⁄ are universal and should not depend on the curing percentage. If we assume that 𝛼 = 0 (without logarithmic corrections) and that the hyperbolic shape of the curves around 𝑇 , is caused by the smooth crossover between glass and liquid phases, due to the non-zero speed at which the temperature was changed in the simulation, the proposed power law seems to agree with our numerical results. The jump of the derivative of the curve 𝜌(𝑇) at 𝑇 = 𝑇 , for an idealized, infinitely slow process can be estimated by fitting lines to linear parts of the curves obtained from the simulation for 𝑇 < 𝑇 , and for 𝑇 > 𝑇 , . This way we verified that, up to numerical errors, the ratio of amplitudes is the same for all curing percentages and we estimated it to be 𝛾 4 " 𝛾 4 5 ⁄ = 0.260 ± 0.004. This universal behavior, observed to the best of our knowledge for the first time in MD simulations, independently shows that our block-chemistry methodology is suitable for modeling epoxy networks. . The two sets of solid dots represent experimental data from White et al. and Simpson et al. originally reported without error bars.