Nonuniform flow in soft glasses of colloidal rods

Dhont, Jan K.G.; Kriegs, H.; Vlassopoulos, D.; Danko, O.; Kang, K.; Marakis, J.

doi:10.1103/PhysRevFluids.2.043301

Journal Article

FZJ-2017-03174

Nonuniform flow in soft glasses of colloidal rods

Dhont, J. K. G. (Corresponding author)FZJ* ; Kang, K.FZJ* ; Kriegs, H.FZJ* ; Danko, O. ; Marakis, J. ; Vlassopoulos, D.

2017
APS College Park, MD

Physical review fluids 2(4), 043301 (2017) [10.1103/PhysRevFluids.2.043301]

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Please use a persistent id in citations: http://hdl.handle.net/2128/14249 doi:10.1103/PhysRevFluids.2.043301

Abstract: Despite our reasonably advanced understanding of the dynamics and flow of glasses made of spherical colloids, the role of shape, i.e., the respective behavior of glasses formed by rodlike, particles is virtually unexplored. Recently, long, thin and highly charged rods (fd-virus particles) were found to vitrify in aqueous suspensions at low ionic strength [Phys. Rev. Lett. 110, 015901 (2013)]. The glass transition of these long-ranged repulsive rods occurs at a concentration far above the isotropic-nematic coexistence region and is characterized by the unique arrest of both the dynamics of domains that constitute the chiral-nematic orientational texture, as well as individual rods inside the domains. Hence, two relevant length scales exist: the domain size of a few hundreds of microns, and the rod-cage size of a few microns, inside the domains. We show that the unique dual dynamic arrest and the existing of two widely separated length scales imparts an unprecedented, highly heterogeneous flow behavior with three distinct signatures. Beyond a weak stress plateau at very small shear rates that characterizes the glass, the kinetic arrest of the domain dynamics gives rise to internal fracture, as a result of domain-domain interactions, as well as wall partial slip. It is shown that, on increasing the shear rate, the fractured plug flow changes to a shear-banded flow profile due to the stress response of the kinetically arrested aligned rods within the domains. Shear-gradient banding occurs due to the strong thinning of the uniform chiral-nematic phase within the domains, i.e., complying with the classic shear-banding scenario, giving rise to a stress plateau in the flow curve. Finally, a linear (uniform) velocity profile is found at the highest shear rates. Vorticity banding is also observed at intermediate and high shear rates. These results point to the crucial role of particle shape in tailoring the flow properties of dense colloidal suspensions. Moreover, they strongly support the argument that the origin of shear banding in soft-particle glasses with long-ranged repulsive interactions is fundamentally different from that of hard-particle glasses with short-ranged repulsive interactions.

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