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Prism and Mirror Systems  137









                                          Figure 7.16  “Unfolding” a 90
                                          prism to show that it is equiva-
                                          lent to a block of glass.



        path is called a tunnel diagram. Such a diagram can be used to deter-
        mine the angular field of the prism as well as the size of the beam
        which will pass through the prism.
          Used in this way, this prism is a  constant-deviation prism.
        Regardless of the angle at which a ray enters the prism, the emergent
        ray will be parallel, as shown in Fig. 7.18a. This characteristic is a
        property of the two reflecting surfaces of the prism. A system which
        directs the light ray back on itself is called a retrodirector; this prism
        is a retrodirector in one meridian only. (Another of the many constant-
        deviation systems possible with two reflectors is the 90° deviation
        arrangement shown in Fig. 7.18b, where the reflecting surfaces are at
        45° to each other.) The constant-deviation angle is just twice the angle
        between the two mirrors.
          A prism made by cutting off one corner of a cube, so that there are
        three mutually perpendicular reflecting surfaces, is retrodirective in
        both meridians. The corner cube (or cube corner) reflector will return
        all the light rays striking it back toward their source, although the
        rays will be displaced laterally.
          A third orientation of the 45°–90°–45° prism is shown in Fig. 7.19,
        in which the bundle of rays arrives parallel to the hypotenuse face of
        the prism. After being refracted downward at the entrance face, the
        rays are reflected upward from the hypotenuse and emerge after a
        second refraction at the exit face. The unfolded path of the rays














        Figure 7.17 Right-angle prism used with hypotenuse as
        entrance and exit face.
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