We report viscosity, recoverable compliance, and molar mass distribution for a series of randomly branched polyester samples with long linear chain sections between branch points. Molecular structure characterization determines $\tau =2.47\mathrm{}\pm 0.05$ for the exponent controlling the molar mass distribution, so this system belongs to the vulcanization (mean-field) universality class. Consequently, branched polymers of similar size strongly overlap and form interchain entanglements. The viscosity diverges at the gel point with an exponent $s=6.1\mathrm{}\pm 0.3,$ that is significantly larger than the value of 1.33 predicted by the branched polymer Rouse model (bead-spring model without entanglements). The recoverable compliance diverges at the percolation threshold with an exponent $t=3.2\mathrm{}\pm \mathrm{0.2.}$ This effect is consistent with the idea that each branched polymer of size equal to the correlation length stores $k_{B}T$ of elastic energy. Near the gel point, the complex shear modulus is a power law in frequency with an exponent $u=0.33\mathrm{}\pm \mathrm{0.05.}$ The measured rheological exponents confirm that the dynamic scaling law $u=t/(s+t)\mathrm{}$ holds for the vulcanization class. Since s is larger and u is smaller than the Rouse values observed in systems that belong to the critical percolation universality class, we conclude that entanglements profoundly increase the longest relaxation time. Examination of the literature data reveals clear trends for the exponents s and u as functions of the chain length between branch points. These dependencies, qualitatively explained by hierarchical relaxation models, imply that the dynamic scaling observed in systems that belong to the vulcanization class is nonuniversal.

• Received 24 August 1998

DOI:https://doi.org/10.1103/PhysRevE.60.5657