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CIELUV

From Wikipedia, the free encyclopedia
Color space

Incolorimetry, theCIE 1976L*,u*,v*color space, commonly known by its abbreviationCIELUV, is acolor space adopted by theInternational Commission on Illumination (CIE) in 1976, as a simple-to-compute transformation of the 1931CIE XYZ color space, but which attemptedperceptual uniformity. It is extensively used for applications such as computer graphics which deal with colored lights. Although additive mixtures of different colored lights will fall on a line in CIELUV's uniformchromaticity diagram (called theCIE 1976 UCS), such additive mixtures will not, contrary to popular belief, fall along a line in the CIELUV color space unless the mixtures are constant inlightness.

Historical background

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ThesRGB gamut (left) andoptimal color solid (theoretical gamut of surfaces) under D65 illumination (right) plotted within the CIELUV color space.u andv are the horizontal axes;L is the vertical axis.

CIELUV is anAdams chromatic valence color space and is an update of theCIE 1964 (U*,V*,W*) color space (CIEUVW). The differences include a slightly modifiedlightness scale and a modified uniform chromaticity scale, in which one of the coordinates,v′, is 1.5 times as large asv in its1960 predecessor. CIELUV andCIELAB were adopted simultaneously by the CIE when no clear consensus could be formed behind only one or the other of these two color spaces.

CIELUV uses Judd-type (translational)white point adaptation (in contrast with CIELAB, which uses avon Kries transform).[1] This can produce useful results when working with a single illuminant, but can predictimaginary colors (i.e., outside thespectral locus) when attempting to use it as achromatic adaptation transform.[2] The translational adaptation transform used in CIELUV has also been shown to perform poorly in predicting corresponding colors.[3]

XYZ → CIELUV and CIELUV → XYZ conversions

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By definition,0 ≤L* ≤ 100.

The forward transformation

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CIELUV is based on CIEUVW and is another attempt to define an encoding with uniformity in the perceptibility ofcolor differences.[4] The non-linear relations forL*,u*, andv* are given below:[4]

L={(293)3Y/Yn,Y/Yn(629)3,116Y/Yn316,Y/Yn>(629)3,u=13L(uun),v=13L(vvn).{\displaystyle {\begin{aligned}L^{*}&={\begin{cases}{\bigl (}{\tfrac {29}{3}}{\bigr )}^{3}Y/Y_{n},&Y/Y_{n}\leq {\bigl (}{\tfrac {6}{29}}{\bigr )}^{3},\\[3mu]116{\sqrt[{3}]{Y/Y_{n}}}-16,&Y/Y_{n}>{\bigl (}{\tfrac {6}{29}}{\bigr )}^{3},\end{cases}}\\[5mu]u^{*}&=13L^{*}\cdot (u^{\prime }-u_{n}^{\prime }),\\[3mu]v^{*}&=13L^{*}\cdot (v^{\prime }-v_{n}^{\prime }).\end{aligned}}}

The quantitiesun andvn are the(u′,v′) chromaticity coordinates of a "specified white object" – which may be termed thewhite point – andYn is its luminance. In reflection mode, this is often (but not always) taken as the(u′,v′) of theperfect reflecting diffuser under that illuminant. (For example, for the2° observer andstandard illuminant C,un = 0.2009,vn = 0.4610.) Equations foru′ andv′ are given below:[5][6]

u=4XX+15Y+3Z=4x2x+12y+3,v=9YX+15Y+3Z=9y2x+12y+3.{\displaystyle {\begin{alignedat}{3}u^{\prime }&={\frac {4X}{X+15Y+3Z}}&&={\frac {4x}{-2x+12y+3}},\\[5mu]v^{\prime }&={\frac {9Y}{X+15Y+3Z}}&&={\frac {9y}{-2x+12y+3}}.\end{alignedat}}}

The reverse transformation

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(u′,v′) chromaticity diagram, also known as the CIE 1976 UCS (uniform chromaticity scale) diagram.

The transformation from(u′,v′) to(x,y) is:[6]

x=9u6u16v+12y=4v6u16v+12{\displaystyle {\begin{aligned}x&={\frac {9u^{\prime }}{6u^{\prime }-16v^{\prime }+12}}\\[5mu]y&={\frac {4v^{\prime }}{6u^{\prime }-16v^{\prime }+12}}\end{aligned}}}

The transformation from CIELUV to XYZ is performed as follows:[6]

u=113(u/L)+un,v=113(v/L)+vn,Y={(329)3L Yn,L8,(1116(L+16))3Yn,L>8,X=9u4vY,Z=123u20v4vY.{\displaystyle {\begin{aligned}u^{\prime }&={\tfrac {1}{13}}(u^{*}/L^{*})+u_{n}^{\prime },\\[3mu]v^{\prime }&={\tfrac {1}{13}}(v^{*}/L^{*})+v_{n}^{\prime },\\[5mu]Y&={\begin{cases}{\bigl (}{\frac {3}{29}}{\bigr )}^{3}L^{*}~\!Y_{n},&L^{*}\leq 8,\\[3mu]{\bigl (}{\tfrac {1}{116}}(L^{*}+16){\bigr )}^{3}\,Y_{n},&L^{*}>8,\end{cases}}\\[5mu]X&={\frac {9u^{\prime }}{4v^{\prime }}}Y,\\[5mu]Z&={\frac {12-3u^{\prime }-20v^{\prime }}{4v^{\prime }}}Y.\end{aligned}}}

Cylindrical representation (CIELCh)

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ThesRGB gamut (left) andoptimal color solid (theoretical gamut of surfaces) under D65 illumination (right) plotted within the CIELCHuv color space.L is the vertical axis;C is the cylinder radius;h is the angle around the circumference.

CIELChuv, orHCL color space (hue–chroma–luminance) is increasingly seen in theinformation visualization community as a way to help with presenting data without the bias implicit in using varyingsaturation.[7][8][9]

Thecylindrical version of CIELUV is known as CIELChuv, or CIELChuv, CIELCh(uv) or CIEHLCuv, whereC*uv is thechroma andhuv is thehue:[6]

Cuv=hypot(u,v)=(u)2+(v)2,{\displaystyle C_{uv}^{*}=\operatorname {hypot} (u^{*},v^{*})={\sqrt {(u^{*})^{2}+(v^{*})^{2}}},}
huv=atan2(v,u),{\displaystyle h_{uv}=\operatorname {atan2} (v^{*},u^{*}),}

whereatan2 function, a "two-argument arctangent", computes thepolar angle from a Cartesian coordinate pair.

Furthermore, the saturation correlate can be defined as

suv=CL=13(uun)2+(vvn)2.{\displaystyle s_{uv}={\frac {C^{*}}{L^{*}}}=13{\sqrt {(u'-u'_{n})^{2}+(v'-v'_{n})^{2}}}.}

Similar correlates of chroma and hue, but not saturation, exist for CIELAB. SeeColorfulness for more discussion on saturation.

Color and hue difference

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Thecolor difference can be calculated using theEuclidean distance of the(L*,u*,v*) coordinates.[6] It follows that a chromaticity distance of(Δu)2+(Δv)2=1/13{\displaystyle {\sqrt {(\Delta u')^{2}+(\Delta v')^{2}}}=1/13} corresponds to the same ΔE*uv as a lightness difference ofΔL* = 1, in direct analogy to CIEUVW.

The Euclidean metric can also be used in CIELCh, with that component of ΔE*uv attributable to difference in hue as[4]ΔH* =C*1C*2 2 sin (Δh/2), whereΔh =h2h1.

See also

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References

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  1. ^Judd, Deane B. (January 1940). "Hue saturation and lightness of surface colors with chromatic illumination".JOSA.30 (1):2–32.doi:10.1364/JOSA.30.000002.
  2. ^Mark D. Fairchild,Color Appearance Models. Reading, MA: Addison-Wesley, 1998.
  3. ^D. H. Alman, R. S. Berns, G. D. Snyder, and W. A. Larson, "Performance testing of color difference metrics using a color-tolerance dataset".Color Research and Application,21:174–188 (1989).
  4. ^abcSchanda, János (2007).Colorimetry: Understanding the CIE System. Wiley Interscience. pp. 61–64.ISBN 978-0-470-04904-4.As 24/116 is not a simple ratio, in some publications the 6/29 ratio is used, in others the approximate value of 0.008856 (used in earlier editions of CIE 15). Similarly some authors prefer to use instead of 841/108 the expression (1/3)×(29/6)2 or the approximate value of 7.787, or instead of 16/116 the ratio 4/29.
  5. ^Colorimetry, second edition: CIE publication 15.2. Vienna: Bureau Central CIE, 1986.
  6. ^abcdePoynton, Charles (2003).Digital Video and HDTV. Morgan-Kaufmann. p. 226.ISBN 1-55860-792-7.
  7. ^Ihaka, Ross (2003)."Colour for Presentation Graphics". In Hornik, Kurt; Leisch, Friedrich; Zeileis, Achim (eds.).Proceedings of the 3rd International Workshop on Distributed Statistical Computing, Vienna, Austria.ISSN 1609-395X.
  8. ^Zeileis, Achim; Hornik, Kurt; Murrell, Paul (2009)."Escaping RGBland: Selecting Colors for Statistical Graphics"(PDF).Computational Statistics & Data Analysis.53 (9):3259–3270.doi:10.1016/j.csda.2008.11.033.
  9. ^Stauffer, Reto; Mayr, Georg J.; Dabernig, Markus; Zeileis, Achim (2015). "Somewhere over the Rainbow: How to Make Effective Use of Colors in Meteorological Visualizations".Bulletin of the American Meteorological Society.96 (2):203–216.Bibcode:2015BAMS...96..203S.doi:10.1175/BAMS-D-13-00155.1.hdl:10419/101098.

External links

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CAM
CIE
RGB
Y′UV
Other
Color systems
and standards
For the vision capacities of organisms or machines, see Color vision.
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