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132   Chapter Seven

                                          Figure 7.10 A useful technique in
                                          determining the orientation of a
                                          reflected image is to visualize
                                          the image as a pencil “bouncing”
                                          off a solid wall as it moves along
                                          the system axis.

        and the blunt end continuing in the original direction, and the third
        shows the pencil in the new orientation after the reflection. If the process
        is repeated with the pencil perpendicular to the plane of the paper, the
        orientation of the other meridian of the image can be determined. The pro-
        cedure can then be repeated through each reflection in the system.
          A card marked with the arrow and crossbar of Fig. 7.11 is also useful
        for this purpose. The reader’s attention is directed to the fact that the
        initial orientation of the pencil, or pattern, is chosen so that one meridian
        of the pattern coincides with the plane of incidence. In the majority of
        reflecting systems, one or the other of the meridians will be in the plane
        of incidence throughout the system, and the application of this technique
        is straightforward. Where this is not the case, the card can be marked
        with a second set of meridians so that the second set is aligned with the
        plane of incidence. This second set can then be carried through the reflec-
        tion as before; the orientation of the final image is of course given by the
        original set of markings. Figure 7.20b exemplifies this method.


        7.8  Plane Parallel Plates
        As will become apparent, most prism systems are the equivalent of a
        thick block of glass. Thus we continue with a discussion of the effects
        produced by a plane-parallel plate of glass. Figure 7.12 shows a lens
        which, in air, would form an image at P. The insertion of the plane
        parallel plate between the lens and P displaces the image to P′. If
        we trace the path of the light rays through the plate, we first notice
        that the ray emerging from the plate has exactly the same  slope
        angle that it had before passing through the plate, since by Snell’s law,












                                         Figure 7.11 Image orientation
                                         after reflection.
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