We present systematic, unique linear
and nonlinear shear rheology
data of an experimentally pure ring polystyrene and its linear precursor.
This polymer was synthesized anionically and characterized by interaction
chromatography and fractionation at the critical condition. Its weight-average
molar mass is 84 kg/mol; i.e., it is marginally entangled (entanglement
number Z ≈ 5). Its linear viscoelastic response
appears to be better described by the Rouse model (accounting for
ring closure) rather than the lattice-animal-based model, suggesting
a transition from unentangled to entangled ring dynamics. The failure
of both models in the terminal region may reflect the remaining unlinked
linear contaminants and/or ring–ring interpenetration. The
viscosity evolution at different shear rates was measured using a
homemade cone-partitioned plate fixture in order to avoid edge fracture
instabilities. Our findings suggest that rings are much less shear
thinning compared to their linear counterparts, whereas both obey
the Cox–Merz rule. The shear stress (or viscosity) overshoot
is much weaker for rings compared to linear chains, pointing to the
fact that their effective deformation is smaller. Finally, step strain
experiments indicate that the damping function data of ring polymers
clearly depart from the Doi–Edwards prediction for entangled
linear chains, exhibiting a weak thinning response. These findings
indicate that these marginally entangled rings behave like effectively
unentangled chains with finite extensibility and deform much less
in shear flow compared to linear polymers. They can serve as guideline
for further investigation of the nonlinear dynamics of ring polymers
and the development of constitutive equations.