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  1. 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).
  2. P. Kubelka and F. Munk, Zeits. f. tech. Physik 12, 593 (1931).
  3. L. Amy, Rev. d'optique 16, 81 (1938).
  4. 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).
  5. J. L. Michaelson, J. Opt. Soc. Am. 28, 365 (1938).
  6. See also A. E. Parker, Symposium on Color, p. 53, published by the American Society for Testing Materials (1941).
  7. 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.
  8. See also J. W. Ryde and B. S. Copper, Proc. Roy. Soc. A131, 464 (1931), especially page 467.
  9. 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.
  10. U. S. Department of Commerce, National Bureau of Standards, Letter Circular, LC-547.

Amy, L.

L. Amy, Rev. d'optique 16, 81 (1938).

Copper, B. S.

See also J. W. Ryde and B. S. Copper, Proc. Roy. Soc. A131, 464 (1931), especially page 467.

Duncan, D. R.

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.

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).

Duntley, S. Q.

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).

Kubelka, P.

P. Kubelka and F. Munk, Zeits. f. tech. Physik 12, 593 (1931).

Michaelson, J. L.

J. L. Michaelson, J. Opt. Soc. Am. 28, 365 (1938).

Munk, F.

P. Kubelka and F. Munk, Zeits. f. tech. Physik 12, 593 (1931).

Parker, A. E.

See also A. E. Parker, Symposium on Color, p. 53, published by the American Society for Testing Materials (1941).

Ryde, J. W.

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.

See also J. W. Ryde and B. S. Copper, Proc. Roy. Soc. A131, 464 (1931), especially page 467.

Other

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).

P. Kubelka and F. Munk, Zeits. f. tech. Physik 12, 593 (1931).

L. Amy, Rev. d'optique 16, 81 (1938).

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).

J. L. Michaelson, J. Opt. Soc. Am. 28, 365 (1938).

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.

See also J. W. Ryde and B. S. Copper, Proc. Roy. Soc. A131, 464 (1931), especially page 467.

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.

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