Pressure-Driven Flow of Wormlike Micellar Solutions in Rectilinear Microchannels
By Michael Cromer, L. Pamela Cook, Gareth H. McKinley
In
this paper the inhomogeneous response of the (two species) VCM model
(Vasquez et al., A network scission model for wormlike micellar
solutions I: model formulation and homogeneous flow predictions. J.
Non-Newtonian Fluid Mech. 144:122-139, 2007) is examined in steady
rectilinear pressure-driven flow through a planar channel. This
microstructural network model incorporates elastically active network
connections that break and reform mimicking the behavior of
concentrated wormlike micellar solutions. The constitutive model, which
includes non-local effects arising from Brownian motion and from the
coupling between the stress and the microstructure (finite length
worms),
consists of a set of coupled nonlinear partial differential
equations describing the two micellar species (a long species ‘A’ and a
shorter species ‘B’) which relax due to reptative and Rouse-like
mechanisms as well as rupture of the long micellar chains. In
pressure-driven flow, the velocity profile predicted by the VCM model
deviates from the regular parabolic profile expected for a Newtonian
fluid and exhibits a complex spatial structure. An apparent slip layer
develops near the wall as a consequence of the microstructural boundary
conditions and the shear-induced diffusion and rupture of the micellar
species. Above a critical pressure drop, the flow exhibits shear
banding with a high shear rate band located near the channel walls.
This pressure-driven shear banding transition or ‘spurt’ has been
observed experimentally in macroscopic and microscopic channel
flow experiments. The detailed structure of the shear banding
profiles and the resulting flow curves predicted by the model depend on
the magnitude of the dimensionless diffusion parameter. For small
channel dimensions, the solutions exhibit ‘non-local’ effects that are
consistent with very recent experiments in microfluidic geometries
(Masselon et al., Influence of boundary conditions and confinement on
non local effects in flows of wormlike micellar systems. Physical
Review E, 81:021502, 2010).