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Irradiance

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In radiometry, irradiance is the radiant flux received by a surface, per unit area, and spectral irradiance is the irradiance of a surface in a given frequency span or wavelength span, per unit frequency or wavelength, depending on whether the spectrum is taken as a function of frequency or of wavelength. The SI unit of irradiance is the watt per square metre (W/m), while that of spectral irradiance is the watt per square metre per hertz (W·m·Hz) or the watt per square metre per metre (W·m)—commonly the watt per square metre per nanometre (W·m·nm). The CGS unit erg per square centimeter per second (erg·cm·s) is often used in astronomy. Irradiance is often called "intensity" in branches of physics other than radiometry, but in radiometry this usage leads to confusion with radiant intensity.

Definitions

Irradiance

Irradiance of a surface, denoted Ee ("e" for "energetic", to avoid confusion with photometric quantities) and measured in W/m, is given by:

E e = Φ e A , {\displaystyle E_{\mathrm {e} }={\frac {\partial \Phi _{\mathrm {e} }}{\partial A}},}

where

  • ∂ is the partial derivative symbol;
  • ∂Φe is the radiant flux received by the surface, measured in W;
  • A is the area of the surface, measured in m.

Spectral irradiance

Spectral irradiance of a surface in a given frequency span, denoted Ee,ν and measured in W·m·Hz, is given by:

E e , ν = E e ν , {\displaystyle E_{\mathrm {e} ,\nu }={\frac {\partial E_{\mathrm {e} }}{\partial \nu }},}

where

  • Ee is the irradiance of the surface in that frequency span, measured in W/m;
  • ν is the frequency span, measured in Hz.

Spectral irradiance of a surface in a given wavelength span, denoted Ee,λ and measured in W/m (commonly in W·m·nm), is given by:

E e , λ = E e λ , {\displaystyle E_{\mathrm {e} ,\lambda }={\frac {\partial E_{\mathrm {e} }}{\partial \lambda }},}
  • Ee is the irradiance of the surface in that wavelength span, measured in W/m;
  • λ is the wavelength, measured in m (commonly in nm).

Alternative definition

Irradiance of a surface is also defined as the time-average of the component of the Poynting vector perpendicular to the surface:

E e = S n ^ , {\displaystyle E_{\mathrm {e} }=\langle \mathbf {S} \cdot \mathbf {\hat {n}} \rangle ,}

where

  • S is the Poynting vector;
  • n ^ {\displaystyle \mathbf {\hat {n}} } is the normal vector to the surface;

In a propagating sinusoidal linearly polarized electromagnetic plane wave, the Poynting vector always points in the direction of propagation while oscillating in magnitude. The irradiance of a surface perpendicular to the direction of propagation is then given by:

E e = n 2 μ 0 c E m 2 = n ϵ 0 c 2 E m 2 , {\displaystyle E_{\mathrm {e} }={\frac {n}{2\mu _{0}\mathrm {c} }}E_{\mathrm {m} }^{2}={\frac {n\epsilon _{0}\mathrm {c} }{2}}E_{\mathrm {m} }^{2},}

where

This formula assumes that the magnetic susceptibility is negligible, i.e. that μr ≈ 1 where μr is the magnetic permeability of the propagation medium. This assumption is typically valid in transparent media in the optical frequency range.

Solar energy

The global irradiance on a horizontal surface on Earth consists of the direct irradiance Ee,dir and diffuse irradiance Ee,diff. On a tilted plane, there is another irradiance component, Ee,refl, which is the component that is reflected from the ground. The average ground reflection is about 20% of the global irradiance. Hence, the irradiance Ee on a tilted plane consists of three components:

E e = E e , d i r + E e , d i f f + E e , r e f l . {\displaystyle E_{\mathrm {e} }=E_{\mathrm {e} ,\mathrm {dir} }+E_{\mathrm {e} ,\mathrm {diff} }+E_{\mathrm {e} ,\mathrm {refl} }.}

The integral of solar irradiance over a time period is called solar irradiation or solar exposure or insolation.

SI radiometry units
Quantity Unit Dimension Notes
Name Symbol Name Symbol
Radiant energy Qe joule J MLT Energy of electromagnetic radiation.
Radiant energy density we joule per cubic metre J/m MLT Radiant energy per unit volume.
Radiant flux Φe watt W = J/s MLT Radiant energy emitted, reflected, transmitted or received, per unit time. This is sometimes also called "radiant power", and called luminosity in Astronomy.
Spectral flux Φe,ν watt per hertz W/Hz MLT Radiant flux per unit frequency or wavelength. The latter is commonly measured in W⋅nm.
Φe,λ watt per metre W/m MLT
Radiant intensity Ie,Ω watt per steradian W/sr MLT Radiant flux emitted, reflected, transmitted or received, per unit solid angle. This is a directional quantity.
Spectral intensity Ie,Ω,ν watt per steradian per hertz W⋅sr⋅Hz MLT Radiant intensity per unit frequency or wavelength. The latter is commonly measured in W⋅sr⋅nm. This is a directional quantity.
Ie,Ω,λ watt per steradian per metre W⋅sr⋅m MLT
Radiance Le,Ω watt per steradian per square metre W⋅sr⋅m MT 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
Specific intensity
Le,Ω,ν watt per steradian per square metre per hertz W⋅sr⋅m⋅Hz MT Radiance of a surface per unit frequency or wavelength. The latter is commonly measured in W⋅sr⋅m⋅nm. This is a directional quantity. This is sometimes also confusingly called "spectral intensity".
Le,Ω,λ watt per steradian per square metre, per metre W⋅sr⋅m MLT
Irradiance
Flux density
Ee watt per square metre W/m MT Radiant flux received by a surface per unit area. This is sometimes also confusingly called "intensity".
Spectral irradiance
Spectral flux density
Ee,ν watt per square metre per hertz W⋅m⋅Hz MT 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 W⋅m⋅Hz) and solar flux unit (1 sfu = 10 W⋅m⋅Hz = 10 Jy).
Ee,λ watt per square metre, per metre W/m MLT
Radiosity Je watt per square metre W/m MT Radiant flux leaving (emitted, reflected and transmitted by) a surface per unit area. This is sometimes also confusingly called "intensity".
Spectral radiosity Je,ν watt per square metre per hertz W⋅m⋅Hz MT Radiosity of a surface per unit frequency or wavelength. The latter is commonly measured in W⋅m⋅nm. This is sometimes also confusingly called "spectral intensity".
Je,λ watt per square metre, per metre W/m MLT
Radiant exitance Me watt per square metre W/m MT 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 watt per square metre per hertz W⋅m⋅Hz MT Radiant exitance of a surface per unit frequency or wavelength. The latter is commonly measured in W⋅m⋅nm. "Spectral emittance" is an old term for this quantity. This is sometimes also confusingly called "spectral intensity".
Me,λ watt per square metre, per metre W/m MLT
Radiant exposure He joule per square metre J/m MT 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 joule per square metre per hertz J⋅m⋅Hz MT Radiant exposure of a surface per unit frequency or wavelength. The latter is commonly measured in J⋅m⋅nm. This is sometimes also called "spectral fluence".
He,λ joule per square metre, per metre J/m MLT
See also:
  1. Standards organizations recommend that radiometric quantities should be denoted with suffix "e" (for "energetic") to avoid confusion with photometric or photon quantities.
  2. ^ Alternative symbols sometimes seen: W or E for radiant energy, P or F for radiant flux, I for irradiance, W for radiant exitance.
  3. ^ Spectral quantities given per unit frequency are denoted with suffix "ν" (Greek letter nu, not to be confused with a letter "v", indicating a photometric quantity.)
  4. ^ Spectral quantities given per unit wavelength are denoted with suffix "λ".
  5. ^ Directional quantities are denoted with suffix "Ω".

See also

References

  1. Griffiths, David J. (1999). Introduction to electrodynamics (3. ed., reprint. with corr. ed.). Upper Saddle River, NJ : Prentice-Hall. ISBN 0-13-805326-X.
  2. ^ Quaschning, Volker (2003). "Technology fundamentals—The sun as an energy resource". Renewable Energy World. 6 (5): 90–93.
  3. Attention: This template ({{cite doi}}) is deprecated. To cite the publication identified by doi:10.1016/0038-092X(60)90062-1, please use {{cite journal}} (if it was published in a bona fide academic journal, otherwise {{cite report}} with |doi=10.1016/0038-092X(60)90062-1 instead.
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