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124      PROPERTIES OF POLARIZED LIGHT

                                    The amount of light transmitted through two polars crossed at various angles can be
                                calculated using Malus’law, which states that
                                                                      2
                                                              I   I cos  ,
                                                                  o
                                where I is the intensity of light passed by an analyzer, I is the intensity of an incident
                                                                             o
                                beam of linearly polarized light, and   is the angle between the azimuth of polarization
                                of the incident light and the transmission axis of the analyzer. Thus, for two polars
                                                     2
                                crossed at a 90° angle, cos     0, and I   0, so polarized light produced by the first fil-
                                ter (the polarizer) is completely excluded by the second filter (the analyzer). For polar-
                                izers partially crossed at 10° and 45°, the light transmitted by the analyzer is reduced by
                                97% and 50%, respectively.


                                DOUBLE REFRACTION IN CRYSTALS

                                Many transparent crystals and minerals such as quartz, calcite, rutile, tourmaline, and
                                others are optically anisotropic and exhibit a property known as double refraction. When
                                letters on a printed page are viewed through a calcite crystal, remarkably each letter
                                appears double (Figure 8-6). Calcite is therefore said to be doubly refracting, or birefrin-
                                gent. Birefringent materials split an incident ray into two components that traverse dif-
                                ferent paths through the crystal and emerge as two separate rays. This occurs because
                                atoms in crystals are ordered in a precise geometric arrangement causing direction-
                                dependent differences in the refractive index. In contrast, a sheet of glass, such as a
                                microscope slide, which is an amorphous mixture of silicates, is usually optically
                                isotropic and does not exhibit double refraction.
                                    When a ray of light is incident on a birefringent crystal, it usually becomes split into
                                two rays that follow separate paths. One ray, the ordinary ray or O ray, observes the laws
                                of normal refraction, while the other ray, the extraordinary ray or E ray, travels along a
                                different path. Thus, for every ray entering the crystal there is a pair of O and E rays that





















                                Figure 8-6
                                Double refraction in a calcite crystal. A letter viewed through a plane surface of the crystal
                                appears double, the two images corresponding to the ordinary and extraordinary rays. As the
                                crystal is rotated, the E ray rotates around the O ray. The O ray obeys the normal laws of
                                refraction and does not rotate.
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