595 - 618 |
Nonlinear time-dependent response of isotactic polypropylene Drozdov AD, Christiansen JD |
619 - 630 |
Strain hardening of various polyolefins in uniaxial elongational flow Gabriela C, Munstedt H |
631 - 642 |
Simultaneous dielectric and dynamic mechanical measurements on PVDF in the molten state: Study of the linear/nonlinear viscoelastic transition Gonnet JM, Guillet J, Sirakov I, Fulchiron R, Seytre G |
643 - 658 |
On the shear thickening flow of dilute CTAT worm-like micellar solutions Macias ER, Bautista F, Soltero JFA, Puig JE, Attane R, Manera O |
659 - 682 |
A model for large deformation of an ellipsoidal droplet with interfacial tension Jackson NE, Tucker CL |
683 - 699 |
Wall slip and extrudate distortion of three polymer melts Kalyon DM, Gevgilili H |
701 - 716 |
Large strain time dependent behavior of cheese Goh SM, Charalambides MN, Williams JG |
717 - 736 |
Separating the effects of sparse long-chain branching on rheology from those due to molecular weight in polyethylenes Doerpinghaus PJ, Baird DG |
737 - 757 |
Cyclic generation of wall slip at the exit of plane Couette flow Mizunuma H, Takagi H |
759 - 778 |
Rheology of sheared flexible fiber suspensions via fiber-level simulations Switzer LH, Klingenberg DJ |
779 - 793 |
Quantitative assessment of strain hardening of low-density polyethylene melts by the molecular stress function model Wagner MH, Yamaguchi M, Takahashi M |
795 - 807 |
Interfacial slip between polymer melts studied by confocal microscopy and rheological measurements Lam YC, Jiang L, Yue CY, Tam KC, Li L |
809 - 818 |
Definitions of entanglement spacing and time constants in the tube model Larson RG, Sridhar T, Leal LG, McKinley GH, Likhtman AE, McLeish TCB |