Understanding
the nonequilibrium dynamics of topologically entangled
polymers under strong external deformation has been a grand challenge
in polymer science for more than half a century. Important deformation-induced
single-polymer structural changes have been identified, such as chain
orientation and stretching. But how these changes impact the physical
entanglement network and bulk viscoelasticity remains largely elusive
in the fast flow regime that involves highly oriented and stretched
polymer chains. Here, through new experimental and theoretical developments,
we establish a unified understanding of the steady-state shear viscosity,
η, of entangled polymer melts at high Rouse Weissenberg numbers, WiR > 1. New capillary rheometry measurements
in the absence of flow instabilities reveal a dramatic change in shear-thinning
scaling from η ∼ γ̇–0.7 ± 0.1 at WiR N/γ̇)0.50 at WiR > 1, where N is the degree of polymerization
and γ̇ is the shear rate. Moreover, the viscosity scaling
exponent with polymer molecular weight decreases with applied shear
stress, and a remarkable unentangled melt scaling η ∼ N emerges under ultrahigh constant stress conditions σ/Ge ≥ 2, where Ge is the equilibrium entanglement elastic modulus. These new observations
are not consistent with existing molecular theories. We construct
a dynamic scaling model based on tension blob concepts as extended
to entangled polymers, resulting in a (near) universal expression
for the shear-thinning behavior controlled by purely dissipative considerations
associated with orientational stress. This physical picture is in
sharp contrast to the predictions of various state-of-the-art tube-based
models based on the widely adopted factorization approximation of
the total stress into stretching and orientational contributions,
and also qualitatively differs from predictions of non-tube-based
slip-link models based on a transient network perspective