Concerning the Statistics of Classical Systems
نویسنده
چکیده
[1] We first define the phase volume of a system as the volume contained within the energy surface in the phase space and define its phase density as its derivative with respective to energy. Because of the ergodic hypothesis, the system phase density can be obtained as the convolution product of the phase densities of the individual parts; and these can again, when the energy of the parts can be separated, be depicted as convolution products of the energy contributions of the assigned phase densities.
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