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230   Chapter Ten

        the normal, the brightness is about 20 percent; at 30°, about 7 percent.
        With two sheets, the diffusion can be increased by spacing them apart,
        although this will destroy their utility as a projection screen.
          A sheet of tracing paper has diffusion characteristics quite similar to
        ground glass, and there are several commercially available plastic screen
        materials which are somewhat better diffusers than ground glass. The
        plastic surface also can be shaped to control the beam spread.
          A rear projection screen, when used in a lighted room, is illuminated
        from both sides. The room light reduces the contrast of the projected
        image. This situation is sometimes alleviated by introducing a sheet
        of gray glass (that is, a neutral filter) between the diffusing screen
        and the observer. When this is done, the light from the projector is
        reduced by a factor of T, the transmission of the gray glass, but the
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        room light is reduced by T , since the room light must pass through
        the gray glass twice to go from the room to the diffuser and back to
        the observer’s eye.

        10.8 Polarizing Materials

        Light behaves as a transverse wave in which the waves vibrate
        perpendicular to the direction of propagation. If the wave motion is
        considered as a vector sum of two such vibrations in perpendicular
        planes, then plane polarized light results when one of the two components
        is removed from a light beam. Plane polarized light can be produced by
        passing the radiation from an ordinary source through a polarizing
        prism, several types of which are available. These prisms depend on
        the birefringent characteristic of calcite (CaCO 3 ), which has a different
        index of refraction for the two planes of polarization. Since light of one
        polarization is refracted more strongly than the other, it is possible to
        separate them either by total internal reflection (as in the Nicol and
        Glan-Thompson prisms) or by deviation in different directions (as in
        the Rochon and Wollaston prisms).
          Such prisms are large, heavy, and expensive. Sheet polarizers,
        which are made by aligning microscopic crystals in a suitable base, are
        thin, light, relatively inexpensive, useful over a wide field of view, and
        simple to fabricate into an almost unlimited range of sizes and shapes.
        Thus, despite the fact that they are not quite as efficient as a good
        prism polarizer and are not effective over as large a wavelength range,
        they have largely supplanted prisms for the great majority of applica-
        tions where polarization is required. Several companies, produce a
        number of types of sheet polarizers. For work in the visible region,
        several types are available, depending on whether optimum transmission
        or optimum extinction (through crossed polarizers) is desired. Special
        types are available for use at high temperatures and also for use in the
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