The clustering of carbon in the detonation regime is studied with the assumption of a diffusion-limited clustering process. The diffusion constants are determined from modified Enskog theory and the Stokes–Einstein relation. With the size dependence of the cluster energy treated with a surface term, the energy difference between clusters and bulk carbon has an asymptotic time dependence of t−1/3. That is, for any given time it takes 1000 times as long to release the next 90% of the carbon energy. This leads to a very slow ‘‘reaction rate’’ which can couple to the reaction zone to produce nonideal time-dependent detonations on the scale of microseconds and centimeters. In addition, any ‘‘bottleneck’’ in the clustering process due to a sticking coefficient of less than one leads to a temporary delay in energy release that persists out to times several orders of magnitude larger than the time scale of the initial effect of the ‘‘bottleneck.’’
No takes yet. Share an insight, caveat, or question.
Shaw et al. (1987) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: