885 - 899 |
Stress relaxation of narrow molar mass distribution polystyrene following uniaxial extension Nielsen JK, Rasmussen HK, Hassager O |
901 - 912 |
Effect of particle aggregation on the magnetic and magnetorheological properties of magnetic suspensions Lopez-Lopez MT, Zugaldia A, Gomez-Ramirez A, Gonzalez-Caballero F, Duran JDG |
913 - 922 |
Double concentric cylinder geometry with slotted rotor to measure the yield stress of complex systems: A numerical study Zhu H, De Kee D |
923 - 940 |
Rheometric investigation on the temporal shear thickening of dilute micellar solutions of C-14-, C-16-, and C(18)TAB/NaSal Dehmoune J, Decruppe JP, Greffier O, Xu H |
941 - 955 |
Rheology of semidilute suspensions of rigid polystyrene ellipsoids at high Peclet numbers Bricker JM, Park HO, Butler JE |
957 - 980 |
Steady state measurements in stress plateau region of entangled polymer solutions: Controlled-rate and controlled-stress modes Ravindranath S, Wang SQ |
981 - 998 |
Biaxial extensional rheology of granular suspensions: The HBP (Herschel-Bulkley for Pastes) model Mascia S, Wilson DI |
999 - 1011 |
New method of forced-resonance measurement for the concentrated and large-viscous liquid in the low frequency range by torsion resonator Wang YZ, Xiong XM, Zhang JX |
1013 - 1025 |
Probing nonlinear rheology with inertio-elastic oscillations Yao NY, Larsen RJ, Weitz DA |
1027 - 1042 |
Elastic encapsulation in bicomponent stratified flow of viscoelastic fluids Yue PT, Zhou CF, Dooley J, Feng JJ |