1996
DOI: 10.1016/0927-7757(96)03621-7
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Network formation and its consequences for the physical behaviour of associating polymers in solution

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Cited by 121 publications
(161 citation statements)
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“…Examples of the complex rheological behavior exhibited by these polymeric networks include the ability to form highly viscous solutions at low to moderate concentrations, a linear viscoelastic response that closely resembles that of a perfect Maxwell fluid with a single relaxation time, 5,11,12 shear thickening at moderate shear rates in steady shear flow followed by marked shear thinning at high shear rate, [13][14][15][16][17][18][19] an Arrheniuslike temperature dependence of the zero-shear rate viscosity, 5,20 and a decrease in the critical shear rate at which onset of shear thickening occurs as the association strength or concentration increases or temperature decreases. 21 Recently, Ng et al 20 disputed the assertion of a single relaxation time suggested by Annable et al 5 and demonstrated that HEUR polymers in fact possesses a dual relaxation behavior.…”
Section: Introductionmentioning
confidence: 99%
“…Examples of the complex rheological behavior exhibited by these polymeric networks include the ability to form highly viscous solutions at low to moderate concentrations, a linear viscoelastic response that closely resembles that of a perfect Maxwell fluid with a single relaxation time, 5,11,12 shear thickening at moderate shear rates in steady shear flow followed by marked shear thinning at high shear rate, [13][14][15][16][17][18][19] an Arrheniuslike temperature dependence of the zero-shear rate viscosity, 5,20 and a decrease in the critical shear rate at which onset of shear thickening occurs as the association strength or concentration increases or temperature decreases. 21 Recently, Ng et al 20 disputed the assertion of a single relaxation time suggested by Annable et al 5 and demonstrated that HEUR polymers in fact possesses a dual relaxation behavior.…”
Section: Introductionmentioning
confidence: 99%
“…The reversible junctions in transient networks typically contain areas of hydrophobic associations, [7][8][9][10] hydrogen bonding, [11][12][13][14][15][16][17] metal-ligand interactions, 18,19 or ionic associations. 20,21 In many cases such junctions are poorly defined aggregates with unknown association strength and kinetics, but in a few transient network materials bulk properties have been directly correlated to defined polymer microstructure or well-characterized reversible interactions leading to important insights into the properties of these systems.…”
Section: Introductionmentioning
confidence: 99%
“…The dramatic change in rheology is due to the propagation of stress through the associative network. 23 HEUR bridges can propagate stress whereas HEURs in loop and dangling configurations cannot. 23 When stress is applied, bridges are extended, contracted, formed, broken, and reformed.…”
Section: Rheologymentioning
confidence: 99%
“…23 HEUR bridges can propagate stress whereas HEURs in loop and dangling configurations cannot. 23 When stress is applied, bridges are extended, contracted, formed, broken, and reformed. 8,23,24 The system remains as disordered as before and shows Newtonian behavior 8,23,24 ( Figure 5).…”
Section: Rheologymentioning
confidence: 99%
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