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In radiometry, radiance is the radiant flux emitted, reflected, transmitted or received by a given surface, per unit solid angle per unit projected area. Radiance is used to characterize diffuse emission and reflection of electromagnetic radiation, and to quantify emission of neutrinos and other particles. The International System of Units, SI unit of radiance is the watt per steradian per square metre (). It is a ''directional'' quantity: the radiance of a surface depends on the direction from which it is being observed.

The related quantity spectral radiance is the radiance of a surface per unit frequency or wavelength, depending on whether the Spectral radiometric quantity, spectrum is taken as a function of frequency or of wavelength.

Historically, radiance was called "intensity" and spectral radiance was called "specific intensity". Many fields still use this nomenclature. It is especially dominant in heat transfer, astrophysics and astronomy. "Intensity" has many other meanings in physics, with the most common being intensity (physics), power per unit area.

Description

Radiance is useful because it indicates how much of the power emitted, reflected, transmitted or received by a surface will be received by an optical system looking at that surface from a specified angle of view. In this case, the solid angle of interest is the solid angle subtended by the optical system's entrance pupil. Since the human eye, eye is an optical system, radiance and its cousin luminance are good indicators of how bright an object will appear. For this reason, radiance and luminance are both sometimes called "brightness". This usage is now discouraged (see the article Brightness for a discussion). The nonstandard usage of "brightness" for "radiance" persists in some fields, notably laser physics.

The radiance divided by the index of refraction squared is Invariant (physics), invariant in geometric optics. This means that for an ideal optical system in air, the radiance at the output is the same as the input radiance. This is sometimes called ''conservation of radiance''. For real, passive, optical systems, the output radiance is ''at most'' equal to the input, unless the index of refraction changes. As an example, if you form a demagnified image with a lens, the optical power is concentrated into a smaller area, so the irradiance is higher at the image. The light at the image plane, however, fills a larger solid angle so the radiance comes out to be the same assuming there is no loss at the lens.

Spectral radiance expresses radiance as a function of frequency or wavelength. Radiance is the integral of the spectral radiance over all frequencies or wavelengths. For radiation emitted by the surface of an ideal black body at a given temperature, spectral radiance is governed by Planck's law, while the integral of its radiance, over the hemisphere into which its surface radiates, is given by the Stefan–Boltzmann law. Its surface is Lambert's cosine law, Lambertian, so that its radiance is uniform with respect to angle of view, and is simply the Stefan–Boltzmann integral divided by π. This factor is obtained from the solid angle 2π steradians of a hemisphere decreased by Stefan–Boltzmann law#Integration of intensity derivation, integration over the cosine of the zenith angle.

Mathematical definitions

Radiance

Radiance of a ''surface'', denoted ''L''_e,Ω ("e" for "energetic", to avoid confusion with photometric quantities, and "Ω" to indicate this is a directional quantity), is defined as
:$L_ = \frac,$
where
*∂ is the partial derivative symbol;
*Φ_e is the radiant flux emitted, reflected, transmitted or received;
*Ω is the solid angle;
*''A'' cos ''θ'' is the ''projected'' area.

In general ''L''_e,Ω is a function of viewing direction, depending on ''θ'' through cos ''θ'' and azimuth angle through . For the special case of a Lambertian reflectance, Lambertian surface, is proportional to cos ''θ'', and ''L''_e,Ω is isotropic (independent of viewing direction).

When calculating the radiance emitted by a source, ''A'' refers to an area on the surface of the source, and Ω to the solid angle into which the light is emitted. When calculating radiance received by a detector, ''A'' refers to an area on the surface of the detector and Ω to the solid angle subtended by the source as viewed from that detector. When radiance is conserved, as discussed above, the radiance emitted by a source is the same as that received by a detector observing it.

Spectral radiance

Spectral radiance in frequency of a ''surface'', denoted ''L''_e,Ω,ν, is defined as
:$L_ = \frac,$
where ''ν'' is the frequency.

Spectral radiance in wavelength of a ''surface'', denoted ''L''_e,Ω,λ, is defined as
:$L_ = \frac,$
where ''λ'' is the wavelength.

Conservation of basic radiance

Radiance of a surface is related to étendue by
:$L_ = n^2 \frac,$
where
*''n'' is the refractive index in which that surface is immersed;
*''G'' is the étendue of the light beam.

As the light travels through an ideal optical system, both the étendue and the radiant flux are conserved. Therefore, ''basic radiance'' defined byWilliam Ross McCluney, ''Introduction to Radiometry and Photometry'', Artech House, Boston, MA, 1994
:$L_^* = \frac$
is also conserved. In real systems, the étendue may increase (for example due to scattering) or the radiant flux may decrease (for example due to absorption) and, therefore, basic radiance may decrease. However, étendue may not decrease and radiant flux may not increase and, therefore, basic radiance may not increase.

SI radiometry units

See also

*Étendue
*Light field
*Sakuma–Hattori equation
*Wien displacement law

References

{{reflist

External links

International Lighting in Controlled Environments Workshop

Physical quantities
Radiometry