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FLIR C2 User Manual

FLIR C2
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Theory of thermography
18
For highly polished materials ε
λ
approaches zero, so that for a perfectly reflecting material
(i.e. a perfect mirror) we have:
For a graybody radiator, the Stefan-Boltzmann formula becomes:
This states that the total emissive power of a graybody is the same as a blackbody at the
same temperature reduced in proportion to the value of ε from the graybody.
Figure 18.8 Spectral radiant emittance of three types of radiators. 1: Spectral radiant emittance; 2: Wave-
length; 3: Blackbody; 4: Selective radiator; 5: Graybody.
Figure 18.9 Spectral emissivity of three types of radiators. 1: Spectral emissivity; 2: Wavelength; 3: Black-
body; 4: Graybody; 5: Selective radiator.
#T559918; r. AN/42281/42281; en-US
76

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FLIR C2 Specifications

General IconGeneral
Package weight540 g
Battery life (max)2 h
Battery recharge time1 h
Weight and Dimensions IconWeight and Dimensions
Depth125 mm
Width80 mm
Height24 mm
Weight130 g

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