investigates longitudinal deformation waves in physically nonlinear coaxial elastic shells containing a viscous incompressible fluid between them. The presence of a viscous incompressible fluid between the shells, as well as the influence of the inertia of the fluid motion on the amplitude and velocity of the wave, are taken into account. The mathematical model phenomenon is constructed by means of the method of two-scale asymptotic expansion. Structural damping in the shells and surrounding elastic media did not allow discovery of the exact solution of the problem of the deformation waves propagation. This leads to the need for numerical methods. A numerical study of the model constructed in the course of this work is carried out by using a difference scheme for the equation similar to the Crank–Nicholson scheme for the heat equation. In the absence of the structural damping and surrounding media influences, and under the similar initial conditions for both shells, the velocity and amplitude of the wave do not change. The result of the numerical experiment coincides with the exact solution, which is found in the case of the absence of the structural damping and surrounding media influences; therefore, the difference scheme is adequate to the generalized modified Korteweg–de Vries equations system. There is energy is transferred in the presence of the fluid, between the shells. The presence of inertia of the fluid motion leads to a decrease in the velocity of the deformation wave.

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