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handbook of modern sensors

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4.1 Radiometry 125<br />

propagation, polarization, spectral contents <strong>of</strong> light beam can all be modified, and<br />

even the speed <strong>of</strong> light and phase <strong>of</strong> its wavelength can be changed.<br />

4.1 Radiometry<br />

Let us consider light traveling through a three-layer material. All layers are made <strong>of</strong><br />

different substances called media. Figure 4.2 shows what happens to a ray <strong>of</strong> light<br />

which travels from the first medium into a flat plate <strong>of</strong> a second medium, and then to<br />

a third medium. Part <strong>of</strong> the incident light is reflected from a planar boundary between<br />

the first and second media according to the law <strong>of</strong> reflection, which historically is<br />

attributed to Euclid:<br />

1 = ′ 1 (4.1)<br />

A part <strong>of</strong> light enters the plate (Medium 2) at a different angle. The new angle 2 is<br />

governed by the refraction law, which was discovered in 1621 by Willebrord Snell<br />

(1580–1626) and is known as Snell’s law:<br />

n 1 sin 1 = n 2 sin 2 , (4.2)<br />

where n 1 and n 2 are the indices <strong>of</strong> refraction <strong>of</strong> two media.<br />

In any medium, light moves slower than in vacuum. An index <strong>of</strong> refraction is a<br />

ratio <strong>of</strong> velocity <strong>of</strong> light in vacuum, c 0 , to that in a medium, c:<br />

n = c 0<br />

c , (4.3)<br />

Fig. 4.2. Light passing through materials with different refractive indices.

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