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Paraxial Optics and Calculations  51









        Figure 3.10    Raytrace through a two mirror system.



        Following our sign convention, the radii are both negative and the dis-
        tance from primary to secondary mirror is also considered negative, since
        the light traverses this distance right to left. The index of the air is taken
        as  1.0 before the primary and after the secondary; between the two, the
        index is  1.0. Thus the optical data of the problem and the computation
        are set up and carried through as shown in Fig. 3.10. Careful attention
        to signs is necessary in this calculation to avoid mistakes.
          The focal length of the system is given by  y 1 /u′ 2   1.0/ 0.002
        500 mm. The final intercept distance (from R 2 to the focus) is equal to
         y 2 /u′ 2   0.2/ 0.002   100 mm, and the focal point lies 20 mm to the
        right of the primary mirror. Notice that the (second) principal plane is
        completely outside the system, 400 mm to the left of the secondary
        mirror, and that this type of system provides a long focal length and a
        large image in a small, compact system.


        Bibliography

        Bass, M., Handbook of Optics, Vol. 1, New York, McGraw-Hill, 1995.
        Fischer, R. E., and B. Tadic-Galeb, Optical System Design, New York, McGraw-Hill, 2000.
        Greivenkamp, J., Field Guide to Geometrical Optics, Bellingham, WA, SPIE, 2004.
        Kingslake, R., Optical System Design, Orlando, Academic, 1983.
        Smith, W. J., Modern Lens Design, New York, McGraw-Hill, 2002.
        Smith, W. J., Practical Optical System Layout, New York, McGraw-Hill, 1997.


        Exercises
        1 A detector, 1 mm on a side, is “immersed” on the plano surface of a plano
        convex lens with an index of 1.50 and a radius of 10.0 mm. When viewed
        through the convex surface, where is the image, and what is the image size if
        the immersion lens is:
           (a)  7.0-mm thick
           (b) 10.0-mm thick
           (c) 16.666 . . . mm thick
        ANSWER:  (a) Using Eq. 3.16, trace a ray from the axial intercept of the plane
        surface through the curved surface, at a height of 1 mm on that surface. The
        ray slope in the glass is 1/7    0.142857 and the slope-index product nu is
        thus  0.214286. The slope after refraction (in air n   1.0) will be given by
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