We study the recombination kinetics and stress relaxation in a generic reversible polymer model, which is believed to resemble a wormlike micellar system. We find evidence that, at high concentrations, the recombination kinetics in this model cannot be described by a mean-field approach, but is diffusion-controlled and dominated by self-recombination events. We observe that the long-time stress relaxation of unentangled chains is proportional to (1/ t ) 1/2 exp [ − t /τ relax ], with a relaxation time given by τ relax = ( t h 2/3 τ ⟨ L ⟩ 1/3 ), where t h is the average diffusion time to a different chain end, and τ ⟨ L ⟩ is the characteristic relaxation time of a system of "dead" polymers of length equal to the average micellar length. A recombination activation barrier is needed to drive the system towards mean-field behaviour. This, in its turn, is often required in order to realistically model the rheology and dynamics of wormlike micelles.
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Padding et al. (2004) studied this question.
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