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Mter Pwjectm
A Department an FHDJECTIDIV & SDllMD
Combining Projection and Anamorphic Lenses Properly
by GIO GAGLIARDI
CinemaScope has been with us for over two years but I venture to say that the optical reasoning and the proper operation of the projection lens with its anamorphic attachment are still not too well understood. By now we are all familiar with the fact that the anamorphic device will spread out a picture to double its size in a horizontal direction when properly aligned. Yet relatively few people in the theatre field have been interested in the principles involved, and for that reason may not be certain of the exact and proper adjustments required to obtain and maintain the best quality CinemaScope picture on the screen.
The regular projection lens, Avhich is made up of spherical elements, magnifies the small picture on the film to the large image on the screen and the magnification is equal and exactly proportional to the ratio of the film dimensions. Both height and width are expanded at the same rate. However, when an anamorphic device is added to a standard lens, the width of the screen image increases at a greater rate than the height. This change of magnification rate for CinemaScope is 2-to-l.
CYLINDRICAL LENS SYSTEM
Anamorphic devices used for projection in the United States consist in a cylindrical lens st’stem, or in a prismatic wedge system. The former is the one originally proposed by Prof. Henri Chretien and is used in the greater number of installations and will be discussed here.
The effects produced by using cylindrical mirrors has been well illustrated by the amusement parks. Most of us are familiar with the elongated or widened images re
flected by these mirrors, depending upon the direction of curvature used in the mirrors. The procedure used by Chretien was somewhat similar, but it was applied to the use of accurately designed refractive cylindrical lenses.
In order to produce a picture having a horizontal magnification double the vertical magnification it would have been necessary to produce a projection lens combination which should have a focal length in the horizontal plane equal to only one-half the focal length in the vertical plane. Such a lens would be almost impossible to design, or at least would be terribly complicated.
ANAMORPHIC OPTICS
The designer went back to the principle and simple construction of the old refractive telescope, which consisted in a converging and diverging lens, as shown in Figure 1. In this simple telescope the ratio of the focal lengths of the front and back elements is made equal to 2, and for this combination the telescopic power is equal to 2. When such a system is placed in front of a regular projection lens, it will reduce the focal length of the entire com
bination to one-half its original focal length.
However, in order to produce the desired anamorphic effect, the standard spherical elements of the telescopic lenses had to be changed to similar cylindrical shapes. These lenses then looked somewhat like the sketch of Figure 2. The refractive curvature of each element was active only in a hori
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Amp. Volts Pos, Grade Neg. Grade
40 (I Kw) 28
42-50
55-65
70
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75-80
80-85
80-90
lOO-IIO
115
115-130
130-150
135-40
150-160
170-180
31-38
3437 38
3537 39-40 37-40 50-55
5460 62
60-66
65-67
5558 68-70 68-69
7x14 7x14 8x14 8x14 9x14 9x14 9x14 9x20 10x20 10x20 1 1x20 13.6x22 13.6x18 13.6x22 13.6x22
54IC
544C
544C
514
544C
5140
544IOC
552-09
552-09
552-09
55209
55301 552-09 523 583-08
6x9 6x9 7x9 7x9 7x9 8x9 8x9 5/16x9 1/32x9 3/8x9 3/8x9 7/16x9 7/16x9 I /2x9 1/2x9
545-20C
545-C
545 C
545G
545C
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557C
557C
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