Page:Elementary Principles in Statistical Mechanics (1902).djvu/206

182 occur in the canonical ensemble of the whole system, these phases will form a canonical ensemble of the same modulus. This canonical ensemble of phases of the first body will consist of parts which belong to the different microcanonical ensembles into which the canonical ensemble of the whole system is divided.

Let us now imagine that the modulus of the principal canonical ensemble is increased by $$2\Delta \Theta$$, and its average energy by $$2\Delta \epsilon$$. The modulus of the canonical ensemble of the phases of the first body considered separately will be increased by $$2\Delta \Theta$$. We may regard the infinity of microcanonical ensembles into which we have divided the principal canonical ensemble as each having its energy increased by $$2\Delta \epsilon$$. Let us see how the ensembles of phases of the first body contained in these microcanonical ensembles are affected. We may assume that they will all be affected in about the same way, as all the differences which come into account may be treated as small. Therefore, the canonical ensemble formed by taking them together will also be affected in the same way. But we know how this is affected. It is by the increase of its modulus by $$2\Delta \Theta$$, a quantity which vanishes when the quantity of the bath is indefinitely increased.

In the case of an infinite bath, therefore, the increase of the energy of one of the microcanonical ensembles by $$2\Delta \epsilon$$, produces a vanishing effect on the distribution in energy of the phases of the first body which it contains. But $$2\Delta \epsilon$$ is more than the average difference of energy between the microcanonical ensembles. The distribution in energy of these phases is therefore the same in the different microcanonical ensembles, and must therefore be canonical, like that of the ensemble which they form when taken together.