345 - 366 |
Influence of stretching induced self-concentration and self-dilution on coil-stretch hysteresis and capillary thinning of unentangled polymer solutions Prabhakar R, Gadkari S, Gopesh T, Shaw MJ |
367 - 378 |
Rheological diagnostic tools for state transitions McKenzie R, Vlassopoulos D |
379 - 392 |
Maximum likelihood estimation for single particle, passive microrheology data with drift Mellnik JWR, Lysy M, Vasquez PA, Pillai NS, Hill DB, Cribb J, McKinley SA, Forest MG |
393 - 406 |
Effects of instrument and fluid inertia in oscillatory shear in rotational rheometers Lauger J, Stettin H |
407 - 418 |
Oscillatory squeeze flow for the study of linear viscoelastic behavior Wingstrand SL, Alvarez NJ, Hassager O, Dealy JM |
419 - 432 |
Confined tube flow of low viscosity emulsions: Effect of matrix elasticity Preziosi V, Tomaiuolo G, Fenizia M, Caserta S, Guido S |
433 - 450 |
Dynamic shear rheology of a thixotropic suspension: Comparison of an improved structure-based model with large amplitude oscillatory shear experiments Armstrong MJ, Beris AN, Rogers SA, Wagner NJ |
451 - 463 |
Viscoelasticity and nonlinear simple shear flow behavior of an entangled asymmetric exact comb polymer solution Snijkers F, Kirkwood KM, Vlassopoulos D, Leal LG, Nikopoulou A, Hadjichristidis N, Coppola S |
465 - 471 |
Stress relaxation following uniaxial extension of polystyrene melt and oligomer dilutions Huang Q, Rasmussen HK |
473 - 489 |
Normal force controlled rheology applied to agar gelation Mao B, Divoux T, Snabre P |
491 - 502 |
Viscoelastic properties of polyacrylamide solutions from creep ringing data Goudoulas TB, Germann N |
503 - 515 |
Axial annular flow of a viscoplastic microgel with wall slip Ortega-Avila JF, Perez-Gonzalez J, Marin-Santibanez BM, Rodriguez-Gonzalez F, Aktas S, Malik M, Kalyon DM |
517 - 529 |
Bond rupture between colloidal particles with a depletion interaction Whitaker KA, Furst EM |