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In , radiant intensity is the emitted, reflected, transmitted or received, per unit , and spectral intensity is the radiant intensity per unit or , depending on whether the spectrum is taken as a function of frequency or of wavelength. These are directional quantities. The SI unit of radiant intensity is the per (), while that of spectral intensity in frequency is the watt per steradian per () and that of spectral intensity in wavelength is the watt per steradian per metre ()—commonly the watt per steradian per nanometre (). Radiant intensity is distinct from and , which are often called intensity in branches of other than radiometry. In radio-frequency engineering, radiant intensity is sometimes called radiation intensity.


Mathematical definitions

Radiant intensity
Radiant intensity, denoted Ie,Ω ("e" for "energetic", to avoid confusion with photometric quantities, and "Ω" to indicate this is a directional quantity), is defined as
I_{\mathrm{e},\Omega} = \frac{\partial \Phi_\mathrm{e}}{\partial \Omega},
where
  • ∂ is the partial derivative symbol;
  • Φe is the emitted, reflected, transmitted or received;
  • Ω is the .

In general, Ie,Ω is a function of viewing angle θ and potentially . For the special case of a Lambertian surface, Ie,Ω follows the Lambert's cosine law Ie,Ω = I0 cos θ.

When calculating the radiant intensity emitted by a source, Ω refers to the solid angle into which the light is emitted. When calculating radiance received by a detector, Ω refers to the solid angle subtended by the source as viewed from that detector.


Spectral intensity
Spectral intensity in frequency, denoted Ie,Ω,ν, is defined as
I_{\mathrm{e},\Omega,\nu} = \frac{\partial I_{\mathrm{e},\Omega}}{\partial \nu},
where ν is the frequency.

Spectral intensity in wavelength, denoted Ie,Ω,λ, is defined as

I_{\mathrm{e},\Omega,\lambda} = \frac{\partial I_{\mathrm{e},\Omega}}{\partial \lambda},
where λ is the wavelength.


Radio-frequency engineering
Radiant intensity is used to characterize the emission of radiation by an antenna:
(2025). 9780072321036, McGraw-Hill.
I_{\mathrm{e},\Omega} = E_\mathrm{e}(r) \, r^2,
where
  • Ee is the of the antenna;
  • r is the distance from the antenna.

Unlike power density, radiant intensity does not depend on distance: because radiant intensity is defined as the power through a solid angle, the decreasing power density over distance due to the inverse-square law is offset by the increase in area with distance.


SI radiometry units

See also


External links

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