A flow chart describing the relationship of various physical quantities, including radiant flux and exitance.
A flow chart describing the relationship of various physical quantities, including radiant flux and exitance

In radiometry, radiant flux or radiant power is the radiant energy emitted, reflected, transmitted, or received per unit time, and spectral flux or spectral power is the radiant flux per unit frequency or wavelength, depending on whether the spectrum is taken as a function of frequency or of wavelength. The SI unit of radiant flux is the watt (W), one joule per second (J/s), while that of spectral flux in frequency is the watt per hertz (W/Hz) and that of spectral flux in wavelength is the watt per metre (W/m)—commonly the watt per nanometre (W/nm). Radiant flux is sometimes called luminosity, especially in astronomy contexts.

Mathematical definitions

Radiant flux

Radiant flux, denoted Φe ('e' for "energetic", to avoid confusion with photometric quantities), is defined as Φ e = d Q e d t Q e = ∫ T ∫ Σ S ⋅ n ^ d A d t {\displaystyle {\begin{aligned}\Phi _{\mathrm {e} }&={\frac {dQ_{\mathrm {e} }}{dt}}\\[2pt]Q_{\mathrm {e} }&=\int _{T}\int _{\Sigma }\mathbf {S} \cdot {\hat {\mathbf {n} }}\,dAdt\end{aligned}}} where

  • Qe is the radiant energy passing out of a closed surface Σ in time interval T;
  • t is time;
  • A is the area of the surface Σ;
  • S is the Poynting vector, representing the directional flow of energy per unit time, per unit area;
  • n is the unit normal vector to the differential area element dA.

The rate of energy flow through the surface fluctuates at the frequency of the radiation, but radiation detectors only respond to the average rate of flow. This is represented by replacing the Poynting vector with the time average of its norm, giving Φ e ≈ ∫ Σ ⟨ | S | ⟩ cos ⁡ α d A , {\displaystyle \Phi _{\mathrm {e} }\approx \int _{\Sigma }\langle |\mathbf {S} |\rangle \cos \alpha \ dA,} where ⟨-⟩ is the time average, and α is the angle between n and S.

Spectral flux

Spectral flux in frequency, denoted Φe,ν, is defined as Φ e , ν = ∂ Φ e ∂ ν , {\displaystyle \Phi _{\mathrm {e} ,\nu }={\frac {\partial \Phi _{\mathrm {e} }}{\partial \nu }},} where ν is the frequency.

Spectral flux in wavelength, denoted Φe,λ, is defined as Φ e , λ = ∂ Φ e ∂ λ , {\displaystyle \Phi _{\mathrm {e} ,\lambda }={\frac {\partial \Phi _{\mathrm {e} }}{\partial \lambda }},} where λ is the wavelength.

SI radiometry units

Comparison of photometric and radiometric quantities
SI radiometry unitsvte
QuantityUnitDimensionNotes
NameSymbolNameSymbol
Radiant energyQejouleJML2⋅T−2Energy of electromagnetic radiation.
Radiant energy densitywejoule per cubicmetreJ/m3ML−1⋅T−2Radiant energy per unit volume.
Radiant fluxΦewattW = J/sML2⋅T−3Radiant energy emitted, reflected, transmitted or received, per unit time. This is sometimes also called "radiant power", and called luminosity in astronomy.
Spectral fluxΦe,νwatt per hertzW/HzML2⋅T−2Radiant flux per unit frequency or wavelength. The latter is commonly measured in W⋅nm−1.
Φe,λwatt per metreW/mMLT−3
Radiant intensityIe,Ωwatt per steradianW/srML2⋅T−3Radiant flux emitted, reflected, transmitted or received, per unit solid angle. This is a directional quantity.
Spectral intensityIe,Ω,νwatt per steradian per hertzW⋅sr−1⋅Hz−1ML2⋅T−2Radiant intensity per unit frequency or wavelength. The latter is commonly measured in W⋅sr−1⋅nm−1. This is a directional quantity.
Ie,Ω,λwatt per steradian per metreW⋅sr−1⋅m−1MLT−3
RadianceLe,Ωwatt per steradian per squaremetreW⋅sr−1⋅m−2MT−3Radiant flux emitted, reflected, transmitted or received by a surface, per unit solid angle per unit projected area. This is a directional quantity. This is sometimes also called "intensity".
Spectral radiance Specific intensityLe,Ω,νwatt per steradian per squaremetre per hertzW⋅sr−1⋅m−2⋅Hz−1MT−2Radiance of a surface per unit frequency or wavelength. The latter is commonly measured in W⋅sr−1⋅m−2⋅nm−1. This is a directional quantity. This is sometimes also called "spectral intensity".
Le,Ω,λwatt per steradian per squaremetre, per metreW⋅sr−1⋅m−3ML−1⋅T−3
Irradiance Flux densityEewatt per square metreW/m2MT−3Radiant flux received by a surface per unit area. This is sometimes also called "intensity".
Spectral irradiance Spectral flux densityEe,νwatt per squaremetre per hertzW⋅m−2⋅Hz−1MT−2Irradiance of a surface per unit frequency or wavelength. This is sometimes also called "spectral intensity". Non-SI units of spectral flux density include jansky (1Jy = 10−26W⋅m−2⋅Hz−1) and solar flux unit (1sfu = 10−22W⋅m−2⋅Hz−1 = 104Jy).
Ee,λwatt per squaremetre, per metreW/m3ML−1⋅T−3
RadiosityJewatt per square metreW/m2MT−3Radiant flux leaving (emitted, reflected and transmitted by) a surface per unit area. This is sometimes also called "intensity".
Spectral radiosityJe,νwatt per squaremetre per hertzW⋅m−2⋅Hz−1MT−2Radiosity of a surface per unit frequency or wavelength. The latter is commonly measured in W⋅m−2⋅nm−1. This is sometimes also called "spectral intensity".
Je,λwatt per squaremetre, per metreW/m3ML−1⋅T−3
Radiant exitanceMewatt per squaremetreW/m2MT−3Radiant flux emitted by a surface per unit area. This is the emitted component of radiosity. "Radiant emittance" is an old term for this quantity. This is sometimes also called "intensity".
Spectral exitanceMe,νwatt per squaremetre per hertzW⋅m−2⋅Hz−1MT−2Radiant exitance of a surface per unit frequency or wavelength. The latter is commonly measured in W⋅m−2⋅nm−1. "Spectral emittance" is an old term for this quantity. This is sometimes also called "spectral intensity".
Me,λwatt per squaremetre, per metreW/m3ML−1⋅T−3
Radiant exposureHejoule per squaremetreJ/m2MT−2Radiant energy received by a surface per unit area, or equivalently irradiance of a surface integrated over time of irradiation. This is sometimes also called "radiant fluence".
Spectral exposureHe,νjoule per squaremetre per hertzJ⋅m−2⋅Hz−1MT−1Radiant exposure of a surface per unit frequency or wavelength. The latter is commonly measured in J⋅m−2⋅nm−1. This is sometimes also called "spectral fluence".
He,λjoule per squaremetre, per metreJ/m3ML−1⋅T−2
See also: SIRadiometryPhotometry

See also

Further reading

  • Boyd, Robert (1983). Radiometry and the Detection of Optical Radiation (Pure & Applied Optics Series). Wiley-Interscience. ISBN978-0-471-86188-1.