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Time range of logarithmic decay.

We assume a logarithmic normal distribution of activation volumes within an ensemble and study four different models of its average thermal relaxation. We extract from them a common rule for the time range on which logarithmic relaxation can be observed. We further show that to a very good approximation the coefficient of magnetic viscosity is S υ =-T/(∂ /∂H) where is the average activation volume within the ensemble