Local strong solution for a class of non-Newtonian fluids with heat-conducting and state function

2019 ◽  
Vol 60 (9) ◽  
pp. 091503
Author(s):  
Yunliang Zhang ◽  
Zhidong Guo
2015 ◽  
Vol 2015 ◽  
pp. 1-17
Author(s):  
Yunliang Zhang ◽  
Zhidong Guo

The aim of this paper is to discuss the model for a class of shear thickening fluids with non-Newtonian potential and heat-conducting. Existence and uniqueness of local strong solutions for the model are proved. In this paper, there exist two difficulties we have to overcome. One is the strong nonlinearity of the system. The other is that the state function is not fixed.


2006 ◽  
Vol 342 (3) ◽  
pp. 169-174 ◽  
Author(s):  
Mamadou Sy ◽  
Didier Bresch ◽  
Francisco Guillén-González ◽  
Jérôme Lemoine ◽  
Maria Angeles Rodríguez-Bellido

Author(s):  
Maoting Tong

In this paper we study solutions and drift homogenization for a class of viscous lake equations by using the method of semigroups of bounded operators. Suppose that the initial value i.e.,for some Hölder continuous function onwith smooth function value satisfying and Then the initial value problem (2) for viscous lake equations has a unique smooth local strong solution. Using this result we study the drift homogenization for three-dimensional stationary Stokes equation in the usual sense


Author(s):  
Matthias Hieber ◽  
Klaus Kress ◽  
Christian Stinner

AbstractConsider the classical Keller–Segel system on a bounded convex domain $$\varOmega \subset {\mathbb {R}}^3$$ Ω ⊂ R 3 . In contrast to previous works it is not assumed that the boundary of $$\varOmega $$ Ω is smooth. It is shown that this system admits a local, strong solution for initial data in critical spaces which extends to a global one provided the data are small enough in this critical norm. Furthermore, it is shown that this system admits for given T-periodic and sufficiently small forcing functions a unique, strong T-time periodic solution.


2018 ◽  
Vol 16 (05) ◽  
pp. 623-647 ◽  
Author(s):  
Xin Zhong

We study an initial boundary value problem for the nonhomogeneous heat conducting fluids with non-negative density. First of all, we show that for the initial density allowing vacuum, the strong solution exists globally if the gradient of viscosity satisfies [Formula: see text]. Then, under certain smallness condition, we prove that there exists a unique global strong solution to the 2D viscous nonhomogeneous heat conducting Navier–Stokes flows with variable viscosity. Our method relies upon the delicate energy estimates and regularity properties of Stokes system and elliptic equation.


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