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All experimental results are explained by a stepwise bulk phase formation process including rearrangement of adatoms in the 2-D adsorbed layer, formation of critical clusters and further rearrangement and growth forming epitaxially orientated 3-D crystallites.
Therefore, patients would be expected to write more open, qualitative comments in the most critical clusters than in other clusters.
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Therefore, in CORA, rate allocation requests coverage scheduling to activate such critical cluster members within the ideal proximity of the clusterhead which we refer as correlator radius.
At the critical cluster size n R c, R-row structure changing to (R + 1 -row structure also means that their energy difference reaches minimum.
The nucleation rate and the number of atoms in the critical cluster (nucleus) are determined from the analysis of the kinetic data.
The thermodynamic specification of the critical cluster size for nucleation has been commonly used as the starting point for bubble growth analyses.
When the limiting stress is reached the critical cluster grows in an unstable way leading to catastrophic failure of the specimen.
The nucleation process must be treated by an atomistic model due to the derived low number of atoms in the critical cluster.
Results showed that, as critical cluster size increases, slope of the fracture probability distribution is given in a Weibull probability scale as follows: mc=i×mf (i, the number of broken fibers in a cluster; mc and mf, Weibull shape parameters for fracture probabilities of a critical cluster and fiber strength, respectively).
The initial conditions for bubble growth are obtained from the state of the pre-bubble nuclei (or clusters) at the upper bound of the critical cluster region predicted by the classical nucleation theory.
The potential of interleaving to delay catastrophic translaminar failure lies in this last aspect, which permits a larger critical cluster of broken fibres than that of classical UD composites.
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