2007
DOI: 10.1209/0295-5075/81/28002
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Cyclic motion and inversion of surface flow direction in a dense polymer brush under shear

Abstract: Using molecular simulations, we study the properties of a polymer brush in contact with an explicit solvent under Couette and Poiseuille flow. The solvent is comprised of chemically identical chains. We present evidence that individual, unentangled chains in the dense brush exhibit cyclic, tumbling motion and non-Gaussian fluctuations of the molecular orientations similar to the behaviour of isolated tethered chains in shear flow. The collective molecular motion gives rise to an inversion of hydrodynamic flow … Show more

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Cited by 49 publications
(84 citation statements)
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“…We also checked the existence of cyclic motion dynamics in semiflexible chains under shear, found in previous works for fully flexible isolated grafted chains and polymer brushes [20,22]. We analysed the effect of stiffness in the mechanism of cyclic motion, whose origin is attributed to spontaneous fluctuations of the polymer chains towards regions of higher velocity in the liquid.…”
Section: B Flow Propertiesmentioning
confidence: 84%
See 1 more Smart Citation
“…We also checked the existence of cyclic motion dynamics in semiflexible chains under shear, found in previous works for fully flexible isolated grafted chains and polymer brushes [20,22]. We analysed the effect of stiffness in the mechanism of cyclic motion, whose origin is attributed to spontaneous fluctuations of the polymer chains towards regions of higher velocity in the liquid.…”
Section: B Flow Propertiesmentioning
confidence: 84%
“…The cyclic dynamics is indeed reduced upon increase of the chain stiffness and vanishes completely for the stiffest chains (k b = 80ε). A more comprehensive characterization of the effect and its consequences for flow inversion [20,22] could be an interesting future study.…”
Section: B Flow Propertiesmentioning
confidence: 99%
“…A relatively large number of experimental investigations (see Klein, Perahia & Warburg 1991; Klein et al 1994; Baker et al 2000; Ivkov et al 2001; Anastassopoulos et al 2006), analytical studies (see e.g. Rabin & Alexander 1990; Milner 1991 a ; Barrat 1992; Kumaran 1993; Sevick & Williams 1994; Aubouy, Harden & Cates 1996; Harden & Cates 1996) as well as computational simulations (see Lai & Binder 1993; Peters & Tildesley 1995; Miao, Guo & Zuckermann 1996; Grest 1996, 1999; Doyle, Shaqfeh & Gast 1997; Irfachsyad, Tildesley & Malfreyt 2002; Wijmans & Smit 2002; Kreer, Binder & Muser 2003; Huang, Wang & Laradji 2006; Pastorino et al 2006; Müller & Pastorino 2008) have addressed the dynamics of polymer brushes exposed to fluid shear flow. However, it is still not well understood whether the polymer brushes show conformational changes, that is, swelling or collapse of the brush height at a certain value of shear rate.…”
Section: Introductionmentioning
confidence: 99%
“…For instance, this choice gives rise to a discontinuous non-bonded force, −∂H nb ({r i,s })/∂r j,t that acts on the t th segment of polymer j . The first-order assignment function, which is defined by [17,130] Π (1) …”
Section: Non-bonded Interactions: Collocation Grid Versus Weighting Fmentioning
confidence: 99%
“…Thus we can choose w 1,1 = 0 and match the pre-weighting factors at the interval boundaries, w p,mp = w p+1,1 . The partition function of the simulation is given by [130] …”
Section: Reversible Transformation Of Self-assembled Morphologiesmentioning
confidence: 99%