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For a good summary of the previous literature and list of references, the reader is referred to S. Q. Duntley, J. Opt. Soc. Am. 32, 61 (1942).
[CrossRef]
Duntley’s equation reduces to the above Eq. (3) for P = 0, Q = 1 (see reference 1). See also D. R. Duncan, Proc. Phys. Soc. 52, 380 (1940).
[CrossRef]
L. Amy, Rev. d’optique 16, 81 (1938).
J. L. Michaelson, J. Opt. Soc. Am. 28, 365 (1938).
[CrossRef]
P. Kubelka and F. Munk, Zeits. f. tech. Physik 12, 593 (1931).
See also J. W. Ryde, Proc. Roy. Soc. A131, 451 (1931). Ryde’s Eq. (59) reduces to the above Eq. (6) for (his) T=T′ = 0, R′ = R.
[CrossRef]
See also J. W. Ryde and B. S. Copper, Proc. Roy. Soc. A131, 464 (1931), especially page 467.
[CrossRef]
L. Amy, Rev. d’optique 16, 81 (1938).
See also J. W. Ryde and B. S. Copper, Proc. Roy. Soc. A131, 464 (1931), especially page 467.
[CrossRef]
Duntley’s equation reduces to the above Eq. (3) for P = 0, Q = 1 (see reference 1). See also D. R. Duncan, Proc. Phys. Soc. 52, 380 (1940).
[CrossRef]
For a good summary of the previous literature and list of references, the reader is referred to S. Q. Duntley, J. Opt. Soc. Am. 32, 61 (1942).
[CrossRef]
P. Kubelka and F. Munk, Zeits. f. tech. Physik 12, 593 (1931).
P. Kubelka and F. Munk, Zeits. f. tech. Physik 12, 593 (1931).
See also A. E. Parker, Symposium on Color, p. 53, published by the American Society for Testing Materials (1941).
See also J. W. Ryde, Proc. Roy. Soc. A131, 451 (1931). Ryde’s Eq. (59) reduces to the above Eq. (6) for (his) T=T′ = 0, R′ = R.
[CrossRef]
See also J. W. Ryde and B. S. Copper, Proc. Roy. Soc. A131, 464 (1931), especially page 467.
[CrossRef]
For a good summary of the previous literature and list of references, the reader is referred to S. Q. Duntley, J. Opt. Soc. Am. 32, 61 (1942).
[CrossRef]
J. L. Michaelson, J. Opt. Soc. Am. 28, 365 (1938).
[CrossRef]
Duntley’s equation reduces to the above Eq. (3) for P = 0, Q = 1 (see reference 1). See also D. R. Duncan, Proc. Phys. Soc. 52, 380 (1940).
[CrossRef]
See also J. W. Ryde, Proc. Roy. Soc. A131, 451 (1931). Ryde’s Eq. (59) reduces to the above Eq. (6) for (his) T=T′ = 0, R′ = R.
[CrossRef]
See also J. W. Ryde and B. S. Copper, Proc. Roy. Soc. A131, 464 (1931), especially page 467.
[CrossRef]
L. Amy, Rev. d’optique 16, 81 (1938).
P. Kubelka and F. Munk, Zeits. f. tech. Physik 12, 593 (1931).
D. R. Duncan, reference 4, bases his calculations on θ ≡ e/μ. The use of Eq. (7) has been found by the author to be more convenient.
U. S. Department of Commerce, National Bureau of Standards, Letter Circular, LC-547.
See also A. E. Parker, Symposium on Color, p. 53, published by the American Society for Testing Materials (1941).
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Graph relating the measured reflection
Calculation of dye constants. Curve
Calculation of constants of red pigment. Curve
Calculation of a pigment mixture, as carried out in Table I.
Use of the relative constants. Curve
Calculation of a color match. Curve
Curves showing the accumulative effect of the various pigments added to white.
The effect.of opacity. Curve
Curves of the reflection and transmission of the white pigment, used for making the opacity correction. Curves
Table I Calculation of the color of a Pigment mixture. The calculations of the reflection value of a sample containing 0.5 percent white pigment, 0.015 percent red pigment shown in Fig. 4, and 0.025 percent yellow pigment are carried out in this table. The calculations are made by means of Eq. (8), and the results are compared with the actual curve obtained for the sample in Fig. 5.
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