2011
DOI: 10.1016/j.jnnfm.2010.11.007
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Pressure-driven flow of wormlike micellar solutions in rectilinear microchannels

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Cited by 39 publications
(40 citation statements)
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“…The nonlinear system of partial differential equations is solved by an adaptive domain decomposition spectral method. 27 For slow flow (i.e., for Wi below the critical value for linear instability), the concentration defect is damped and the steady state flow is the normal linear profile. We first consider two cases for Wi = 10, which is within the linear instability window for our chosen model parameters.…”
Section: -5mentioning
confidence: 99%
“…The nonlinear system of partial differential equations is solved by an adaptive domain decomposition spectral method. 27 For slow flow (i.e., for Wi below the critical value for linear instability), the concentration defect is damped and the steady state flow is the normal linear profile. We first consider two cases for Wi = 10, which is within the linear instability window for our chosen model parameters.…”
Section: -5mentioning
confidence: 99%
“…This issue has recently been considered in detail using numerical simulation [Cromer et al (2010); Nghe et al (2010)]. …”
Section: B Microscale Shear Flowsmentioning
confidence: 99%
“…At higher W i, however, the retardance along the channel centerline is finite indicating non-zero normal stress difference along the center of the channel. The increased contribution of elastic stresses even in regions of low shear rate near the channel centerline can be rationalized by the possibility of diffusion of elastic stresses due to the importance of non-local effects that have been documented in the microfluidic flows of other complex fluids [Masselon et al (2008)], and recently studied numerically [Cromer et al (2010)]. …”
Section: Background Corrected Birefringence Profilesmentioning
confidence: 99%
“…The non-local nature of the flow curve is caused by diffusion of more highly stressed micellar species to regions of lower stress, which can be significant because the small gap width in the microfluidic device (99.6 µm) results in large spatial gradients in the stress field. In this regime the flow is no longer truly determined by the local conditions, since the diffusion gives rise to stress boundary layers [52], which are typically on the order of δ ∼ 10 µm, thereby altering the resulting stress vs. shear rate relationship. This has been documented for this CPyCl/NaSal system by Ober et al [24].…”
Section: Introductionmentioning
confidence: 99%