Interfacial rheology is crucial in dictating morphology
and ultimate
properties of particle-stabilized polymer blends, but is challenging
to be determined. In this study, a fully polymeric dumbbell-shaped
Janus nanoparticle (JNP) of polymethyl methacrylate (PMMA) and polystyrene
(PS) spheres with equal sizes (∼80 nm) was prepared and used
as an efficient compatibilizer for PMMA/PS blends. The JNPs were preferentially
localized at the PMMA/PS interface, thereby reducing the interfacial
tension and refining the morphology in both droplet-matrix and co-continuous
type blends, whereby a JNP concentration ∼2.5 wt % is sufficient
to reach a saturation in droplet size reduction due to compatibilization.
Based on the linear viscoelastic moduli and corresponding relaxation
spectra (H(τ)*τ) of JNP-compatibilized
droplet-matrix blends, besides the droplet shape relaxation time (τF), a longer relaxation time (τβ), typically
related to interfacial viscoelasticity, was readily identified. The
dependence of τβ on the JNP concentration (W
JNPs) was significantly dominated by the droplet
size reduction induced by the JNP compatibilization, with τβ decreasing with increasing W
JNPs. The viscoelastic properties extracted from τβ typically originate from a combination of gradients in interfacial
tension due to the particle redistribution at the droplet interface
(Marangoni stresses) and the deviatoric stresses of intrinsic rheological
origin. The latter originate from the intrinsic viscoelasticity of
the particle-laden interface, which is enhanced by particle jamming
and particle–polymer interactions, such as entanglements between
chains from the polymeric spheres and those penetrating from the bulk
into the spheres. To address the challenge of isolating these contributions,
a JNP-sandwiched PMMA/PS multilayer structure was designed to exclude
the effect of Marangoni stresses and droplet curvature, thus having
no τF but a new relaxation (τ′β), which characterizes the contribution of intrinsic interfacial
viscoelasticity. The τ′β was observed
to increase with JNP coverage (Σ) following the Vogel–Fulcher–Tammann
model that is typically used to describe the divergent behavior of
the “cage” effect in classical colloidal glasses. Moreover,
a multimode Maxwell model fitting allows to split the interfacial
relaxation into the confined diffusion of JNPs within their cage and
the entanglements between the JNPs and the bulk.