Long-chain branching profoundly modifies the nonlinear oscillatory response of entangled polymer melts by introducing arm-retraction pathways absent in linear polymers. We present a molecular tube theory that explains the characteristic maximum of the Nonlinearity Index (NLI) observed experimentally in long-chain-branched polymers. The theory extends the recently developed nonlinear tube-orientation description of linear polymers by incorporating branch-mediated orientational constraints and delayed arm retraction. The backbone initially develops nonlinear orientation as in the corresponding linear polymer, whereas long-arm retraction subsequently relaxes the stored branch-mediated orientational constraint and progressively erases backbone orientational memory. This competition produces a characteristic NLI maximum followed by a post-peak decay. The theory distinguishes the onset of nonlinear backbone orientation, the subsequent activation of arm-mediated relaxation, and the later strain at which branch-mediated relaxation balances orientational buildup and produces the NLI maximum. The architecture ratio, defined as the relative size of a long side arm compared with the backbone span between neighboring branch points, controls the strength of branch-mediated suppression, while the absolute arm length determines the arm-retraction time and hence the frequency dependence of the relaxation crossover. The resulting framework provides a molecular interpretation of nonlinear Fourier rheology and directly links the nonlinear harmonic response to polymer architecture.
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Nichetti et al. (2026) studied this question.
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