| 675 - 681 |
Letter to the editor: Cone partitioned plate (CPP) vs circular couette
Ravindranath S, Wang YY, Boukany P, Li X |
| 683 - 686 |
Response to: CPP vs circular couette
Hu YT |
| 687 - 706 |
Influence of pH and temperature on the rheology of aqueous quartz-bitumen suspensions
Gutierrez L, Pawlik M |
| 707 - 723 |
Effects of tube persistence length on dynamics of mildly entangled polymers
Qin J, Milner ST, Stephanou PS, Mavrantzas VG |
| 725 - 742 |
Time evolution of the structure of organoclay/polypropylene nanocomposites and application of the time-temperature superposition principle
Zouari R, Domenech T, Vergnes B, Peuvrel-Disdier E |
| 743 - 766 |
Viscoelastic properties of solutions of polystyrene melts and carbon dioxide: Analysis of a transient shear rheology approach
Handge UA, Altstadt V |
| 767 - 795 |
A visco-hyperelastic formulation for the rheology of immiscible blends
Yao DG |
| 797 - 822 |
Microrheology, microstructure, and aging of physically cross-linked poly(vinyl alcohol)/poly(ethylene glycol) blends
Yang N, Hutter JL, de Bruyn JR |
| 823 - 873 |
A full-chain constitutive model for bidisperse blends of linear polymers
Read DJ, Jagannathan K, Sukumaran SK, Auhl D |
| 875 - 923 |
The role of dilation and confining stresses in shear thickening of dense suspensions
Brown E, Jaeger HM |
| 925 - 939 |
The rheological characterization of algae suspensions for the production of biofuels
Adesanya VO, Vadillo DC, Mackley MR |
| 941 - 954 |
A simple accurate method for measuring viscosity of liquid metals at high temperatures
Elahi SH, Adelnia H, Shahverdi HR |
| 955 - 981 |
Using startup of steady shear flow in a sliding plate rheometer to determine material parameters for the purpose of predicting long fiber orientation
Ortman K, Baird D, Wapperom P, Whittington A |
