Abstract
For pt.I see ibid., vol.7, p.2130 (1974). Elementary methods of relativistic statistical mechanics developed in the previous paper are applied to the particular case of a relativistic gas with constant particle number. They are compared with an earlier approach and are shown to be inequivalent and superior to it. A third approach, based on a radical re-appraisal of the principles underlying the earlier one, is introduced. The two new schemes are examined, and the difficulties inherent in each are considered.
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