guide to thin section microscopy - Mineralogical Society of America
guide to thin section microscopy - Mineralogical Society of America
guide to thin section microscopy - Mineralogical Society of America
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Guide <strong>to</strong> Thin Section Microscopy<br />
Optical properties: basic principles<br />
Refraction <strong>of</strong> light: The velocity <strong>of</strong> light (as measured in air) is reduced if it enters<br />
substances <strong>of</strong> higher density (liquids, glasses, minerals). If the angle between the incident<br />
light rays and the phase boundary (e.g., air/glass) is different from 90˚, the light rays change<br />
the propagation direction; they are refracted. Snell's Law <strong>of</strong> refraction applies (Fig. 4-2) as<br />
long as the materials involved are isotropic (cf. Ch. 4.1.2). In a <strong>thin</strong> <strong>section</strong>, the object (d = 25<br />
μm) lies embedded between epoxy resin and glass. As light velocity is almost identical in<br />
glass and epoxy resin, refraction occurs mainly at boundary surfaces between the object and<br />
epoxy resin, but also at phase boundaries wi<strong>thin</strong> the object (Fig. 4-2).<br />
The light velocity v <strong>of</strong> a specified material is an important parameter for its identification. For<br />
technical convenience, the refractive index n is used instead <strong>of</strong> velocity. The refractive index<br />
is defined as the ratio between light velocity v 0 in vacuum (about the same as in air) and light<br />
velocity in the material studied. In isotropic materials, it can be determined experimentally by<br />
measuring the angles <strong>of</strong> refraction α and β, whereby Snell's Law n 2 /n 1 = sinα/sinβ applies. As<br />
light velocities in all solid and liquid substances are smaller than v 0 (n 1 = n air = 1), refractive<br />
indices are generally larger than 1.<br />
Raith, Raase & Reinhardt – February 2012<br />
Figure 4-2. Refraction <strong>of</strong> light, dispersion<br />
When passing through a glass prism, rays <strong>of</strong><br />
white light are “split up” in<strong>to</strong> their spectral<br />
colours due <strong>to</strong> differential refraction at the<br />
two prism surfaces. This demonstrates that<br />
ray velocity is dependent on wavelength<br />
(causing dispersion). Therefore, monochromatic<br />
light must be used when determining<br />
refractive indices.<br />
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