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References

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  1. R. W. Preisendorfer, J. Mar. Res. 18, 1 (1959).
  2. J. T. O. Kirk, Aust. J. Mar. Freshwater Res. 32, 517 (1981).
    [CrossRef]
  3. J. H. Jerome, J. E. Bruton, R. P. Bukata, Appl. Opt. 21, 642 (1982).
    [CrossRef] [PubMed]
  4. L. V. Whitney, Trans. Wis. Acad. Sci. Arts Lett. 31, 175 (1938).

1982

1981

J. T. O. Kirk, Aust. J. Mar. Freshwater Res. 32, 517 (1981).
[CrossRef]

1959

R. W. Preisendorfer, J. Mar. Res. 18, 1 (1959).

1938

L. V. Whitney, Trans. Wis. Acad. Sci. Arts Lett. 31, 175 (1938).

Bruton, J. E.

Bukata, R. P.

Jerome, J. H.

Kirk, J. T. O.

J. T. O. Kirk, Aust. J. Mar. Freshwater Res. 32, 517 (1981).
[CrossRef]

Preisendorfer, R. W.

R. W. Preisendorfer, J. Mar. Res. 18, 1 (1959).

Whitney, L. V.

L. V. Whitney, Trans. Wis. Acad. Sci. Arts Lett. 31, 175 (1938).

Appl. Opt.

Aust. J. Mar. Freshwater Res.

J. T. O. Kirk, Aust. J. Mar. Freshwater Res. 32, 517 (1981).
[CrossRef]

J. Mar. Res.

R. W. Preisendorfer, J. Mar. Res. 18, 1 (1959).

Trans. Wis. Acad. Sci. Arts Lett.

L. V. Whitney, Trans. Wis. Acad. Sci. Arts Lett. 31, 175 (1938).

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Tables (4)

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Table I Relative Depths of the 1% Subsurface Irradiance Level as a Function of Solar Zenith Angle and Diffuse Component of Incident Radiation (ω = 0.0)

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Table II Relative Depths of the 1% Subsurface Irradiance Level as a Function of Solar Zenith Angle and Diffuse Component of Incident Radiation (ω = 0.6)

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Table III Relative Depths of the 1% Subsurface Irradiance Level as a Function of Solar Zenith Angle and Diffuse Component of Incident Radiation (ω = 0.75)

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Table IV Relative Depths of the 1% Subsurface Irradiance Level as a Function of Solar Zenith Angle and Diffuse Component of Incident Radiation (ω = 0.9)

Equations (7)

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Z = 1 k av · ln [ 100 X ] .
Z 1 Z 2 = k av 2 k av 1 .
k av 1 k av 2 = k av ( ω , θ 1 , F 1 ) k av ( ω , θ 2 , F 2 ) = Z ( ω , θ 2 , F 2 ) Z ( ω , θ 1 , F 1 )
k = ( a 2 + n a b ) 0.5 ,
k av ( ω , 0,0 ) = ( a 2 + 0.230 a b ) 0.5 .
k av ( ω 1 , θ 1 , F 1 ) = k av ( ω 1 , 0,0 ) Z ( ω 1 , θ 1 , F 1 ) = ( a 1 2 + 0.230 a 1 b 1 ) 0.5 Z ( ω 1 , θ 1 , F 1 ) .
k av ( ω 2 , θ 2 , F 2 ) = k av ( ω 1 , θ 1 , F 1 ) · Z ( ω 1 , θ 1 , F 1 ) · k av ( ω 2 , 0,0 ) Z ( ω 2 , θ 2 , F 2 ) · k av ( ω 1 , 0,0 ) = k av ( ω 1 , θ 1 , F 1 ) · Z ( ω 1 , θ 1 , F 1 ) · ( a 2 2 + 0.230 a 2 b 2 ) 0.5 Z ( ω 2 , θ 2 , F 2 ) · ( a 1 2 + 0.230 a 1 b 1 ) 0.5 .

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