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Corrections

R. S. Scharlack, "All-dielectric compound parabolic concentrator: corrigenda," Appl. Opt. 17, 1482-1482 (1978)
https://www.osapublishing.org/ao/abstract.cfm?uri=ao-17-10-1482

References

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  1. R. Winston, J. Opt. Soc. Am. 60, 245 (1970).
    [Crossref]
  2. N. S. Kapany, A. Rabl, R. Winston, The Enrico Fermi Institute, U. of Chicago; also N. Goodman, R. Ignatius, L. Wharton, R. Winston, Appl. Opt. 15, 2434 (1976).
    [Crossref] [PubMed]
  3. A. Veneruso, SAND 76-0027 (1976).
  4. A. Meinel, M. Meinel, Applied Solar Energy (Addison Wesley, Reading, 1977).

1976 (1)

A. Veneruso, SAND 76-0027 (1976).

1970 (1)

Kapany, N. S.

N. S. Kapany, A. Rabl, R. Winston, The Enrico Fermi Institute, U. of Chicago; also N. Goodman, R. Ignatius, L. Wharton, R. Winston, Appl. Opt. 15, 2434 (1976).
[Crossref] [PubMed]

Meinel, A.

A. Meinel, M. Meinel, Applied Solar Energy (Addison Wesley, Reading, 1977).

Meinel, M.

A. Meinel, M. Meinel, Applied Solar Energy (Addison Wesley, Reading, 1977).

Rabl, A.

N. S. Kapany, A. Rabl, R. Winston, The Enrico Fermi Institute, U. of Chicago; also N. Goodman, R. Ignatius, L. Wharton, R. Winston, Appl. Opt. 15, 2434 (1976).
[Crossref] [PubMed]

Veneruso, A.

A. Veneruso, SAND 76-0027 (1976).

Winston, R.

R. Winston, J. Opt. Soc. Am. 60, 245 (1970).
[Crossref]

N. S. Kapany, A. Rabl, R. Winston, The Enrico Fermi Institute, U. of Chicago; also N. Goodman, R. Ignatius, L. Wharton, R. Winston, Appl. Opt. 15, 2434 (1976).
[Crossref] [PubMed]

J. Opt. Soc. Am. (1)

SAND 76-0027 (1)

A. Veneruso, SAND 76-0027 (1976).

Other (2)

A. Meinel, M. Meinel, Applied Solar Energy (Addison Wesley, Reading, 1977).

N. S. Kapany, A. Rabl, R. Winston, The Enrico Fermi Institute, U. of Chicago; also N. Goodman, R. Ignatius, L. Wharton, R. Winston, Appl. Opt. 15, 2434 (1976).
[Crossref] [PubMed]

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Figures (2)

Fig. 1
Fig. 1

Analysis.

Fig. 2
Fig. 2

Tracking requirement and acceptance angle for a dielectric filled CPC at 35° latitude during solstice.

Equations (8)

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tan η = tan α - tan Ψ cos δ tan α tan Ψ + cos δ ,
K x 2 + K y 2 + K z 2 = 1.
sin ϕ = K x ( K x 2 + K z 2 ) 1 / 2 ,
sin ϕ = K x ( 1 - K y 2 ) 1 / 2
sin ϕ = K x ( 1 - K y 2 ) 1 / 2
sin ϕ sin ϕ = n n [ 1 - ( n n ) 2 K y 2 1 - K y 2 ] 1 / 2 .
F = [ 1 - ( n n ) 2 ( cos γ tan δ ) 2 1 - ( cos γ tan δ ) 2 ] 1 / 2 .
C = 1 sin θ = F · ( n / n ) sin θ .

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