Molecular dynamics simulations of the dissociation of methane, ethylene, and benzene at 50 GPa show that thermally activated carbon–carbon bond breaking produces a stationary n−5/2 distribution of short-lived n-atom carbon chains. Chain fragmentation rates follow an Arrhenius law in temperature, and the fraction of carbon existing as small chains increases with increasing temperature, ultimately approaching 1 at some critical temperature. Mean-field coagulation theory with added fragmentation terms yields the stationary n−5/2 distribution and shows that the rate of carbon coagulation to bulk material slows down with increasing temperature, approaching zero at the critical temperature.
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Viecelli et al. (2002) studied this question.
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