Abstract

The initial‐boundary value problem for the mathematical model of low‐concentrated aqueous polymer solutions is considered. For this initial‐boundary value problem a concept of a weak solution is introduced and the existence theorem for such solutions is proved.

Highlights

  • The initial-boundary value problem for the mathematical model of low-concentrated aqueous polymer solutions is considered. For this initial-boundary value problem a concept of a weak solution is introduced and the existence theorem for such solutions is proved

  • The study of fluid motion is a source of a large number of mathematical problems

  • In the given system v(x,t) is the velocity vector of the particle at a point x at an instant t; p = p(x,t) is the pressure of the fluid at a point x at an instant t; f = f (x,t) is the vector of body forces acting on the fluid; σ = (σij(x)) is the deviator of the stress tensor

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Summary

Introduction

Motion of an incompressible fluid in a bounded domain Ω ⊂ Rn on a time interval [0, T], (T < ∞) is described by the following system of equations in Cauchy’s form [3]:. (x, t) ∈ Ω × [0, T], div v = 0, (x, t) ∈ Ω × [0, T]. By Div σ we denote the vector of divergences of columns of the matrix σ. The system of (1.1) describes formally the motion of all kinds of fluids. To complete the given system one usually uses various relations between the deviator of the stress tensor σ and the strain rate tensor Ᏹ = (Ᏹij), Ᏹi j.

Mathematical model of polymer solutions
Principal notations and functional spaces
Statement of the problem and the main result
Properties of operators L and K
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