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1 ereby eliminating layering as the driver for shear thinning.
2 ereas the other is strongly viscoelastic and shear thinning.
3 study reveals rich RBC dynamics that govern shear thinning.
4 that the resulting hydrogel is rigid but is shear-thinning.
6 d that there is a strong correlation between shear thinning and a two-particle measure of the shear s
7 nts on SWNT/p-PNCPA aqueous suspensions show shear thinning and near Newtonian behavior at 10 and 50
9 of the neutrophil needs to incorporate both shear thinning and surface viscosity to remain valid ove
10 the particle configurations associated with shear thinning and thickening cast doubt on that conclus
11 and gel strength, but also leads to special shear-thinning and recovery properties of the hydrogel.
12 fabrication of self-assembled hydrogels with shear-thinning and self-healing properties employing rat
16 s, the plateau force exhibited a significant shear thinning as indicated by a weak power-law dependen
18 mer conversion to be tracked in spite of the shear-thinning behavior, and could be applied to study t
20 ar regime, the aggregation flows, exhibiting shear-thinning behaviour with a stress load that is comp
21 all four of the C-trim dispersions exhibited shear-thinning behaviours, which could be best described
22 que for nonequilibrium systems, we show that shear thinning can be decoupled from layering, thereby e
23 ibed as a self-similar elastic object with a shear-thinning damping term and a stiffness that becomes
24 ects) and wall- (due to fluid elasticity and shear thinning effects) directed elastic lift forces.
28 viscosity, Newtonian fluids to viscoelastic, shear-thinning fluids having much larger zero-shear visc
29 lose to that of water and exhibit negligible shear thinning, focusing occurs over a wide range of ela
34 ologic temperature is a highly viscoelastic, shear-thinning liquid suspension consisting of lipid lam
37 lain this peculiar observation by the strong shear thinning of the confined fluid and the osmotic rep
38 suggest that the hypermotile V is caused by shear thinning of the resistive population of strongly b
39 smaller than those of the FISP, those of the shear-thinning precursor are several times larger than t
40 ion and cell viability are unaffected by the shear thinning process and gel/cell constructs stay fixe
42 croscopic single-particle dynamics show that shear thinning results from the decreased relative contr
44 even models with both surface viscosity and shear thinning studied are still not sufficient to fully
46 fficiently through environments that contain shear-thinning viscoelastic fluids, such as the extracel
48 simple Newtonian fluid (i.e., models without shear thinning) were grossly incapable of accounting for
49 uest-host interactions, undergo disassembly (shear-thinning) when injected through a syringe and then
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