Color solid

A color solid is the three-dimensional representation of a color model, an analog of the two-dimensional color wheel. The added spatial dimension allows a color solid to depict an added dimension of color variation. Whereas a two-dimensional color wheel typically depicts the variables of hue (red, green, blue, etc.) and lightness (gradations of light and dark, tints or shades), a color solid adds the variable of colorfulness (either chroma or saturation), allowing the solid to depict all conceivable colors in an organized three-dimensional structure.

Painters long mixed colors by combining relatively bright pigments with black and white. Mixtures with white are called tints, mixtures with black are called shades, and mixtures with both are called tones. See Tints and shades.[1]
Side-by-side comparison of several different color solids for the HSL, HSV and RGB color models. Potential shapes include cubes, cylinders, cones and spheres.


Exterior view of color sphere of Albert Henry Munsell, 1900.
Interior cross section of Munsell's color sphere and color tree, 1915.
Philipp Otto Runge’s Farbenkugel (color sphere), 1810, showing the surface of the sphere (top two images), and horizontal and vertical cross sections (bottom two images).
Color sphere of Johannes Itten, 1919-20. A much clearer representation of his model appears in The Art of Color, 1961.
Color sphere modeled in salt dough by Jesse Hensel, 2011.
Section of Hensel's sphere revealing a color spectrum.

Different color theorists have each designed unique color solids. Many are in the shape of a sphere, whereas others are warped three-dimensional ellipsoid figuresthese variations being designed to express some aspect of the relationship of the colors more clearly. The color spheres conceived by Phillip Otto Runge and Johannes Itten are typical examples and prototypes for many other color solid schematics.[2]

Pure, saturated hues of equal brightness are located around the equator at the periphery of the color sphere. As in the color wheel, contrasting (or complementary) hues are located opposite each other. Moving toward the center of the color sphere on the equatorial plane, colors become less and less saturated, until all colors meet at the central axis as a neutral gray. Moving vertically in the color sphere, colors become lighter (toward the top) and darker (toward the bottom). At the upper pole, all hues meet in white; at the bottom pole, all hues meet in black.

The vertical axis of the color sphere, then, is gray all along its length, varying from black at the bottom to white at the top. All pure (saturated) hues are located on the surface of the sphere, varying from light to dark down the color sphere. All impure (unsaturated hues, created by mixing contrasting colors) comprise the sphere's interior, likewise varying in brightness from top to bottom.


Artists and art critics find the color solid to be a useful means of organizing the three variables of colorhue, lightness, and saturation (or chroma), as modelled in the HCL and HSL color modelsin a single schematic, using it as an aid in the composition and analysis of visual art.


Despite the general description given earlier, historically, different authors have structured their shapes differently, internally. For instance, among the spherical color solids, "colorfulness" (or "chroma" or "saturation", depending) may increase or decrease horizontally from a central axis (Munsell and Itten, above), or may increase outwardly in every direction from a central point (Runge, also above). Further, definitions for "chroma", "colorfulness", "saturation", etc. vary between color models. For instance, in the Munsell and HSV systems, dark colors can have a full range of different "saturations", whereas light colors always have a low "saturation". In the HSL system, both a very light color and a very dark color may be equally "saturated". (Other systems differ in other ways.) Lastly, if colors are meant to be kept perceptually uniform, then a perfectly regular shape such as a sphere, cylinder or cone is not possible. Rather, models aiming for perceptual uniformity tend to be highly irregular in shape. Compare, for instance, Albert Munsell's color sphere with his later color tree; or, compare any of the above systems with CIELAB or CIELUV.

See also


  1. Levkowitz and Herman (1993)
  2. Johannes Itten, "The Art of Color", 1961. Trans. Ernst Van Haagen. New York: Reinhold Publishing Corporation, 1966. ISBN 0-442-24038-4.
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