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nydus/The Theory of Heat RadiationPublic
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188.

It now remains to prove that the sum Φ=∑1∞(wn−ζwn−1)logwn−[(1−ζ)n−1]wnlogζ,\Label[eqn](356)\upshape (356) where the quantities wn are subject only to the restrictions that [eqn:(353)] (353) and [eqn:(354)] (354) can never become negative. For this purpose we determine that system of values of the w's which, with a fixed value of ζ, makes the sum Φ a minimum. In this case δΦ=0, or

∑1∞(δwn−ζδwn−1)logwn+(wn−ζwn−1)δwnwn\Label[eqn](357)\upshape (357)−[(1−ζ)n−1]δwnlogζ=0,

where, according to [eqn:(353)] (353) and [eqn:(354)] (354), ∑1∞δwn=0andδw0=0.\Label[eqn](358)\upshape (358) If we suppose all the separate terms of the sum to be written out, the equation may be put into the following form: ∑1∞δwn{logwn−ζlogwn+1+wn−ζwn−1wn−[(1−ζ)n−1]logζ}=0.\Label[eqn](359)\upshape (359) From this, by taking account of [eqn:(358)] (358), we get as the condition for a minimum, that logwn−ζlogwn+1+wn−ζwn−1wn−[(1−ζ)n−1]logζ\Label[eqn](360)\upshape (360) must be independent of n.

The solution of this functional equation is wn=(1−ζ)ζn−1\Label[eqn](361)\upshape (361) for it satisfies [eqn:(360)] (360) as well as [eqn:(353)] (353) and [eqn:(354)] (354). With this value [eqn:(356)] (356) becomes Φ=0.\Label[eqn](362)\upshape (362)

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