Densely packed soft microgels (pastes)
behave as a yield-stress
fluid. They act as soft elastic solids with finite equilibrium shear
modulus (G0) below a critical stress (σc) whereas they flow like liquids above σc. The effects of size and stiffness heterogeneities in the constituent
microgels on the rheological properties of the pastes are revealed
using the binary microgel mixtures by an oscillatory rheometer and
diffusive wave spectroscopy (DWS). The binary blends with various
degrees of size and stiffness disparities are made by mixing the pastes
with the same apparent particle-volume fraction (ϕeff) at various values of relative weight fraction of soft microgels
(fsoft). The G0–fsoft relations for the soft/hard
microgel mixtures are significantly influenced by size disparity:
The relations for small size disparities well obey the logarithmic
mixing rule, while those for large size disparities have a wide fsoft regime in which G0 are almost equal to those of the single small-microgel pastes
(G0,small), regardless of whether the
small microgels are soft or hard. The characteristic fsoft region with G0 ≈ G0,small for the mixtures with large size disparities
is attributed to the developed continuous phase of small microgels
(overwhelming in number) where the large microgels are discretely
dispersed. The steady-state flow behavior of the binary pastes above
σc obey the classical Hershel–Bulkley (H–B)
equation. In each binary paste, the characteristic time (τcage) of the fast local dynamics of microgels trapped in the
densely packed structures evaluated from DWS is close to the characteristic
time (τHB) obtained from the parameters in the H–B
equation and G0. This agreement shows
that the dynamics of the positional rearrangement of microgels in
the steady-state flow is closely related to the fast local dynamics
in the quiescent state of the pastes, independently of the size and
stiffness disparities in the constituent microgels.