75 - 83 |
Mesohydrodynamics of membrane suspensions Gu JF, Grmela M, Bousmina M |
84 - 87 |
Fluid boundary of a viscoplastic Bingham flow for finite solid deformations Thual O, Lacaze L |
88 - 97 |
Constitutive equation with fractional derivatives for the generalized UCM model Yang P, Lam YC, Zhu KQ |
98 - 109 |
Transient shear rheology of carbon nanofiber/polystyrene melt composites Kagarise C, Xu JH, Wang YR, Mahboob M, Koelling KW, Bechtel SE |
110 - 119 |
Fiber orientation kinetics of a concentrated short glass fiber suspension in startup of simple shear flow Eberle APR, Velez-Garcia GM, Baird DG, Wapperom P |
120 - 135 |
A semi-Lagrangian micro-macro method for viscoelastic flow calculations Prieto JL, Bermejo R, Laso M |
136 - 142 |
Control of homogeneous shear flow of multimode Maxwell fluids Savelev E, Renardy M |
143 - 157 |
A numerical method for solving the dynamic three-dimensional Ericksen-Leslie equations for nematic liquid crystals subject to a strong magnetic field Cruz PA, Tome MF, Stewart IW, McKee S |
158 - 162 |
Self-similar collapse of a circular cavity of a power-law liquid Gratton J, Perazzo CA |
163 - 173 |
The Dean instability in power-law and Bingham fluids in a curved rectangular duct Fellouah H, Castelain C, Ould-El-Moctar A, Peerhossaini H |
174 - 183 |
Study on the pulsating flow of a worm-like micellar solution Herrera EE, Calderas F, Chavez AE, Manero O |