2005
DOI: 10.1142/s0218202505000686
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Steady Stokes Flows With Threshold Slip Boundary Conditions

Abstract: We prove the existence, uniqueness and continuous dependence on the data of weak solutions to boundary-value problems that model steady flows of incompressible Newtonian fluids with wall slip in bounded domains. The flows satisfy the Stokes equations and a nonlinear slip boundary condition: for slip to occur, the magnitude of the tangential traction must exceed a prescribed threshold, which is independent of the normal stress, and where slip occurs the tangential traction is equal to a prescribed, possibly non… Show more

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Cited by 57 publications
(37 citation statements)
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“…Equations (2.1) and (2.2) are supplemented by nonlinear slip boundary of friction type, which is the main modeling assumption in this work. It should be pointed out that such boundary conditions have already been considered in [43,44]. Hence we will just state the mathematical equations governing this phenomenon as the physical merits of such model have been discussed elsewhere (see particularly [43]).…”
Section: Preliminaries and Weak Formulationsmentioning
confidence: 99%
See 3 more Smart Citations
“…Equations (2.1) and (2.2) are supplemented by nonlinear slip boundary of friction type, which is the main modeling assumption in this work. It should be pointed out that such boundary conditions have already been considered in [43,44]. Hence we will just state the mathematical equations governing this phenomenon as the physical merits of such model have been discussed elsewhere (see particularly [43]).…”
Section: Preliminaries and Weak Formulationsmentioning
confidence: 99%
“…It should be pointed out that such boundary conditions have already been considered in [43,44]. Hence we will just state the mathematical equations governing this phenomenon as the physical merits of such model have been discussed elsewhere (see particularly [43]). So, we assume that the boundary of Ω, say, ∂Ω is made of two components S and Γ, and it is required that ∂Ω = S ∪ Γ, with S ∩ Γ = ∅.…”
Section: Preliminaries and Weak Formulationsmentioning
confidence: 99%
See 2 more Smart Citations
“…On S, we first assume the impermeability condition v N = v · n = 0 on S, (1.4) where n is the outward unit normal on the boundary ∂Ω, and v N is the normal component of the velocity, while v τ = v − v N n is its tangential component. In addition to (1.4) we also impose on S, a "friction type" boundary condition [5,6,7,8,16], which is the main ingredient of this work. The "friction type" boundary condition can be formulated with the knowledge of a positive function g : S −→ (0, ∞) called threshold slip or barrier function, and the use of sub-differential to link quantities of interest.…”
Section: Introduction We Consider Steady Flows Of Incompressible Vismentioning
confidence: 99%