Page:Elementary Principles in Statistical Mechanics (1902).djvu/101

Rh We have therefore

The average values of the powers of the anomalies of the energies are perhaps most easily found as follows. We have identically, since $$\overline\epsilon$$ is a function of $$\Theta$$, while $$\epsilon$$ is a function of the $$p$$'s and $$q$$'s, i. e., by (108),