| 1167 - 1186 |
Cone-partitioned-plate geometry for the ARES rheometer with temperature control
Snijkers F, Vlassopoulos D |
| 1187 - 1203 |
Hard vs soft constraints in the full field reconstruction of incompressible flow kinematics from noisy scattered velocimetry data
Sadati M, Luap C, Kroger M, Ottinger HC |
| 1205 - 1218 |
Rheological properties of polymer composites with flexible fine fibers
Yokohara T, Nobukawa S, Yamaguchi M |
| 1219 - 1246 |
Loss of solutions in shear banding fluids driven by second normal stress differences
Skorski S, Olmsted PD |
| 1247 - 1270 |
Basic characteristics of uniaxial extension rheology: Comparing monodisperse and bidisperse polymer melts
Wang YY, Cheng SW, Wang SQ |
| 1271 - 1295 |
Effects of weak elasticity on the stability of high Reynolds number co-and counter-rotating Taylor-Couette flows
Dutcher CS, Muller SJ |
| 1297 - 1318 |
Rotational diffusion may govern the rheology of magnetic suspensions
Kuzhir P, Magnet C, Bossis G, Meunier A |
| 1319 - 1340 |
Numerical predictions of the viscosity of non-Brownian suspensions in the semidilute regime
Rexha G, Minale M |
| 1341 - 1373 |
Evaluation of molecular linear viscoelastic models for polydisperse H polybutadienes
Li SW, Park HE, Dealy JM |
| 1375 - 1397 |
Shear-induced phase separation (SIPS) with shear banding in solutions of cationic surfactant and salt
Thareja P, Hoffmann IH, Liberatore MW, Helgeson ME, Hu YT, Gradzielski M, Wagner NJ |
