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nydus/The Theory of Heat RadiationPublic

This text examines the physical distinction between heat conduction and heat radiation, noting that radiation is independent of the medium through which it passes. It establishes that heat rays are physically identical to light rays and applies the principles of experimental optics to the study of thermal radiation.

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188.

It now remains to prove that the sum Φ=1(wnζwn1)logwn[(1ζ)n1]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(δwnζδwn1)logwn+(wnζwn1)δwnwn\Label[eqn](357)\upshape (357)[(1ζ)n1]δwnlogζ=0,

where, according to [eqn:(353)] (353) and [eqn:(354)] (354), 1δwn=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: 1δwn{logwnζlogwn+1+wnζwn1wn[(1ζ)n1]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 logwnζlogwn+1+wnζwn1wn[(1ζ)n1]logζ\Label[eqn](360)\upshape (360) must be independent of n.

The solution of this functional equation is wn=(1ζ)ζn1\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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