Movatterモバイル変換


[0]ホーム

URL:


Jump to content
WikipediaThe Free Encyclopedia
Search

Reflectance

From Wikipedia, the free encyclopedia
Capacity of an object to reflect light
Spectral reflectance curves foraluminium (Al),silver (Ag), andgold (Au) metalmirrors at normal incidence

Thereflectance of the surface of amaterial is its effectiveness inreflectingradiant energy. It is the fraction of incident electromagnetic power that is reflected at the boundary. Reflectance is a component of the response of theelectronic structure of the material to the electromagnetic field of light, and is in general a function of the frequency, orwavelength, of the light, its polarization, and theangle of incidence. The dependence of reflectance on the wavelength is called areflectance spectrum orspectral reflectance curve.

Mathematical definitions

[edit]

Hemispherical reflectance

[edit]

Thehemispherical reflectance of a surface, denotedR, is defined as[1]R=ΦerΦei,{\displaystyle R={\frac {\Phi _{\mathrm {e} }^{\mathrm {r} }}{\Phi _{\mathrm {e} }^{\mathrm {i} }}},}whereΦer is theradiant fluxreflected by that surface andΦei is the radiant fluxreceived by that surface.

Spectral hemispherical reflectance

[edit]

Thespectral hemispherical reflectance in frequency andspectral hemispherical reflectance in wavelength of a surface, denotedRν andRλ respectively, are defined as[1]Rν=Φe,νrΦe,νi,{\displaystyle R_{\nu }={\frac {\Phi _{\mathrm {e} ,\nu }^{\mathrm {r} }}{\Phi _{\mathrm {e} ,\nu }^{\mathrm {i} }}},}Rλ=Φe,λrΦe,λi,{\displaystyle R_{\lambda }={\frac {\Phi _{\mathrm {e} ,\lambda }^{\mathrm {r} }}{\Phi _{\mathrm {e} ,\lambda }^{\mathrm {i} }}},}where

Directional reflectance

[edit]

Thedirectional reflectance of a surface, denotedRΩ, is defined as[1]RΩ=Le,ΩrLe,Ωi,{\displaystyle R_{\Omega }={\frac {L_{\mathrm {e} ,\Omega }^{\mathrm {r} }}{L_{\mathrm {e} ,\Omega }^{\mathrm {i} }}},}where

  • Le,Ωr is theradiancereflected by that surface;
  • Le,Ωi is the radiance received by that surface.

This depends on both the reflected direction and the incoming direction. In other words, it has a value for every combination of incoming and outgoing directions. It is related to thebidirectional reflectance distribution function and its upper limit is 1. Another measure of reflectance, depending only on the outgoing direction, isI/F, whereI is the radiance reflected in a given direction andF is the incoming radiance averaged over all directions, in other words, the total flux of radiation hitting the surface per unit area, divided by π.[2] This can be greater than 1 for a glossy surface illuminated by a source such as the sun, with the reflectance measured in the direction of maximum radiance (see alsoSeeliger effect).

Spectral directional reflectance

[edit]

Thespectral directional reflectance in frequency andspectral directional reflectance in wavelength of a surface, denotedRΩ,ν andRΩ,λ respectively, are defined as[1]RΩ,ν=Le,Ω,νrLe,Ω,νi,{\displaystyle R_{\Omega ,\nu }={\frac {L_{\mathrm {e} ,\Omega ,\nu }^{\mathrm {r} }}{L_{\mathrm {e} ,\Omega ,\nu }^{\mathrm {i} }}},}RΩ,λ=Le,Ω,λrLe,Ω,λi,{\displaystyle R_{\Omega ,\lambda }={\frac {L_{\mathrm {e} ,\Omega ,\lambda }^{\mathrm {r} }}{L_{\mathrm {e} ,\Omega ,\lambda }^{\mathrm {i} }}},}where

Again, one can also define a value ofI/F (see above) for a given wavelength.[3]

Reflectivity

[edit]
Fresnel reflection coefficients for a boundary surface between air and a variable material in dependence of the complex refractive index and the angle of incidence
"Reflectivity" redirects here. For the EM formulation, seeFresnel power reflection.

For homogeneous and semi-infinite (seehalfspace) materials, reflectivity is the same as reflectance. Reflectivity is the square of the magnitude of theFresnel reflection coefficient,[4]which is the ratio of the reflected to incidentelectric field;[5] as such the reflection coefficient can be expressed as acomplex number as determined by theFresnel equations for a single layer, whereas the reflectance is always a positivereal number.

For layered and finite media, according to theCIE,[citation needed] reflectivity is distinguished fromreflectance by the fact that reflectivity is a value that applies tothick reflecting objects.[6] When reflection occurs from thin layers of material, internal reflection effects can cause the reflectance to vary with surface thickness. Reflectivity is the limit value of reflectance as the sample becomes thick; it is the intrinsic reflectance of the surface, hence irrespective of other parameters such as the reflectance of the rear surface. Another way to interpret this is that the reflectance is the fraction of electromagnetic power reflected from a specific sample, while reflectivity is a property of the material itself, which would be measured on a perfect machine if the material filled half of all space.[7]

Surface type

[edit]

Given that reflectance is a directional property, most surfaces can be divided into those that givespecular reflection and those that givediffuse reflection.

For specular surfaces, such as glass or polished metal, reflectance is nearly zero at all angles except at the appropriate reflected angle; that is the same angle with respect to the surface normal in theplane of incidence, but on the opposing side. When the radiation is incident normal to the surface, it is reflected back into the same direction.

For diffuse surfaces, such as matte white paint, reflectance is uniform; radiation is reflected in all angles equally or near-equally. Such surfaces are said to beLambertian.

Most practical objects exhibit a combination of diffuse and specular reflective properties.

Liquid reflectance

[edit]
Reflectance of smooth water at 20 °C (refractive index 1.333)

Reflection of light occurs at a boundary at which theindex of refraction changes. Specular reflection is calculated by theFresnel equations.[8] Fresnel reflection is directional and therefore does not contribute significantly toalbedo which primarily diffuses reflection.

A liquid surface may be wavy. Reflectance may be adjusted to account forwaviness.

Grating efficiency

[edit]

The generalization of reflectance to adiffraction grating, which disperses light bywavelength, is calleddiffraction efficiency.

Other radiometric coefficients

[edit]
Radiometry coefficients
QuantitySI unitsNotes
NameSym.
Hemispherical emissivityεRadiant exitance of asurface, divided by that of ablack body at the same temperature as that surface.
Spectral hemispherical emissivityεν
ελ
Spectral exitance of asurface, divided by that of ablack body at the same temperature as that surface.
Directional emissivityεΩRadianceemitted by asurface, divided by that emitted by ablack body at the same temperature as that surface.
Spectral directional emissivityεΩ,ν
εΩ,λ
Spectral radianceemitted by asurface, divided by that of ablack body at the same temperature as that surface.
Hemispherical absorptanceARadiant fluxabsorbed by asurface, divided by that received by that surface. This should not be confused with "absorbance".
Spectral hemispherical absorptanceAν
Aλ
Spectral fluxabsorbed by asurface, divided by that received by that surface. This should not be confused with "spectral absorbance".
Directional absorptanceAΩRadianceabsorbed by asurface, divided by the radiance incident onto that surface. This should not be confused with "absorbance".
Spectral directional absorptanceAΩ,ν
AΩ,λ
Spectral radianceabsorbed by asurface, divided by the spectral radiance incident onto that surface. This should not be confused with "spectral absorbance".
Hemispherical reflectanceRRadiant fluxreflected by asurface, divided by that received by that surface.
Spectral hemispherical reflectanceRν
Rλ
Spectral fluxreflected by asurface, divided by that received by that surface.
Directional reflectanceRΩRadiancereflected by asurface, divided by that received by that surface.
Spectral directional reflectanceRΩ,ν
RΩ,λ
Spectral radiancereflected by asurface, divided by that received by that surface.
Hemispherical transmittanceTRadiant fluxtransmitted by asurface, divided by that received by that surface.
Spectral hemispherical transmittanceTν
Tλ
Spectral fluxtransmitted by asurface, divided by that received by that surface.
Directional transmittanceTΩRadiancetransmitted by asurface, divided by that received by that surface.
Spectral directional transmittanceTΩ,ν
TΩ,λ
Spectral radiancetransmitted by asurface, divided by that received by that surface.
Hemispherical attenuation coefficientμm−1Radiant fluxabsorbed andscattered by avolume per unit length, divided by that received by that volume.
Spectral hemispherical attenuation coefficientμν
μλ
m−1Spectral radiant fluxabsorbed andscattered by avolume per unit length, divided by that received by that volume.
Directional attenuation coefficientμΩm−1Radianceabsorbed andscattered by avolume per unit length, divided by that received by that volume.
Spectral directional attenuation coefficientμΩ,ν
μΩ,λ
m−1Spectral radianceabsorbed andscattered by avolume per unit length, divided by that received by that volume.

See also

[edit]

References

[edit]
  1. ^abcd"Thermal insulation — Heat transfer by radiation — Physical quantities and definitions".ISO 9288:1989.ISO catalogue. 1989. Retrieved2015-03-15.
  2. ^Cuzzi, Jeffrey; Chambers, Lindsey; Hendrix, Amanda (Oct 21, 2016)."Rough Surfaces: is the dark stuff just shadow?".Icarus.289:281–294.doi:10.1016/j.icarus.2016.10.018.PMC 6839776.PMID 31708591.
  3. ^See for exampleP.G.J Irwin; et al. (Jan 12, 2022)."Hazy Blue Worlds: A Holistic Aerosol Model for Uranus and Neptune, Including Dark Spots".Journal of Geophysical Research: Planets.127 (6) e2022JE007189.arXiv:2201.04516.Bibcode:2022JGRE..12707189I.doi:10.1029/2022JE007189.hdl:1983/65ee78f0-1d28-4017-bbd9-1b49b24700d7.PMC 9286428.PMID 35865671.S2CID 245877540.
  4. ^E. Hecht (2001). Optics (4th ed.). Pearson Education.ISBN 0-8053-8566-5.
  5. ^IUPAC,Compendium of Chemical Terminology, 5th ed. (the "Gold Book") (2025). Online version: (2006–) "Reflectance".doi:10.1351/goldbook.R05235
  6. ^"CIE International Lighting Vocabulary". Archived fromthe original on 2016-06-16. Retrieved2010-12-04.
  7. ^Palmer and Grant,The Art of Radiometry
  8. ^Ottaviani, M. and Stamnes, K. and Koskulics, J. and Eide, H. and Long, S.R. and Su, W. and Wiscombe, W., 2008: 'Light Reflection from Water Waves: Suitable Setup for a Polarimetric Investigation under Controlled Laboratory Conditions.Journal of Atmospheric and Oceanic Technology,25 (5), 715--728.

External links

[edit]
Look upreflectance in Wiktionary, the free dictionary.
Retrieved from "https://en.wikipedia.org/w/index.php?title=Reflectance&oldid=1319464930"
Categories:
Hidden categories:

[8]ページ先頭

©2009-2025 Movatter.jp