1 - 10 |
Combined interfacial shear rheology and microstructure visualization of asphaltenes at air-water and oil-water interfaces Lin YJ, Barman S, He P, Zhang ZQ, Christopher GF, Biswal SL |
11 - 23 |
Elongation thinning and morphology deformation of nanoparticle-filled polypropylene/polystyrene blends in elongational flow Kong MQ, Huang YJ, Lv YD, Yang QD, Li GX, Larson RG |
25 - 47 |
Evaluation of tube models for linear entangled polymers in simple and complex flows Varchanis S, Dimakopoulos Y, Tsamopoulos J |
49 - 61 |
Nonlinear stability and dynamics of nonisothermal film casting Tian FC, Tang XL, Xu TY, Yang JS, Xie C, Li LB |
63 - 79 |
Asymmetric soft-hard colloidal mixtures: Osmotic effects, glassy states and rheology Merola MC, Parisi D, Truzzolillo D, Vlassopoulos D, Deepak VD, Gauthier M |
81 - 87 |
Linear viscoelastic response and steady shear viscosity of native cellulose in 1-ethyl-3-methylimidazolium methylphosphonate Chen X, Liang SW, Wang SW, Colby RH |
89 - 106 |
Stress bifurcation in large amplitude oscillatory shear of yield stress fluids Yang K, Liu ZW, Wang J, Yu W |
107 - 120 |
Rheological analysis of core-stabilized Pluronic F127 by semi-interpenetrating network (sIPN) in aqueous solution Li XL, Park EK, Hyun K, Oktavia L, Kwak M |
121 - 134 |
A constitutive model for entangled polydisperse linear flexible polymers with entanglement dynamics and a configuration dependent friction coefficient. Part I: Model derivation Mead DW, Monjezi S, Park J |
135 - 147 |
A constitutive model for entangled polydisperse linear flexible polymers with entanglement dynamics and a configuration dependent friction coefficient. Part II. Modeling "shear modification" following cessation of fast shear flows Mead DW, Monjezi S, Park J |
149 - 159 |
Binary colloidal glasses under transient stress- and strain-controlled shear Sentjabrskaja T, Hendricks J, Jacob AR, Petekidis G, Egelhaaf SU, Laurati M |
161 - 170 |
Influence of rheology on renewable pressure-sensitive adhesives from a triblock copolymer Ewert TR, Mannion AM, Coughlin ML, Macosko CW, Bates FS |
171 - 181 |
Linear-nonlinear dichotomy of rheological responses in particle-filled polymer melts Xiong WT, Wang XR |
183 - 196 |
Fractal approaches to characterize the structure of capillary suspensions using rheology and confocal microscopy Bossler F, Maurath J, Dyhr K, Willenbacher N, Koos E |
197 - 207 |
A well defined glass state obtained by oscillatory shear Perez-Ocampo L, Zaccone A, Laurati M |
209 - 219 |
Rising bubbles in yield stress materials Lopez WF, Naccache MF, Mendes PRD |
221 - 233 |
On the origin of brittle fracture of entangled polymer solutions and melts Wagner MH, Narimissa E, Huang Q |
235 - 247 |
A novel hybrid population balance-Brownian dynamics method for simulating the dynamics of polymer-bridged colloidal latex particle suspensions Hajizadeh E, Yu S, Wang SH, Larson RG |
249 - 264 |
Periodic "stick-slip" transition within a continuum model for entangled supramolecular polymers Boudara VAH, Read DJ |
265 - 275 |
Morphology of critically sized crystalline nuclei at shear-induced crystal nucleation in amorphous solid Galimzyanov BN, Mokshin AV |
277 - 293 |
Frequency-sweep medium-amplitude oscillatory shear (MAOS) Singh PK, Soulages JM, Ewoldt RH |
295 - 311 |
Flow field based data processing for the oscillating conical bob interfacial shear rheometer Tajuelo J, Rubio MA, Pastor JM |
313 - 320 |
The use of principal spatial tensor to predict anisotropic fiber orientation in concentrated fiber suspensions Tseng HC, Chang RY, Hsu CH |
321 - 342 |
A multimode structural kinetics constitutive equation for the transient rheology of thixotropic elasto-viscoplastic fluids Wei YF, Solomon MJ, Larson RG |
343 - 356 |
Evaluating models for polycaprolactone crystallization via simultaneous rheology and Raman spectroscopy Kotula AP, Migler KB |
357 - 369 |
Extending yield-stress fluid paradigms Nelson AZ, Bras RE, Liu JP, Ewoldt RH |
371 - 403 |
Single polymer dynamics for molecular rheology Schroeder CM |