| 1315 - 1324 |
Stress relaxation of entangled ring polymer chains in a linear matrix
Hou JX |
| 1325 - 1341 |
Rheology of thermoplastic vulcanizates (TPVs)
Ghahramani N, Iyer KA, Doufas AK, Hatzikiriakos SG |
| 1343 - 1356 |
Effect of nitrogen doping on medium-amplitude oscillatory shear (MAOS) response of nanotube/polyvinylidene fluoride nanocomposites: Molecular simulations, rheology, and broadband electrical conductivity
Sadeghi S, Arjmand M, Navas IO, Sundararaj U |
| 1357 - 1371 |
Selective distribution of nanoparticles in immiscible blends: Effects on the morphology evolution and rheology in quiescent annealing, shear and extensional flow
Zhu XY, Kong MQ, Lv YD, Huang YJ, Li GX |
| 1373 - 1378 |
Chain tension reduces monomer friction in simulated polymer melts
Bobbili SV, Milner ST |
| 1379 - 1389 |
Rheology of crystallizing LLDPE
Andreev M, Nicholson DA, Kotula A, Moore JD, den Doelder J, Rutledge GC |
| 1391 - 1408 |
Shear induced demixing in bidisperse and polydisperse polymer blends: Predictions from a multifluid model
Peterson JD, Fredrickson GH, Leal LG |
| 1409 - 1424 |
The weakly nonlinear response and nonaffine interpretation of the Johnson-Segalman/Gordon-Schowalter model
Ramlawi N, Bharadwaj NA, Ewoldt RH |
| 1425 - 1438 |
Rheology of end-linking polydimethylsiloxane networks filled with silica
Xu HL, Ding L, Song YH, Wang WJ |
| 1439 - 1453 |
General fractional models for linear viscoelastic characterization of asphalt cements
Cao W |
| 1455 - 1464 |
Temperature, time, pressure, and CO2 concentration dependence of rheological properties for poly(methyl methacrylate)/expanded graphite composites
Huang HX, Yu LM |
| 1465 - 1496 |
A full-chain tube-based constitutive model for living linear polymers
Peterson JD, Cates ME |
| 1497 - 1499 |
Comment on "A revisitation of generalized Newtonian fluids" [J. Rheol. 64, 493-504 (2020)]
Park JM |
| 1501 - 1524 |
Rheology discussions: The physics of dense suspensions
Jamali S, Del Gado E, Morris JF |
