| 485 - 497 |
The origin of stress-oscillation damping during start-up and reversal of torsional shearing of nematics
Mather PT, Pearson DS, Larson RG, Gu DF, Jamieson AM |
| 498 - 504 |
Smectic rheology
Colby RH, Ober CK, Gillmor JR, Connelly RW, Duong T, Galli G, Laus M |
| 505 - 512 |
Effect of molecular architecture on the electrorheological behavior of liquid crystal polymers in nematic solvents
Chiang YC, Jamieson AM, Campbell S, Lin YH, OSidocky N, Chien LC, Kawasumi M, Percec V |
| 513 - 523 |
Stress relaxation as a microstructural probe for immiscible polymer blends
Vinckier I, Mewis J, Moldenaers P |
| 524 - 533 |
Nonlinear rheology of a concentrated spherical silica suspension .2. Role of strain in shear-thickening
Watanabe H, Yao ML, Osaki K, Shikata T, Niwa H, Morishima Y |
| 534 - 543 |
Sticky dumbbells: from Hookean dumbbells to transient network
Palierne JF |
| 544 - 554 |
A constant-contour-length reptation model without independent alignment or consistent averaging approximations for chain retraction
Hua CC, Schieber JD, Andrews NC |
| 555 - 567 |
Extensional rheology of concentrated poly(ethylene oxide) solutions
Gauri V, Koelling KW |
| 568 - 578 |
Rheological characterization of polyethylene terephthalate resins using a multimode Phan-Tien-Tanner constitutive relation
Hatzikiriakos SG, Heffner G, Vlassopoulos D, Christodoulou K |
| 579 - 584 |
＇＇Fracture＇＇ phenomena in shearing flow of viscous liquids
Archer LA, Ternet D, Larson RG |
| 585 - 589 |
The ''decaying springs'' model for irreversibility in polymer melts
Buggisch H, Konig T |
