The peculiarities of non-exponential degradation kinetics in topological-disordered solids are analyzed. It was shown that degradation transformations, described by ideal exponential function, are determined by one value of activation energy independently to the structural dispersivity of the system, while the non-exponential degradation kinetics corresponds to stretched or suppressed exponential-power-like relaxation function. The stretched degradation kinetics is proper to own degradation transformations in one-type systems. The degradation transformations, including two or more different elementary processes, are described by suppressed kinetics.
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