| 1081 - 1099 |
Large-amplitude oscillatory shear flow from the corotational Maxwell model
Giacomin AJ, Bird RB, Johnson LM, Mix AW |
| 1100 - 1115 |
Numerical simulations of mounding and submerging flows of shear-thinning jets impinging in a container
Roberts SA, Rao RR |
| 1116 - 1122 |
The consequences of yield stress on deployment of a non-Newtonian anti-HIV microbicide gel
Tasoglu S, Park SC, Peters JJ, Katz DF, Szeri AJ |
| 1123 - 1128 |
Misting of non-Newtonian liquids in forward roll coating
Owens MS, Vinjamur M, Scriven LE, Macosko CW |
| 1129 - 1136 |
Simulation of fiber reinforced composite materials mold filling process and mechanical properties analysis
Yang BX, Ouyang J, Li XJ |
| 1137 - 1157 |
A high-resolution finite-difference method for simulating two-fluid, viscoelastic gel dynamics
Wright GB, Guy RD, Du J, Fogelson AL |
| 1158 - 1172 |
A Newton-Krylov finite volume algorithm for the power-law non-Newtonian fluid flow using pseudo-compressibility technique
Nejat A, Jalali A, Sharbatdar M |
| 1173 - 1182 |
Wall effects on the transportation of a cylindrical particle in power-law fluids
Despeyroux A, Ambari A, Ben Richou A |
| 1183 - 1189 |
Self-consistent particle simulation of model-stabilized colloidal suspensions
Myung JS, Song S, Ahn KH, Lee SJ |
| 1190 - 1197 |
An algebraic closure for the DNS of fiber-induced turbulent drag reduction in a channel flow
Moosaie A, Manhart M |
| 1198 - 1209 |
On the "viscosity overshoot" during the uniaxial extension of a low density polyethylene
Burghelea TI, Stary Z, Munstedt H |
