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000858755 037__ $$aFZJ-2018-07600
000858755 041__ $$aEnglish
000858755 1001_ $$0P:(DE-Juel1)173831$$aPark, Gunwoo$$b0$$eCorresponding author$$ufzj
000858755 1112_ $$aAnnual European Rheology Conference 2018$$cSorrento$$d2018-04-17 - 2018-04-20$$gAERC2018$$wItaly
000858755 245__ $$aExploring Shear Thickening of Telechelic Associating Polymers through Stochastic Simulations
000858755 260__ $$c2018
000858755 3367_ $$033$$2EndNote$$aConference Paper
000858755 3367_ $$2DataCite$$aOther
000858755 3367_ $$2BibTeX$$aINPROCEEDINGS
000858755 3367_ $$2DRIVER$$aconferenceObject
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000858755 3367_ $$0PUB:(DE-HGF)6$$2PUB:(DE-HGF)$$aConference Presentation$$bconf$$mconf$$s1546440091_934$$xAfter Call
000858755 520__ $$aHydrophobically modified exthoxylated urethane (HEUR) is one of the most popular examples of telechelic associating polymer. In a certain range of HEUR concentration in aqueous solution, (i) linear viscoelasticity follows a single-Maxwellian behavior with a characteristic time controlled by the network relaxation due to association/dissociation kinetics. In simple shear flows, HEUR systems often (ii) exhibit strain hardening in the transient startup when the shear rate exceeds the reciprocal relaxation time, and (iii) at steady state deviate from the Cox-Merz rule, deviations including (iv) a shear-thickening phenomenon. Recently, Park and Ianniruberto [1] suggested a new stochastic simulation to describe the complex rheological behavior listed in (i-iv). The results indicate that finite extensibility effects are mostly responsible for the strain hardening, while deviations from the Cox-Merz rule are due to the persistence of bridge chains. However, the detailed mechanism behind the shear thickening is still unclear. In this study, we show additional observables by using the same simulation method for a better understanding of the shear-thickening phenomenon. Furthermore, we extend the range of the parameter space explored in [1] by examining larger (and more reasonable) values of the ratio between the loop dissociation time and the Brownian diffusion time of flower-like micelles. [1] G. W. Park and G. Ianniruberto, J. Rheol. 61, 1293 (2017)
000858755 536__ $$0G:(DE-HGF)POF3-551$$a551 - Functional Macromolecules and Complexes (POF3-551)$$cPOF3-551$$fPOF III$$x0
000858755 536__ $$0G:(GEPRIS)221475706$$aSFB 985 B06 - Kontinuierliche Trennung und Aufkonzentrierung von Mikrogelen (B06) (221475706)$$c221475706$$x1
000858755 65027 $$0V:(DE-MLZ)SciArea-180$$2V:(DE-HGF)$$aMaterials Science$$x0
000858755 65027 $$0V:(DE-MLZ)SciArea-210$$2V:(DE-HGF)$$aSoft Condensed Matter$$x1
000858755 65017 $$0V:(DE-MLZ)GC-1602-2016$$2V:(DE-HGF)$$aPolymers, Soft Nano Particles and Proteins$$x0
000858755 7001_ $$0P:(DE-HGF)0$$aIanniruberto, G.$$b1
000858755 8564_ $$uhttps://juser.fz-juelich.de/record/858755/files/presentation%20file.pdf$$yOpenAccess
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000858755 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)173831$$aForschungszentrum Jülich$$b0$$kFZJ
000858755 9101_ $$0I:(DE-HGF)0$$6P:(DE-HGF)0$$aExternal Institute$$b1$$kExtern
000858755 9131_ $$0G:(DE-HGF)POF3-551$$1G:(DE-HGF)POF3-550$$2G:(DE-HGF)POF3-500$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bKey Technologies$$lBioSoft – Fundamentals for future Technologies in the fields of Soft Matter and Life Sciences$$vFunctional Macromolecules and Complexes$$x0
000858755 9141_ $$y2018
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000858755 9201_ $$0I:(DE-Juel1)ICS-3-20110106$$kICS-3$$lWeiche Materie $$x0
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