Abstract

The description of ideal flux concentrators as shapes that do not disturb the geometrical vector flux field is extended to all the known types of ideal flux concentrators. This is accomplished, in part, by the introduction of vector flux sinks.

© 1981 Optical Society of America

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References

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  1. R. Winston and W. T. Welford, "Geometrical vector flux and some new nonimaging concentrators," J. Opt. Soc. Am. 69, 532–536 (1979).
  2. R. Winston and W. T. Welford, "Ideal flux concentrators as shapes that do not disturb the geometrical vector flux field: a new derivation of the compound parabolic concentrator," J. Opt. Soc. Am. 69, 536–539 (1980).
  3. W. T. Welford and R. Winston, The Optics of Nonimaging Concentrators (Academic, New York, 1978).
  4. A. Rabl and R. Winston, "Ideal concentrators for finite sources and restricted exit angles," Appl. Opt. 15, 2880–2883 (1976).
  5. M. Collares-Pereira, A. Rabl, and R. Winston, "Lens-mirror combinations with maximal concentration," Appl. Opt. 16, 2677–2683 (1977).
  6. A. Rabl, "Solar concentrators with maximal concentration for cylindrical absorbers," Appl. Opt. 15, 1871–1873 (1976).
  7. M. E. Barnett, "The geometrical vector flux field within a compound elliptical concentrator," Optik 54, 429–432 (1980).

1980 (2)

1979 (1)

1977 (1)

1976 (2)

Barnett, M. E.

M. E. Barnett, "The geometrical vector flux field within a compound elliptical concentrator," Optik 54, 429–432 (1980).

Collares-Pereira, M.

Rabl, A.

Welford, W. T.

Winston, R.

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