Negative Orlicz–Sobolev norms and strongly nonlinear systems in fluid mechanics (original) (raw)

Monotonicity methods in generalized Orlicz spaces for a class of non-Newtonian fluids

Mathematical Methods in the Applied Sciences, 2009

Communicated by M. Lachowicz The paper concerns existence of weak solutions to the equations describing a motion of some non-Newtonian fluids with non-standard growth conditions of the Cauchy stress tensor. Motivated by the fluids of strongly inhomogeneous behavior and having the property of rapid shear thickening, we observe that the L p framework is not suitable to capture the described situation. We describe the growth conditions with the help of general x-dependent convex function. This formulation yields the existence of solutions in generalized Orlicz spaces. As examples of motivation for considering non-Newtonian fluids in such spaces, we recall the electrorheological fluids, magnetorheological fluids, and shear thickening fluids. The existence of solutions is established by the generalization of the classical Minty method to non-reflexive spaces. The result holds under the assumption that the lowest growth of the Cauchy stress is greater than the critical exponent q = (3d+2) / (d+2), where d is for space dimension. The restriction on the exponent q is forced by the convective term.

Unsteady flows of heat-conducting non-Newtonian fluids in Musielak–Orlicz spaces

Nonlinearity, 2018

Our purpose is to show the existence of weak solutions for unsteady flow of non-Newtonian incompressible nonhomogeneous, heat-conducting fluids with generalised form of the stress tensor without any restriction on its upper growth. Motivated by fluids of nonstandard rheology we focus on the general form of growth conditions for the stress tensor which makes anisotropic Musielak-Orlicz spaces a suitable function space for the considered problem. We do not assume any smallness condition on initial data in order to obtain long-time existence. Within the proof we use monotonicity methods, integration by parts adapted to nonreflexive spaces and Young measure techniques.

On steady flow of non-Newtonian fluids with frictional boundary conditions in reflexive Orlicz spaces

Nonlinear Analysis-real World Applications, 2018

A stationary viscous incompressible non-Newtonian fluid flow problem is studied with a non-polynomial growth of the extra (viscous) part of the Cauchy stress tensor together with a multivalued nonmonotone frictional boundary condition described by the Clarke subdifferential. We provide an abstract result on existence of solution to a subdifferential operator inclusion and a hemivariational inequality in the reflexive Orlicz-Sobolev space setting modeling the flow phenomenon. We establish the existence result, and under additional conditions, also uniqueness of a weak solution in the Orlicz-Sobolev space to the flow problem.

Bounded solutions of unilateral problems for strongly nonlinear equations in Orlicz spaces

Electronic Journal of Qualitative Theory of Differential Equations, 2013

In this paper, we prove the existence of bounded solutions of unilateral problems for strongly nonlinear equations whose principal part having a growth not necessarily of polynomial type and a degenerate coercivity, the lower order terms do not satisfy the sign condition and appropriate integrable source terms. We do not impose the ∆ 2-condition on the considered N-functions defining the Orlicz-Sobolev functional framework.

Nonlinear Boundary Value Problems via Minimization on Orlicz-Sobolev Spaces

We develop arguments on convexity and minimization of energy functionals on Orlicz-Sobolev spaces to investigate existence of solution to the equation displaystyle−mboxdiv(phi(∣nablau∣)nablau)=f(x,u)+hmboxinOmega\displaystyle -\mbox{div} (\phi(|\nabla u|) \nabla u) = f(x,u) + h \mbox{in} \Omegadisplaystylemboxdiv(phi(nablau)nablau)=f(x,u)+hmboxinOmega under Dirichlet boundary conditions, where OmegasubsetbfRN\Omega \subset {\bf R}^{N}OmegasubsetbfRN is a bounded smooth domain, phi:(0,infty)longrightarrow(0,infty)\phi : (0,\infty)\longrightarrow (0,\infty)phi:(0,infty)longrightarrow(0,infty) is a suitable continuous function and f:OmegatimesbfRtobfRf: \Omega \times {\bf R} \to {\bf R}f:OmegatimesbfRtobfR satisfies the Carath\'eodory conditions, while hhh is a measure.