| 85 - 100 |
Additional effects on internal flow of non-Newtonian fluids in the presence of a particle
Pereira RG |
| 101 - 133 |
An experimental determination of the stress-microstructure relationship in semi-concentrated fiber suspensions
Petrich MP, Koch DL, Cohen C |
| 135 - 146 |
Network constitutive equation with internal viscosity: application to stress jump prediction
Sun N, Fong CFCM, De Kee D |
| 147 - 184 |
Non-isothermal viscoelastic flow computations in an axisymmetric contraction at high Weissenberg numbers by a finite volume method
Wachs A, Clermont JR |
| 185 - 198 |
The flow of a class of Oldroyd fluids around a re-entrant corner
Fontelos MA, Friedman A |
| 199 - 233 |
Transient two-dimensional coating flow of a viscoelastic fluid film on a substrate of arbitrary shape
Khayat RE |
| 235 - 251 |
Shear-induced rupturing of a viscous drop in a Bingham liquid
Li J, Renardy YY |
| 253 - 276 |
Stability of the mixing layer of fiber suspensions: role of the closure approximation and off-plane orientation
Azaiez J |
| 277 - 293 |
Energetic effects on the stability of viscoelastic Dean flow
Al-Mubaiyedh UA, Sureshkumar R, Khomami B |
| 295 - 314 |
Shear banding and secondary flow in viscoelastic fluids between a cone and plate
Kumar S, Larson RG |
| 315 - 342 |
Deformation of a two-dimensional viscoelastic drop at non-zero Reynolds number in time-periodic extensional flows
Sarkar K, Schowalter WR |
| 343 - 362 |
Squeezing flow of a viscoelastic solid
Phan-Thien N |
| 363 - 374 |
Convective orientational renewal in entangled polymers
Ianniruberto G, Marrucci G |
