Weakly nonlinear analysis of viscous instability in flow past a neo-Hookean surface

Chokshi, Paresh ; Kumaran, V. (2008) Weakly nonlinear analysis of viscous instability in flow past a neo-Hookean surface Physical Review E, 77 (5). 056303_1-056303_15. ISSN 1063-651X

Full text not available from this repository.

Official URL: http://pre.aps.org/abstract/PRE/v77/i5/e056303

Related URL: http://dx.doi.org/10.1103/PhysRevE.77.056303

Abstract

We analyze the stability of the plane Couette flow of a Newtonian fluid past an incompressible deformable solid in the creeping flow limit where the viscous stresses in the fluid (of the order ηfV/R) are comparable with the elastic stresses in the solid (of the order G). Here, ηf is the fluid viscosity, V is the top-plate velocity, R is the channel width, and G is the shear modulus of the elastic solid. For (ηfV/GR)=O(1), the flexible solid undergoes finite deformations and is, therefore, appropriately modeled as a neo-Hookean solid of finite thickness which is grafted to a rigid plate at the bottom. Both linear as well as weakly nonlinear stability analyses are carried out to investigate the viscous instability and the effect of nonlinear rheology of solid on the instability. Previous linear stability studies have predicted an instability as the dimensionless shear rate Γ=(ηfV/GR) is increased beyond the critical value Γc. The role of viscous dissipation in the solid medium on the stability behavior is examined. The effect of solid-to-fluid viscosity ratio ηr on the critical shear rate Γc for the neo-Hookean model is very different from that for the linear viscoelastic model. Whereas the linear elastic model predicts that there is no instability for H<√ηr, the neo-Hookean model predicts an instability for all values of ηr and H. The value of Γc increases upon increasing ηr from zero up to √ηr/H≈1, at which point the value of Γc attains a peak and any further increase in ηr results in a decrease in Γc. The weakly nonlinear analysis indicated that the bifurcation is subcritical for most values of H when ηr=0. However, upon increasing ηr, there is a crossover from subcritical to supercritical bifurcation for √ηr/H≈1. Another crossover is observed as the bifurcation again becomes subcritical at large values of ηr. A plot in H versus √ηr/H space is constructed to mark the regions where the bifurcation is subcritical and supercritical. The equilibrium amplitude and some physical quantities of interest, such as the total strain energy of the disturbance in the srolid, have been calculated, and the effect of parameters H, ηr, and interfacial tension on these quantities are analyzed.

Item Type:Article
Source:Copyright of this article belongs to American Physical Society.
ID Code:18570
Deposited On:17 Nov 2010 09:30
Last Modified:06 Jun 2011 04:44

Repository Staff Only: item control page