IT is said that, the light intensity of a globe in some direction is given, if it be made of perectly diffusing material, by bA (θ), where b denotes its brightness and A (θ) its projected area in the directien, or else, if it be made of perfectly non-diffusing material, by η*i (e), where i (8) is the light intensity of the working lamp in the direction and η* some proper positive fraction.
But these are true only for ideal cases, which, by the author's opinion, are two extremities of real cases. Then he has assumed as following:
where
k1 and
k2 are some positive fractions which are to be summed up to unity.
The quantities
I (θ) and
i (θ) are to be obtained by ordinary photometry, and A (θ)'s are measured from the photographes of projections (shown in Fig.3's). So then
k1b and k
2η* can be determined, and to this end he escheemed method of “Uchisaka-curve” (as shown in Fig. 2's), which was named so in honor of his old teacher, Mr.Motowo Uchisaka.
This paper is the first report of the studies on light distributions of globes, by the above opinion, about various specimens.
Postscriptly, he introduces “diffusing power” which was defined by Dr. Halbertsina as “Lichtstreuvermogen, ” which has scarcely been known in Japan, and also the author's method to measure it.
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