A
Connection between
Jamming and Discontinuous Shear Thickening
in (non-Brownian) Suspensions
In Newtonian fluids
the viscosity does not change with an
applied shear rate, while non-Newtonian
fluids usually show a decrease of viscosity
when sheared faster; i.e., they shear
thin. The opposite behavior, shear thickening,
is less common but can be quite dramatic:
beyond a certain shear rate the viscosity
increases potentially by orders of magnitude.
We used rheometry measurements to
characterize the critical behavior in
two model shear thickening suspensions:
cornstarch in water and glass spheres
in oil. The slope of the shear thickening
part of the viscosity curve is found
to increase dramatically with packing
fraction and diverge at a critical packing
fraction. The magnitude of the viscosity
and the yield stress are also found to
have scalings that diverge at that same
critical packing fraction. We observe
shear thickening as long as the yield
stress is less than the stress at the
viscosity maximum. Above this point the
suspensions transition to purely shear
thinning. Based on these data we developed
a dynamic jamming phase diagram for suspensions
and show that a limiting case of shear thickening
corresponds to a jammed state.
Eric Brown
and Heinrich M. Jaeger, "Dynamic
Jamming Point for Shear Thickening Suspensions ",
Phys. Rev. Lett. 103,
086001 (2009). link
to article