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Microsecond relaxation processes in shear and extensional flows of weakly elastic polymer solutions
A Minimal Model for Vorticity and Gradient Banding in Complex Fluids
A general phenomenological reaction-diffusion model for flow-induced phase
transitions in complex fluids is presented. The model consists of an equation
of motion for a nonconserved composition variable, coupled to a Newtonian
stress relations for the reactant and product species. Multivalued reaction
terms allow for different homogeneous phases to coexist with each other,
resulting in banded composition and shear rate profiles. The one-dimensional
equation of motion is evolved from a random initial state to its final
steady-state. We find that the system chooses banded states over homogeneous
states, depending on the shape of the stress constitutive curve and the
magnitude of the diffusion coefficient. Banding in the flow gradient direction
under shear rate control is observed for shear-thinning transitions, while
banding in the vorticity direction under stress control is observed for
shear-thickening transitions.Comment: 11 pages, submitted to Eur Phys J
Dynamic Response of Block Copolymer Wormlike Micelles to Shear Flow
The linear and non-linear dynamic response to an oscillatory shear flow of
giant wormlike micelles consisting of Pb-Peo block copolymers is studied by
means of Fourier transform rheology. Experiments are performed in the vicinity
of the isotropic-nematic phase transition concentration, where the location of
isotropic-nematic phase transition lines is determined independently. Strong
shear-thinning behaviour is observed due to critical slowing down of
orientational diffusion as a result of the vicinity of the isotropic- nematic
spinodal. This severe shear-thinning behaviour is shown to result in gradient
shear banding. Time-resolved Small angle neutron scattering experiments are
used to obtain insight in the microscopic phenomena that underly the observed
rheological response. An equation of motion for the order-parameter tensor and
an expression of the stress tensor in terms of the order-parameter tensor are
used to interpret the experimental data, both in the linear and non-linear
regime. Scaling of the dynamic behaviour of the orientational order parameter
and the stress is found when critical slowing down due to the vicinity of the
isotropic-nematic spinodal is accounted for.Comment: Accepted by J. Phys.: Condens. Matter, CODEF II Special Issue. 20
pages, 9 figure
Dynamic Response of Block Copolymer Wormlike Micelles to Shear Flow
The linear and non-linear dynamic response to an oscillatory shear flow of
giant wormlike micelles consisting of Pb-Peo block copolymers is studied by
means of Fourier transform rheology. Experiments are performed in the vicinity
of the isotropic-nematic phase transition concentration, where the location of
isotropic-nematic phase transition lines is determined independently. Strong
shear-thinning behaviour is observed due to critical slowing down of
orientational diffusion as a result of the vicinity of the isotropic- nematic
spinodal. This severe shear-thinning behaviour is shown to result in gradient
shear banding. Time-resolved Small angle neutron scattering experiments are
used to obtain insight in the microscopic phenomena that underly the observed
rheological response. An equation of motion for the order-parameter tensor and
an expression of the stress tensor in terms of the order-parameter tensor are
used to interpret the experimental data, both in the linear and non-linear
regime. Scaling of the dynamic behaviour of the orientational order parameter
and the stress is found when critical slowing down due to the vicinity of the
isotropic-nematic spinodal is accounted for.Comment: Accepted by J. Phys.: Condens. Matter, CODEF II Special Issue. 20
pages, 9 figure
Stress response and structural transitions in sheared gyroidal and lamellar amphiphilic mesophases: lattice-Boltzmann simulations
We report on the stress response of gyroidal and lamellar amphiphilic
mesophases to steady shear simulated using a bottom-up lattice-Boltzmann model
for amphiphilic fluids and sliding periodic (Lees-Edwards) boundary conditions.
We study the gyroid per se (above the sponge-gyroid transition, of high
crystallinity) and the molten gyroid (within such a transition, of
shorter-range order). We find that both mesophases exhibit shear-thinning, more
pronounced and at lower strain rates for the molten gyroid. At late times after
the onset of shear, the skeleton of the crystalline gyroid becomes a structure
of interconnected irregular tubes and toroidal rings, mostly oriented along the
velocity ramp imposed by the shear, in contradistinction with free-energy
Langevin-diffusion studies which yield a much simpler structure of disentangled
tubes. We also compare the shear stress and deformation of lamellar mesophases
with and without amphiphile when subjected to the same shear flow applied
normal to the lamellae. We find that the presence of amphiphile allows (a) the
shear stress at late times to be higher than in the case without amphiphile,
and (b) the formation of rich patterns on the sheared interface, characterised
by alternating regions of high and low curvature.Comment: 15 pages, 10 figures, Physical Review E, in pres
Generality of shear thickening in suspensions
Suspensions are of wide interest and form the basis for many smart fluids.
For most suspensions, the viscosity decreases with increasing shear rate, i.e.
they shear thin. Few are reported to do the opposite, i.e. shear thicken,
despite the longstanding expectation that shear thickening is a generic type of
suspension behavior. Here we resolve this apparent contradiction. We
demonstrate that shear thickening can be masked by a yield stress and can be
recovered when the yield stress is decreased below a threshold. We show the
generality of this argument and quantify the threshold in rheology experiments
where we control yield stresses arising from a variety of sources, such as
attractions from particle surface interactions, induced dipoles from applied
electric and magnetic fields, as well as confinement of hard particles at high
packing fractions. These findings open up possibilities for the design of smart
suspensions that combine shear thickening with electro- or magnetorheological
response.Comment: 11 pages, 9 figures, accepted for publication in Nature Material
Glass transitions and shear thickening suspension rheology
We introduce a class of simple models for shear thickening and/ or `jamming'
in colloidal suspensions. These are based on schematic mode coupling theory
(MCT) of the glass transition, having a memory term that depends on a density
variable, and on both the shear stress and the shear rate. (Tensorial aspects
of the rheology, such as normal stresses, are ignored for simplicity.) We
calculate steady-state flow curves and correlation functions. Depending on
model parameters, we find a range of rheological behaviours, including
`S-shaped' flow curves, indicating discontinuous shear thickening, and
stress-induced transitions from a fluid to a nonergodic (jammed) state, showing
zero flow rate in an interval of applied stress. The shear thickening and
jamming scenarios that we explore appear broadly consistent with experiments on
dense colloids close to the glass transition, despite the fact that we ignore
hydrodynamic interactions. In particular, the jamming transition we propose is
conceptually quite different from various hydrodynamic mechanisms of shear
thickening in the literature, although the latter might remain pertinent at
lower colloid densities. Our jammed state is a stress-induced glass, but its
nonergodicity transitions have an analytical structure distinct from that of
the conventional MCT glass transition.Comment: 33 pages; 19 figure
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