| 959 - 961 |
Comments on "Objective flow classification parameters and their use in general steady flows" by PO Brunn
Thompson RL, Mendes PRD |
| 963 - 974 |
Flow analysis for wormlike micellar solutions in an axisymmetric capillary channel
Yamamoto T, Hashimoto T, Yamashita A |
| 977 - 988 |
Photoviscoelastic behavior and residual thermal birefringence in optical-grade polycarbonates
Lin TH, Isayev AI |
| 989 - 997 |
Elasticity and dynamics of particle gels in non-Newtonian melts
Romeo G, Filippone G, Fernandez-Nieves A, Russo P, Acierno D |
| 999 - 1013 |
Shear and elongational flow behavior of acrylic thickener solutions Part I: Effect of intermolecular aggregation
Kheirandish S, Guybaidullin I, Wohlleben W, Willenbacher N |
| 1015 - 1021 |
Strain energy function of an uncross-linked butadiene rubber estimated from planar extension
Urayama K, Akuzawa N, Takigawa T |
| 1023 - 1038 |
Measurement of pressure coefficient of melt viscosity: drag flow versus capillary flow
Park HE, Lim ST, Laun HM, Dealy JM |
| 1039 - 1048 |
Coarse-grained model of entangled polymer melts in non-equilibrium
Rakshit A, Picu RC |
| 1049 - 1059 |
Reliable plate-plate MRF magnetorheometry based on validated radial magnetic flux density profile simulations
Laun HM, Schmidt G, Gabriel C, Kieburg C |
| 1061 - 1076 |
A unified model for polystyrene-nanorod and polystyrene-nanoplatelet melt composites
Kagarise C, Koelling KW, Wang YR, Bechtel SE |
