Abstract

In this note, in 2D and 3D smooth bounded domain, we show the existence of strong solution for generalized Navier-Stokes equation modeling bypx-power law with Dirichlet boundary condition under the restriction3n/n+2n+2<px<2n+1/n−1. In particular, if we neglect the convective term, we get a unique strong solution of the problem under the restriction2n+1/n+3<px<2n+1/n−1, which arises from the nonflatness of domain.

Highlights

  • We consider the steady flows of nonNewtonian fluids in Rn, n = 2, 3, which is modeled by the following system: 8 >>>

  • Global higher differentiability for weak solutions to the problem (1) with pðxÞ = const have been studied by several authors; for example, see [8,9,10,11,12,13,14,15,16,17,18,19] under the condition f ∈ Lp∧′ðΩÞ with p∧′ = p/ðp − 1Þ and p ≔ min fp, 2g

  • Global higher differentiability of weak solution to the problem (1) in 3D smooth domain is studied by us in [20] by using a global higher integrability condition, which holds under the condition f ∈ Lαp∧′ðxÞðΩÞ, where p∧′ ðxÞ = ðpðxÞÞ/ðpðxÞ − 1Þ, pðxÞ ≔ min fpðxÞ, 2g, and α > 1

Read more

Summary

Introduction

Global higher differentiability for weak solutions to the problem (1) with pðxÞ = const have been studied by several authors; for example, see [8,9,10,11,12,13,14,15,16,17,18,19] under the condition f ∈ Lp∧′ðΩÞ with p∧′ = p/ðp − 1Þ and p ≔ min fp, 2g It was first established in [8] by Beirao da Veiga. Global higher differentiability of weak solution to the problem (1) in 3D smooth domain is studied by us in [20] by using a global higher integrability condition, which holds under the condition f ∈ Lαp∧′ðxÞðΩÞ, where p∧′ ðxÞ = ðpðxÞÞ/ðpðxÞ − 1Þ, pðxÞ ≔ min fpðxÞ, 2g, and α > 1 This is slightly stronger rather than the standard condition f ∈ Lp∧′ðΩÞ for the case p = const.

Preliminaries
The Proof of Main Results
The Proof of Theorem 1 without the Convective Term
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.