Page 224 - Modern Optical Engineering The Design of Optical Systems
P. 224

Optical Materials  207

        in series will be 0.45   0.45   20 percent unless they have a uniform
        spectral transmission (neutral density). To take an extreme example,
        if the filter transmits nothing from 1 to 1.5  m and 90 percent from 1.5
        to 2  m, its “average” transmission will be 45 percent within the 1- to
        2- m band. However, two such filters, when combined, will transmit
        zero from 1 to 1.5  m, and about 81 percent from 1.5 to 2  m, for an
        “average” transmission of about 40 percent, rather than the 20 percent
        which two neutral density filters would transmit.
          The photographic density of a filter is the log of its opacity (the
        reciprocal of transmittance), thus
                                       1
                               D   log      log T
                                       T
        where D is the density and T is the transmittance of the material. Note
        that transmittance does not account for surface reflection losses; thus,
        density is directly proportional to thickness. To a fair approximation,
        the density of a “stack” of neutral density absorption filters is the sum
        of the individual densities.
          Equation 10.3 can be written to the base 10 if desired. This is done
        when the term “density” is used to describe the transmission of, for
        example, a photographic filter. The equation becomes

                                   T   10  density

        so that a density of 1.0 means a transmission of 10 percent, a density
        of 2.0 means a transmission of 1 percent, etc. Note that densities can
        be added. A neutral absorbing filter with a density of 1.0 combined
        with a filter of density 2.0 will yield a density of 3.0 and a transmission
                                  3
        of 0.1   0.01   0.001   10 .
        Index dispersion
        The index of refraction of an optical material varies with wavelength as
        indicated in Fig. 10.1 where a  very long spectral range is shown. The
        dashed portions of the curve represent absorption bands. Notice that the
        index rises markedly after each absorption band, and then begins to drop
        with increasing wavelength. As the wavelength continues to increase, the
        slope of the curve levels out until the next absorption band is approached,






                                         Figure 10.1 Dispersion curve of
                                         an optical material. The dashed
                                         lines indicate absorption bands.
                                         (Anomolous dispersion.)
   219   220   221   222   223   224   225   226   227   228   229