Grassmann's laws describe empirical results about how the perception of mixtures of colored lights (i.e., lights that co-stimulate the same area on the retina) composed of different spectral power distributions can be algebraically related to one another in a color matching context. Discovered by Hermann Grassmann[1] these "laws" are actually principles used to predict color match responses to a good approximation under photopic and mesopic vision. A number of studies have examined how and why they provide poor predictions under specific conditions.[2][3]
The original laws
Grassmann's original laws were set out in his 1853 paper "Zur Theorie der Farbenmischung"[1]. The translations here are from 1854[4].
- Every impression of colour of this kind may be analysed into three mathematically determinable elements,--the tint, the intensity of the colour, and the intensity of the intermixed white.
- If one of two mingling lights be continuously altered (whilst the other remains unchanged), the impression of the mixed light also is continuously changed.
- Two colours, each of which has a constant tint and a constant intensity of the intermixed white, also give constant mixed colours, no matter of what homogeneous colours they may be composed.
- The total intensity of the mixture is the sum of the intensities of the lights mixed.
Modern interpretation

The four laws are described in modern texts[6] with varying degrees of algebraic notation and are summarized as follows (the precise numbering and corollary definitions can vary across sources[7]):
- First law
- Two colored lights appear different if they differ in either dominant wavelength, luminance or purity. Corollary: For every colored light there exists a light with a complementary color such that a mixture of both lights either desaturates the more intense component or gives uncolored (grey/white) light.
- Second law
- The appearance of a mixture of light made from two components changes if either component changes. Corollary: A mixture of two colored lights that are non-complementary result in a mixture that varies in hue with relative intensities of each light and in saturation according to the distance between the hues of each light.
- Third law
- There are lights with different spectral power distributions but appear identical. First corollary: such identical appearing lights must have identical effects when added to a mixture of light. Second corollary: such identical appearing lights must have identical effects when subtracted (i.e., filtered) from a mixture of light.
- Fourth law
- The intensity of a mixture of lights is the sum of the intensities of the components. This is also known as Abney's law.
These laws entail an algebraic representation of colored light.[8] Assuming beam 1 and 2 each have a color, and the observer chooses
(
R
1
,
G
1
,
B
1
)
{\displaystyle (R_{1},G_{1},B_{1})}
as the strengths of the primaries that match beam 1 and
(
R
2
,
G
2
,
B
2
)
{\displaystyle (R_{2},G_{2},B_{2})}
as the strengths of the primaries that match beam 2, then if the two beams were combined, the matching values will be the sums of the components. Precisely, they will be
(
R
,
G
,
B
)
{\displaystyle (R,G,B)}
, where
R
=
R
1
+
R
2
,
G
=
G
1
+
G
2
,
B
=
B
1
+
B
2
.
{\displaystyle {\begin{aligned}R&=R_{1}+R_{2},\\G&=G_{1}+G_{2},\\B&=B_{1}+B_{2}.\end{aligned}}}
Grassmann's laws can be expressed in general form by stating that for a given color with a spectral power distribution
I
(
λ
)
{\displaystyle I(\lambda )}
the RGB coordinates are given by
R
=
∫
0
∞
I
(
λ
)
r
¯
(
λ
)
d
λ
,
G
=
∫
0
∞
I
(
λ
)
g
¯
(
λ
)
d
λ
,
B
=
∫
0
∞
I
(
λ
)
b
¯
(
λ
)
d
λ
.
{\displaystyle {\begin{aligned}R&=\int _{0}^{\infty }I(\lambda )\,{\bar {r}}(\lambda )\,d\lambda ,\\G&=\int _{0}^{\infty }I(\lambda )\,{\bar {g}}(\lambda )\,d\lambda ,\\B&=\int _{0}^{\infty }I(\lambda )\,{\bar {b}}(\lambda )\,d\lambda .\end{aligned}}}
Observe that these are linear in
I
{\displaystyle I}
; the functions
r
¯
(
λ
)
,
g
¯
(
λ
)
,
b
¯
(
λ
)
{\displaystyle {\bar {r}}(\lambda ),{\bar {g}}(\lambda ),{\bar {b}}(\lambda )}
are the color-matching functions with respect to the chosen primaries.
See also
References
- Grassmann, H. (1853). "Zur Theorie der Farbenmischung". Annalen der Physik und Chemie. 165 (5): 69–84. Bibcode:1853AnP...165...69G. doi:10.1002/andp.18531650505.
- Pokorny, Joel; Smith, Vivianne C.; Xu, Jun (1 February 2012). "Quantal and non-quantal color matches: failure of Grassmann's laws at short wavelengths". Journal of the Optical Society of America A. 29 (2): A324-36. Bibcode:2012JOSAA..29A.324P. doi:10.1364/JOSAA.29.00A324. PMID 22330396.
- Brill, Michael H.; Robertson, Alan R. (2007). "Open Problems on the Validity of Grassmann's Laws". Colorimetry: Understanding the CIE System. John Wiley & Sons, Inc. pp. 245–259. doi:10.1002/9780470175637.ch10. ISBN 978-0-470-17563-7.
- Grassmann (1854-04-01). "XXXVII. On the theory of compound colours". The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science. 7 (45): 254–264. doi:10.1080/14786445408647464. ISSN 1941-5982.
- Hermann Grassmann; Gert Schubring (1996). Hermann Günther Grassmann (1809-1877): visionary mathematician, scientist and neohumanist scholar: papers from a sesquicentennial conference. Springer. p. 78. ISBN 978-0-7923-4261-8.
- Stevenson, Scott. "University of Houston Vision OPTO 5320 Vision Science 1 Lecture Notes" (PDF). University of Houston Vision OPTO 5320 Vision Science 1 Course Materials. Archived from the original (PDF) on 5 January 2018. Retrieved 4 January 2018.
- Judd, Deane Brewster; Technology, Center for Building (1979). Contributions to Color Science. NBS. p. 457. Retrieved 6 January 2018.
- Reinhard, Erik; Khan, Erum Arif; Akyuz, Ahmet Oguz; Johnson, Garrett (2008). Color Imaging: Fundamentals and Applications. CRC Press. p. 364. ISBN 978-1-4398-6520-0.