Radiant flux





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), that is the joule per second (J/s) in SI base units, 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).




Contents






  • 1 Mathematical definitions


    • 1.1 Radiant flux


    • 1.2 Spectral flux




  • 2 Relationship with the Poynting vector


  • 3 SI radiometry units


  • 4 See also


  • 5 References


  • 6 Further reading





Mathematical definitions



Radiant flux


Radiant flux, denoted Φe ("e" for "energetic", to avoid confusion with photometric quantities), is defined as[1]


Φe=∂Qe∂t,{displaystyle Phi _{mathrm {e} }={frac {partial Q_{mathrm {e} }}{partial t}},}Phi _{mathrm {e} }={frac {partial Q_{mathrm {e} }}{partial t}},

where



  • ∂ is the partial derivative symbol;


  • Qe is the radiant energy emitted, reflected, transmitted or received;


  • t is the time.



Spectral flux


Spectral flux in frequency, denoted Φe,ν, is defined as[1]


Φe,ν=∂Φe∂ν,{displaystyle Phi _{mathrm {e} ,nu }={frac {partial Phi _{mathrm {e} }}{partial nu }},}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[1]


Φe,λ=∂Φe∂λ,{displaystyle Phi _{mathrm {e} ,lambda }={frac {partial Phi _{mathrm {e} }}{partial lambda }},}Phi _{mathrm {e} ,lambda }={frac {partial Phi _{mathrm {e} }}{partial lambda }},

where λ is the wavelength.



Relationship with the Poynting vector


One can show that the radiant flux of a surface is the flux of the Poynting vector through this surface, hence the name "radiant flux":


Φe=∮ΣS⋅n^dA=∮Σ|S|cos⁡αdA,{displaystyle Phi _{mathrm {e} }=oint _{Sigma }mathbf {S} cdot mathbf {hat {n}} ,mathrm {d} A=oint _{Sigma }|mathbf {S} |cos alpha ,mathrm {d} A,}Phi _{mathrm {e} }=oint _{Sigma }mathbf {S} cdot mathbf {hat {n}} ,mathrm {d} A=oint _{Sigma }|mathbf {S} |cos alpha ,mathrm {d} A,

where




  • Σ is the surface;


  • S is the Poynting vector;


  • n is a unit normal vector to that surface;


  • A is the area of that surface;


  • α is the angle between n and S.


But the time-average of the norm of the Poynting vector is used instead, because in radiometry it is the only quantity that radiation detectors are able to measure:


Φe=∮Σ|S|⟩cos⁡αdA,{displaystyle Phi _{mathrm {e} }=oint _{Sigma }langle |mathbf {S} |rangle cos alpha ,mathrm {d} A,}Phi _{mathrm {e} }=oint _{Sigma }langle |mathbf {S} |rangle cos alpha ,mathrm {d} A,

where < • > is the time-average.



SI radiometry units


























































































































































































































































































































SI radiometry units


Quantity
Unit
Dimension
Notes

Name

Symbol[nb 1]

Name

Symbol

Symbol

Radiant energy

Qe[nb 2]

joule

J

ML2T−2
Energy of electromagnetic radiation.

Radiant energy density

we
joule per cubic metre
J/m3

ML−1T−2
Radiant energy per unit volume.

Radiant flux
Φe[nb 2]

watt

W = J/s

ML2T−3
Radiant energy emitted, reflected, transmitted or received, per unit time. This is sometimes also called "radiant power".

Spectral flux
Φe,ν[nb 3]
 or
Φe,λ[nb 4]
watt per hertz
 or
watt per metre
W/Hz
 or
W/m

ML2T−2
 or
MLT−3
Radiant flux per unit frequency or wavelength. The latter is commonly measured in W⋅nm−1.

Radiant intensity

Ie,Ω[nb 5]
watt per steradian
W/sr

ML2T−3
Radiant flux emitted, reflected, transmitted or received, per unit solid angle. This is a directional quantity.

Spectral intensity

Ie,Ω,ν[nb 3]
 or
Ie,Ω,λ[nb 4]
watt per steradian per hertz
 or
watt per steradian per metre
W⋅sr−1⋅Hz−1
 or
W⋅sr−1⋅m−1

ML2T−2
 or
MLT−3
Radiant intensity per unit frequency or wavelength. The latter is commonly measured in W⋅sr−1⋅nm−1. This is a directional quantity.

Radiance

Le,Ω[nb 5]
watt per steradian per square metre
W⋅sr−1⋅m−2

MT−3
Radiant 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 confusingly called "intensity".

Spectral radiance

Le,Ω,ν[nb 3]
 or
Le,Ω,λ[nb 4]
watt per steradian per square metre per hertz
 or
watt per steradian per square metre, per metre
W⋅sr−1⋅m−2⋅Hz−1
 or
W⋅sr−1⋅m−3

MT−2
 or
ML−1T−3
Radiance 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 confusingly called "spectral intensity".

Irradiance
Flux density

Ee[nb 2]
watt per square metre
W/m2

MT−3
Radiant flux received by a surface per unit area. This is sometimes also confusingly called "intensity".

Spectral irradiance
Spectral flux density

Ee,ν[nb 3]
 or
Ee,λ[nb 4]
watt per square metre per hertz
 or
watt per square metre, per metre
W⋅m−2⋅Hz−1
 or
W/m3

MT−2
 or
ML−1T−3
Irradiance of a surface per unit frequency or wavelength. This is sometimes also confusingly called "spectral intensity". Non-SI units of spectral flux density include jansky (1 Jy = 10−26 W⋅m−2⋅Hz−1) and solar flux unit (1 sfu = 10−22 W⋅m−2⋅Hz−1 = 104 Jy).

Radiosity

Je[nb 2]
watt per square metre
W/m2

MT−3
Radiant flux leaving (emitted, reflected and transmitted by) a surface per unit area. This is sometimes also confusingly called "intensity".

Spectral radiosity

Je,ν[nb 3]
 or
Je,λ[nb 4]
watt per square metre per hertz
 or
watt per square metre, per metre
W⋅m−2⋅Hz−1
 or
W/m3

MT−2
 or
ML−1T−3
Radiosity of a surface per unit frequency or wavelength. The latter is commonly measured in W⋅m−2⋅nm−1. This is sometimes also confusingly called "spectral intensity".

Radiant exitance

Me[nb 2]
watt per square metre
W/m2

MT−3
Radiant 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 confusingly called "intensity".

Spectral exitance

Me,ν[nb 3]
 or
Me,λ[nb 4]
watt per square metre per hertz
 or
watt per square metre, per metre
W⋅m−2⋅Hz−1
 or
W/m3

MT−2
 or
ML−1T−3
Radiant 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 confusingly called "spectral intensity".

Radiant exposure

He
joule per square metre
J/m2

MT−2
Radiant 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 exposure

He,ν[nb 3]
 or
He,λ[nb 4]
joule per square metre per hertz
 or
joule per square metre, per metre
J⋅m−2⋅Hz−1
 or
J/m3

MT−1
 or
ML−1T−2
Radiant 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".

Hemispherical emissivity

ε



1
Radiant exitance of a surface, divided by that of a black body at the same temperature as that surface.

Spectral hemispherical emissivity

εν
 or
ελ



1
Spectral exitance of a surface, divided by that of a black body at the same temperature as that surface.

Directional emissivity

εΩ



1
Radiance emitted by a surface, divided by that emitted by a black body at the same temperature as that surface.

Spectral directional emissivity

εΩ,ν
 or
εΩ,λ



1
Spectral radiance emitted by a surface, divided by that of a black body at the same temperature as that surface.

Hemispherical absorptance

A



1
Radiant flux absorbed by a surface, divided by that received by that surface. This should not be confused with "absorbance".

Spectral hemispherical absorptance

Aν
 or
Aλ



1
Spectral flux absorbed by a surface, divided by that received by that surface. This should not be confused with "spectral absorbance".

Directional absorptance

AΩ



1
Radiance absorbed by a surface, divided by the radiance incident onto that surface. This should not be confused with "absorbance".

Spectral directional absorptance

AΩ,ν
 or
AΩ,λ



1
Spectral radiance absorbed by a surface, divided by the spectral radiance incident onto that surface. This should not be confused with "spectral absorbance".

Hemispherical reflectance

R



1
Radiant flux reflected by a surface, divided by that received by that surface.

Spectral hemispherical reflectance

Rν
 or
Rλ



1
Spectral flux reflected by a surface, divided by that received by that surface.

Directional reflectance

RΩ



1
Radiance reflected by a surface, divided by that received by that surface.

Spectral directional reflectance

RΩ,ν
 or
RΩ,λ



1
Spectral radiance reflected by a surface, divided by that received by that surface.

Hemispherical transmittance

T



1
Radiant flux transmitted by a surface, divided by that received by that surface.

Spectral hemispherical transmittance

Tν
 or
Tλ



1
Spectral flux transmitted by a surface, divided by that received by that surface.

Directional transmittance

TΩ



1
Radiance transmitted by a surface, divided by that received by that surface.

Spectral directional transmittance

TΩ,ν
 or
TΩ,λ



1
Spectral radiance transmitted by a surface, divided by that received by that surface.

Hemispherical attenuation coefficient

μ
reciprocal metre
m−1

L−1
Radiant flux absorbed and scattered by a volume per unit length, divided by that received by that volume.

Spectral hemispherical attenuation coefficient

μν
 or
μλ
reciprocal metre
m−1

L−1
Spectral radiant flux absorbed and scattered by a volume per unit length, divided by that received by that volume.

Directional attenuation coefficient

μΩ
reciprocal metre
m−1

L−1
Radiance absorbed and scattered by a volume per unit length, divided by that received by that volume.

Spectral directional attenuation coefficient

μΩ,ν
 or
μΩ,λ
reciprocal metre
m−1

L−1
Spectral radiance absorbed and scattered by a volume per unit length, divided by that received by that volume.
See also: SI · Radiometry · Photometry




  1. ^ Standards organizations recommend that radiometric quantities should be denoted with suffix "e" (for "energetic") to avoid confusion with photometric or photon quantities.


  2. ^ abcde Alternative symbols sometimes seen: W or E for radiant energy, P or F for radiant flux, I for irradiance, W for radiant exitance.


  3. ^ abcdefg Spectral quantities given per unit frequency are denoted with suffix "ν" (Greek)—not to be confused with suffix "v" (for "visual") indicating a photometric quantity.


  4. ^ abcdefg Spectral quantities given per unit wavelength are denoted with suffix "λ" (Greek).


  5. ^ ab Directional quantities are denoted with suffix "Ω" (Greek).




See also



  • Luminous flux

  • Heat flux

  • Power (physics)

  • Radiosity (heat transfer)



References





  1. ^ abc "Thermal insulation — Heat transfer by radiation — Physical quantities and definitions". ISO 9288:1989. ISO catalogue. 1989. Retrieved 2015-03-15..mw-parser-output cite.citation{font-style:inherit}.mw-parser-output q{quotes:"""""""'""'"}.mw-parser-output code.cs1-code{color:inherit;background:inherit;border:inherit;padding:inherit}.mw-parser-output .cs1-lock-free a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/6/65/Lock-green.svg/9px-Lock-green.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .cs1-lock-limited a,.mw-parser-output .cs1-lock-registration a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/d/d6/Lock-gray-alt-2.svg/9px-Lock-gray-alt-2.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .cs1-lock-subscription a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/a/aa/Lock-red-alt-2.svg/9px-Lock-red-alt-2.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .cs1-subscription,.mw-parser-output .cs1-registration{color:#555}.mw-parser-output .cs1-subscription span,.mw-parser-output .cs1-registration span{border-bottom:1px dotted;cursor:help}.mw-parser-output .cs1-hidden-error{display:none;font-size:100%}.mw-parser-output .cs1-visible-error{font-size:100%}.mw-parser-output .cs1-subscription,.mw-parser-output .cs1-registration,.mw-parser-output .cs1-format{font-size:95%}.mw-parser-output .cs1-kern-left,.mw-parser-output .cs1-kern-wl-left{padding-left:0.2em}.mw-parser-output .cs1-kern-right,.mw-parser-output .cs1-kern-wl-right{padding-right:0.2em}




Further reading



  • Boyd, Robert (1983). Radiometry and the Detection of Optical Radiation (Pure & Applied Optics Series). Wiley-Interscience. ISBN 978-0-471-86188-1.



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