Physically confining polymers into
nanoscale pores induces significant
changes in their dynamics. Although different results on the effect
of confinement on the dynamics of polymers have been reported, changes
in the segmental mobility of polymers typically are correlated with
changes in their chain mobility due to increased monomeric relaxation
times. In this study, we show that translational and segmental dynamics
of polymers confined in disordered packings of nanoparticles (NPs)
can exhibit completely opposite behavior. We monitor the capillary
rise dynamics of entangled polystyrene (PS) in disordered packings
of silica NPs of 7 and 27 nm diameter. The effective viscosity of
PS in 27 nm SiO2 NP packings, inferred based on the Lucas–Washburn
equation, is significantly smaller than the bulk viscosity, and the
extent of reduction in the translational motion due to confinement
increases with the molecular weight of PS, reaching 4 orders of magnitude
reduction for PS with a molecular weight of 4M g/mol. The glass transition
temperature of entangled PS in the packings of 27 nm SiO2 NPs, however, increases by 45 K, indicating significant slowdown
of segmental motion. Interestingly, confinement of the polymers into
packings made of 7 nm SiO2 NPs results in molecular weight-independent
effective viscosity. The segmental dynamics of PS in 7 nm SiO2 NP packings are slowed down even further, as evidenced by
a 65 K increase in glass transition temperature. These seemingly disparate
effects are explained by the microscopic reptation-like transport
controlling the translational motion and the physical confinement
affecting the segmental dynamics under extreme nanoconfinement. Although
we do not fully understand the origin of the molecular weight-independent
effective viscosity of PS in the 7 nm SiO2 NP packings,
nonlinear flow and hyperconfinement effects may be playing a role.
The novel flow behavior that we observe opens new ground for further
theoretical exploration of the dynamics of extremely confined polymer
melts.