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000058131 0247_ $$2DOI$$a10.1140/epje/i2006-10220-0
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000058131 084__ $$2WoS$$aChemistry, Physical
000058131 084__ $$2WoS$$aMaterials Science, Multidisciplinary
000058131 084__ $$2WoS$$aPhysics, Applied
000058131 084__ $$2WoS$$aPolymer Science
000058131 1001_ $$0P:(DE-Juel1)130920$$aRipoll, M.$$b0$$uFZJ
000058131 245__ $$aHydrodynamic screening of star polymers in shear flow
000058131 260__ $$aBerlin$$bSpringer$$c2007
000058131 300__ $$a349 - 354
000058131 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article
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000058131 440_0 $$01985$$aEuropean Physical Journal E$$v23$$x1292-8941
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000058131 520__ $$aThe mutual effects of the conformations of a star polymer in simple shear flow and the deformation of the solvent flow field are investigated by a hybrid mesoscale simulation technique. We characterize the flow field near the star polymer as a function of its functionality (arm number) f . A strong screening of the imposed flow is found inside the star polymer, which increases with increasing f . To elucidate the importance of hydrodynamic screening, we compare results for hydrodynamic and random solvents. The dependence of the polymer orientation angle on the Weissenberg number shows a power law behavior with super-universal exponent --independent of hydrodynamic and excluded-volume interactions. In contrast, the polymer rotation frequency changes qualitatively when hydrodynamic interactions are switched on.
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000058131 588__ $$aDataset connected to Web of Science, Pubmed
000058131 650_2 $$2MeSH$$aComputer Simulation
000058131 650_2 $$2MeSH$$aDiffusion
000058131 650_2 $$2MeSH$$aElasticity
000058131 650_2 $$2MeSH$$aMicrofluidics
000058131 650_2 $$2MeSH$$aMolecular Conformation
000058131 650_2 $$2MeSH$$aMovement
000058131 650_2 $$2MeSH$$aPhysics: methods
000058131 650_2 $$2MeSH$$aPolymers: chemistry
000058131 650_2 $$2MeSH$$aShear Strength
000058131 650_2 $$2MeSH$$aSoftware
000058131 650_2 $$2MeSH$$aSolvents: chemistry
000058131 650_2 $$2MeSH$$aStress, Mechanical
000058131 650_2 $$2MeSH$$aViscosity
000058131 650_7 $$00$$2NLM Chemicals$$aPolymers
000058131 650_7 $$00$$2NLM Chemicals$$aSolvents
000058131 650_7 $$2WoSType$$aJ
000058131 7001_ $$0P:(DE-Juel1)131039$$aWinkler, R. G.$$b1$$uFZJ
000058131 7001_ $$0P:(DE-Juel1)130665$$aGompper, G.$$b2$$uFZJ
000058131 773__ $$0PERI:(DE-600)2004003-9$$a10.1140/epje/i2006-10220-0$$gVol. 23, p. 349 - 354$$p349 - 354$$q23<349 - 354$$tThe @European physical journal / E$$v23$$x1292-8941$$y2007
000058131 8567_ $$uhttp://dx.doi.org/10.1140/epje/i2006-10220-0
000058131 909CO $$ooai:juser.fz-juelich.de:58131$$pVDB
000058131 9131_ $$0G:(DE-Juel1)FUEK414$$bMaterie$$kP54$$lKondensierte Materie$$vKondensierte Materie$$x0$$zentfällt   bis 2009
000058131 9141_ $$y2007
000058131 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed
000058131 9201_ $$0I:(DE-Juel1)VDB782$$d31.12.2010$$gIFF$$kIFF-2$$lTheorie der Weichen Materie und Biophysik$$x0
000058131 9201_ $$0I:(DE-Juel1)VDB1045$$gJARA$$kJARA-SIM$$lJülich-Aachen Research Alliance - Simulation Sciences$$x1
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