Journal of the Society of Motion Picture Engineers (1930-1949)

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N, Image 3/4 way out to spectator 4 3.5 Image 2/3 way out to spectator 3 2.5 Image 1/2 way out to spectator 2 1.5 Image at plane of screen 1 / / / 0.5 / / Image at «, / Q B B-0 B = 0 B=0 B-f / / / / / / p / / / / / / 1 / / f / / / / / / / / / // / / / J D = 0/ N>0/ // / I I / // / 1 1 1 | / /Xr>=o I^N=0 1 1 /tan c/t Region of negative fi D and N values /J 1 ' ' (High C value) •« A£ — (Medium C value , Ar / D > 0 (Distances in reciprocal units) 1 N = 0 J le) (Low C vah Fig. 3. The three types of stereoscopic transmission system: #+, 5 = 0 and B — . be that a point situated at infinity in the scene will appear at some nearer distance in the cinema. All examples of stereoscopic transmission (in other words, all Class B = 0 B+ B instances of 3-D recording and reproduction) must fall into one of these three classes, whose main characteristics may be exhibited thus: Name Characteristic Ortho-infinite Linear; infinity points correctly represented. Hyper-infinite Nonlinear ; objects short of infinity represented at infinity. Hypo-infinite Nonlinear; objects at infinity represented closer than infinity; cardboarding. In the example of a B — system shown in Fig. 3, it will be noticed that infinity (i.e. D = 0) will appear on the screen plane, that is, at N\. This will occur, for example, if a shot of distant objects is taken with the camera axes parallel (<p = 0), and projected with the projector axes toed-in so that the parallax of the aper ture centerlines is zero (ZCL = 0). This frequently happens with amateur projection of stereoscopic stills and movies. In short, the B factor can be varied at three stages in the production process, either angularly or by displacement, as follows : Spottiswoode, Spottiswoode and Smith: 3-D Photography 259