717 - 728 |
Scaling behavior of the elastic properties of non-dilute MWCNT-epoxy suspensions Khalkhal F, Carreau PJ |
729 - 740 |
Reversed planar elongation of soft polymeric networks Jensen MK, Rasmussen HK, Skov AL, Hassager O |
741 - 752 |
Normal stress differences in large-amplitude oscillatory shear flow for the corotational "ANSR" model Giacomin AJ, Bird RB |
753 - 766 |
Numerical study of chain conformation on shear banding using diffusive Rolie-Poly model Chung C, Uneyama T, Masubuchi Y, Watanabe H |
767 - 778 |
Dependence of the dynamic moduli of heterogeneous nematic polymers on planar anchoring relative to flow direction Choate EP, Forest MG |
779 - 785 |
Rheology of carbon black suspensions. IV. Effect of suspending media on the sol-gel transition behavior Aoki Y |
787 - 793 |
Rheology of carbon black suspensions. V. Heat-induced gelation and its reversibility Aoki Y |
795 - 807 |
TTS in LAOS: validation of time-temperature superposition under large amplitude oscillatory shear Vananroye A, Leen P, Van Puyvelde P, Clasen C |
809 - 823 |
Anomalous rheology of polypyrrole nanoparticle/alginate suspensions: effect of solids volume fraction, particle size, and electronic state Thanpitcha T, Li Z, Rujiravanit R, Sirivat A, Jamieson AM |
825 - 836 |
Microstructure and magnetorheology of graphite-based MR elastomers Tian TF, Li WH, Alici G, Du H, Deng YM |
837 - 866 |
Analytic derivation of the Cox-Merz rule using the MLD "toy" model for polydisperse linear polymers Mead DW |