The torque on a rotating n -bladed vane in a newtonian fluid or linear elastic medium

The vane is an n -bladed paddle which rotates with angular velocity Ω in a linear viscoelastic fluid. The blades, of zero thickness, are equally spaced around the axis r = 0, and extend from r = 0 to r = a . The problem is assumed two-dimensional. The stress and fluid velocity (or material displacements) are obtained by a Wiener–Hopf technique for the case of a no-slip boundary condition on the surface of the blades, and for the case of zero shear stress on the blades. The torque M (per unit length) required to rotate the vane in an incompressible newtonian fluid of viscosity μ may be approximated as M ≈ 4π μa 2 Ω (1 – n –1 ) to within 1% for the no-slip boundary condition; with the slip boundary condition the same expression is accurate to within 4%. Results are also given for the angular dependence and strength of the stress singularity at the tip of each blade.

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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