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Published in 2019 at "Journal of Mathematical Sciences"
DOI: 10.1007/s10958-019-04264-3
Abstract: A system of equations describing the motion of fluids of Maxwell type is considered:∂∂tυ+υ⋅∇υ−∫0tKt−τdτ+∇p=fxt,diυυ=0.$$ \frac{\partial }{\partial t}\upsilon +\upsilon \cdot \nabla \upsilon -\underset{0}{\overset{t}{\int }}K\left(t-\tau \right) d\tau +\nabla p=f\left(x,t\right),\kern0.5em di\upsilon\;\upsilon =0. $$ Here K(t) is an exponential…
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Keywords:
type maxwell;
weak solutions;
maxwell flows;
solutions hopf ... See more keywords