Radiation Terms

Blackbody
A hypothetical entity which absorbs all energy, reflects none and emits energy with perfect efficiency.  A blackbody is assumed to satisfy the following ideal conditions;
  1. A blackbody absorbs all incident radiation regardless of wavelength and direction.
  2. For a prescribed temperature and wavelength, no surface can emit more energy than a blackbody.
  3. Although the radiation emitted by a blackbody is a function of wavelength, it is independent of direction. A blackbody is defined as a diffuse emitter.

Since a true blackbody is only a theoretical device, practical devices must have smaller emissive powers. It is therefore necessary to identify a property called emissivity that is defined as;

Emissivity
The ratio of emittance of a given object and a theoretical blackbody at the same temperature. The emissivity of a theoretical blackbody is defined as 1.0 and that of a perfect reflector as 0.
          (Thus emissivity = 1.0 - reflectivity.)
In practice emissivity is a function of both wave length and temperature. However, for most practical applications a single average value (which covers a selected wave band) can usually be used.
Radiant Flux
Rate at which photons strike a surface measured in watts (amount of energy delivered per unit of time).
Irradiance
Radiant flux per unit area (watts per square meter) incoming.
Radiant Exitance
The rate at which radiation is emitted from a unit area (watts per square meter).
 

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