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Optical System Considerations  55

          Note that these equations are equally applicable to systems composed
        of either thick or “thin” lenses. Obviously, when applied to thin lenses,
        d becomes the spacing between elements, since the element and its
        principal planes are coincident.

        Focal lengths of two-component systems
        The preceding equations may be used to derive compact expressions
        for the effective focal length and back focal length of a system
        comprised of two separated components. Let us assume that we have
        two components of powers   a and   b separated by a distance d (if the
        lenses are “thin”; if they are thick, d is the separation of their princi-
        pal points). The system is sketched in Fig. 4.2.
          Beginning with a ray parallel to the axis which strikes lens a at y a ,
        we have
                            u   0
                              a
                            u′   0   y      by Eq. 4.1
                              a       a  a
                             y   y   dy     y (1   d  )    by Eq. 4.2
                              b   a     a  a   a       a
                            u′   y     y (1   d  )       by Eq. 4.1
                              b     a  a  a        a  b
                                 y (       d    )
                                    a  a    b     a  b
          The power (reciprocal focal length) of the system is given by

                              2 ur    1
                                  b  5   5         d
                         ab    y a    f ab  a    b     a  b
                              1    1     d
                                                                     (4.4)
                             f     f    f f
                              a    b    a b

















        Figure 4.2 Raytrace through two separated components to determine
        the focal length and back focus distance of the combination.
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