565 - 587 |
Rheological experiments at constant stress as efficient method to characterize polymeric materials Munstedt H |
589 - 605 |
Strain hardening of molten thermoplastic polymers reinforced with poly(tetrafluoroethylene) nanofibers Jurczuk K, Galeski A, Piorkowska E |
607 - 633 |
Modeling of the blood rheology in steady-state shear flows Apostolidis AJ, Beris AN |
635 - 658 |
Large amplitude oscillatory shear and uniaxial extensional rheology of blends from linear and long-chain branched polyethylene and polypropylene Ahirwal D, Filipe S, Neuhaus I, Busch M, Schlatter G, Wilhelm M |
659 - 679 |
Squeeze flow behaviors of magnetorheological plastomers under constant volume Xu YG, Gong XL, Liu TX, Xuan SH |
681 - 721 |
A mesoscopic simulation method for predicting the rheology of semi-dilute wormlike micellar solutions Zou WZ, Larson RG |
723 - 736 |
Universality and speedup in equilibrium and nonlinear rheology predictions of the fixed slip-link model Andreev M, Feng HL, Yang L, Schieber JD |
737 - 757 |
Numerical prediction of nonlinear rheology of branched polymer melts Das C, Read DJ, Auhl D, Kapnistos M, den Doelder J, Vittorias I, McLeish TCB |
759 - 777 |
A generalized Oldroyd's model for non-Newtonian liquids with applications to a dilute emulsion of deformable drops Martin R, Zinchenko A, Davis R |
779 - 797 |
Inferring meaningful relaxation spectra from experimental data McDougall I, Orbey N, Dealy JM |
799 - 818 |
The two-dimensional flow of a foam through a constriction: Insights from the bubble model Lang VJ |