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handbook of modern sensors

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3.13 Light 111<br />

[38] whose emissivity is over 0.999. A cavity body is fabricated <strong>of</strong> solid copper<br />

with a cavity <strong>of</strong> any shape; an inversed cone is preferable. An imbedded temperature<br />

sensor and a thermoelectric heater/cooler with a control circuit (not shown) form a<br />

thermostat that maintains the temperature <strong>of</strong> the cavity on a preset level. That may be<br />

above or below the ambient temperature. The inner portion <strong>of</strong> the cavity should be<br />

painted with organic paint. The visible color <strong>of</strong> the paint is not important, because in<br />

the infrared spectral range, there is no correlation with reflectivity in the visible range<br />

(which determines visible color). The most troublesome portion <strong>of</strong> a cavity is located<br />

near the aperture, because it is very difficult to ensure that the temperature <strong>of</strong> the left<br />

side <strong>of</strong> the blackbody (as in Fig. 3.46B) is independent <strong>of</strong> ambient and equal to the<br />

rest <strong>of</strong> the cavity walls. To minimize the effects <strong>of</strong> ambient temperature and increase<br />

the virtual cavity size, the inner surface <strong>of</strong> the front wall around the cavity is highly<br />

polished and gold plated. Thus, the front side <strong>of</strong> the cavity has very low emissivity<br />

and, thus, its temperature is not that critical. In addition, the gold surface reflects<br />

rays emitted by the right-side parts <strong>of</strong> the cavity walls that have high emissivity and<br />

thus enhances the cavity effect. The entire copper body is covered with a thermally<br />

insulating layer. It should be noted that the blackbody surface is the virtual surface<br />

<strong>of</strong> the aperture, which, in reality, is a void.<br />

3.13 Light<br />

Light is a very efficient form <strong>of</strong> energy for sensing a great variety <strong>of</strong> stimuli. Among<br />

many others, these include distance, motion, temperature, and chemical composition.<br />

Light has an electromagnetic nature. It may be considered a propagation <strong>of</strong> either<br />

quanta <strong>of</strong> energy or electromagnetic waves. Different portions <strong>of</strong> the wave-frequency<br />

spectrum are given special names: ultraviolet (UV), visible, near-, mid-, and farinfrared<br />

(IR), microwaves, radiowaves, and so forth. The name “light” was arbitrarily<br />

given to electromagnetic radiation which occupies wavelengths from approximately<br />

0.1 to 100 µm. Light below the shortest wavelength that we can see (violet) is called<br />

ultraviolet, and higher than the longest that we can see (red) is called infrared. The<br />

infrared range is arbitrarily subdivided into three regions: near-infrared (from about<br />

0.9 to 1.5 mµ), mid-infrared (1.5 to 4 µm), and far-infrared (4 to 100 µm).<br />

Different portions <strong>of</strong> the radiation spectrum are studied by separate branches <strong>of</strong><br />

physics. An entire electromagnetic spectrum is represented in Fig. 3.41. It spreads<br />

from γ -rays (the shortest) to radiowaves (the longest). In this section, we will briefly<br />

review those properties <strong>of</strong> light which are mostly concerned with the visible and<br />

near-infrared portions <strong>of</strong> the electromagnetic spectrum. Thermal radiation (mid- and<br />

far-infrared regions) are covered in Section 3.12.<br />

The velocity <strong>of</strong> light c 0 in vacuum is independent <strong>of</strong> wavelengths and can be<br />

expressed as µ 0 = 4π × 10 −7 henrys/m and ε 0 = 8.854 × 10 −12 farads/m , which are<br />

the magnetic and electric permitivities <strong>of</strong> free space:<br />

c 0 = 1 √<br />

µ0 ε 0<br />

= 299,792,458.7 ± 1.1 m s . (3.145)

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