| 1335 - 1362 |
Stress diffusion in shear banding wormlike micelles
Fardin MA, Radulescu O, Morozov A, Cardoso O, Browaeys J, Lerouge S |
| 1363 - 1375 |
Adding salt to a surfactant solution: Linear rheological response of the resulting morphologies
Gaudino D, Pasquino R, Grizzuti N |
| 1377 - 1395 |
Microstructure and rheology of soft to rigid shear-thickening colloidal suspensions
Jamali S, Boromand A, Wagner N, Maia J |
| 1397 - 1417 |
Effect of extensional viscosity on cocontinuity of immiscible polymer blends
Hedegaard AT, Gu LL, Macosko CW |
| 1419 - 1430 |
Murray's law revisited: Quemada's fluid model and fractal trees
Moreau B, Mauroy B |
| 1431 - 1447 |
A rheological method for the determination of "super toughness point" of polymer blends: A blend system of nylon1212 with maleated poly(ethylene-octene)
Wang WJ, Song XL, Wei JM, Cao SK, Cao YX, Chen JZ, Wang JW |
| 1449 - 1486 |
Flows of suspensions of particles in yield stress fluids
Ovarlez G, Mahaut F, Deboeuf S, Lenoir N, Hormozi S, Chateau X |
| 1487 - 1505 |
A model for complex flows of soft glassy materials with application to flows through fixed fiber beds
Sarkar A, Koch DL |
| 1507 - 1525 |
Molecular based prediction of the extensional rheology of high molecular weight polystyrene dilute solutions: A hi-fidelity Brownian dynamics approach
Saadat A, Khomami B |
