The no-slip boundary condition in fluid mechanics

Resonance ◽  
2004 ◽  
Vol 9 (5) ◽  
pp. 61-71 ◽  
Author(s):  
Sandeep Prabhakara ◽  
M. D. Deshpande
Resonance ◽  
2004 ◽  
Vol 9 (4) ◽  
pp. 50-60 ◽  
Author(s):  
Sandeep Prabhakara ◽  
M. D. Deshpande

Soft Matter ◽  
2015 ◽  
Vol 11 (40) ◽  
pp. 7851-7856 ◽  
Author(s):  
Savvas G. Hatzikiriakos

The classical no-slip boundary condition of fluid mechanics is not always a valid assumption for the flow of several classes of complex fluids including polymer melts, their blends, polymer solutions, microgels, glasses, suspensions and pastes.


2005 ◽  
Vol 15 (03) ◽  
pp. 343-374 ◽  
Author(s):  
GUY BAYADA ◽  
NADIA BENHABOUCHA ◽  
MICHÈLE CHAMBAT

A thin micropolar fluid with new boundary conditions at the fluid-solid interface, linking the velocity and the microrotation by introducing a so-called "boundary viscosity" is presented. The existence and uniqueness of the solution is proved and, by way of asymptotic analysis, a generalized micropolar Reynolds equation is derived. Numerical results show the influence of the new boundary conditions for the load and the friction coefficient. Comparisons are made with other works retaining a no slip boundary condition.


Author(s):  
Joris C. G. Verschaeve

By means of the continuity equation of the incompressible Navier–Stokes equations, additional physical arguments for the derivation of a formulation of the no-slip boundary condition for the lattice Boltzmann method for straight walls at rest are obtained. This leads to a boundary condition that is second-order accurate with respect to the grid spacing and conserves mass. In addition, the boundary condition is stable for relaxation frequencies close to two.


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