Abstract

We have calculated corneal transparency using a theory given by Twersky and a model of Hart and Farrell. The results do not correspond with experimental observations.

© 1976 Optical Society of America

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References

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  1. V. Twersky, J. Opt. Soc. Am. 65, 524 (1975).
  2. R. W. Hart and R. A. Farrell, Bull. Math. Biophys. 33, 165 (1971).
  3. B. O. Hedbys and C. H. Dohlman, Exp. Eye Res. 2, 122 (1963).
  4. We do not enter into a discussion here of the problems of passing from two to three dimensions and the questions posed by introducing a scaling length which is assumed to be constant, independent of the parameters of interest. The physical significance of such a scaling length is unclear from Twersky’s work.

Dohlman, C. H.

B. O. Hedbys and C. H. Dohlman, Exp. Eye Res. 2, 122 (1963).

Farrell, R. A.

R. W. Hart and R. A. Farrell, Bull. Math. Biophys. 33, 165 (1971).

Hart, R. W.

R. W. Hart and R. A. Farrell, Bull. Math. Biophys. 33, 165 (1971).

Hedbys, B. O.

B. O. Hedbys and C. H. Dohlman, Exp. Eye Res. 2, 122 (1963).

Twersky, V.

V. Twersky, J. Opt. Soc. Am. 65, 524 (1975).

Other

V. Twersky, J. Opt. Soc. Am. 65, 524 (1975).

R. W. Hart and R. A. Farrell, Bull. Math. Biophys. 33, 165 (1971).

B. O. Hedbys and C. H. Dohlman, Exp. Eye Res. 2, 122 (1963).

We do not enter into a discussion here of the problems of passing from two to three dimensions and the questions posed by introducing a scaling length which is assumed to be constant, independent of the parameters of interest. The physical significance of such a scaling length is unclear from Twersky’s work.

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