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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.