Society of Motion Picture Engineers : incorporation and by-laws (1919)

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Fig. 17. brilliancy, such as an arc crater, the value of condenser efficiency in actual projection can be as high as those given in Fig. 9, but from Figs. 22 to 24, it is evident that when using the 900-watt motionpicture lamp, the illumination that can be obtained with a uniform screen is less than the maximum illumination represented by the tops of these curves. Fig. 25 shows the reductions with piano convex and the two prismatic condensers for 2^-inch and 1^-inch objectives. Fig. 25 Piano Prismatic Prismatic Convex No. 2 No. 3 Condenser Objective 2^" U4" 2^" 1^" 2^^" U/^" Max. Illumination 59 .37 .56 .35 .61 .38 Max. Uniform Illumination .28 .30 .45 .11 .58 .38 These figures show the great gain in uniform illumination, with an un-uniform source, made possible by the use of a condenser, such as the prismatic, which does not give a true image. The very low value with prismatic No. 2, when used with a small objective, is 113