David L. Fried: Difference between revisions

From Wikipedia, the free encyclopedia
Content deleted Content added
Jaraalbe (talk | contribs)
category
Jaraalbe (talk | contribs)
m see also
Line 10: Line 10:
* Fried, D. L. (1966) "Optical resolution through a randomly inhomogeneous medium for very long and very short exposures", J. Opt. Soc. Amer. 56:1372-9 [http://www.opticsinfobase.org/abstract.cfm?id=53167]
* Fried, D. L. (1966) "Optical resolution through a randomly inhomogeneous medium for very long and very short exposures", J. Opt. Soc. Amer. 56:1372-9 [http://www.opticsinfobase.org/abstract.cfm?id=53167]
* Fried, D. L. (1965) "Statistics of a Geometric Representation of Wavefront Distortion", J. Opt. Soc. Amer., 55:1427-1435.
* Fried, D. L. (1965) "Statistics of a Geometric Representation of Wavefront Distortion", J. Opt. Soc. Amer., 55:1427-1435.

==See also==
* [[Astronomical seeing]]


{{DEFAULTSORT:Fried, David L}}
{{DEFAULTSORT:Fried, David L}}

Revision as of 20:14, 11 November 2007

David L. Fried is a scientist, best known for his contributions to optics. Fried described what has come to be known as Fried's seeing diameter, or r0 (usually pronounced r-naught). The seeing diameter is effectively a limiting aperture due to atmospheric turbulence, and is found either empirically or statistically. The seeing diameter limits optical resolution. Note that it is a diameter, not a radius, even though r is used as the variable.

Typical values for Fried's seeing diameter in the visible spectrum may range from less than 1 cm (you can detect turbulence with your eye) to 20 cm on Mt. Haleakala.

Honors

1993 - David L. Fried, Optical Sciences Company, SPIE Technology Achievement Award.[1]

References

  • Fried, D. L. (1966) "Optical resolution through a randomly inhomogeneous medium for very long and very short exposures", J. Opt. Soc. Amer. 56:1372-9 [2]
  • Fried, D. L. (1965) "Statistics of a Geometric Representation of Wavefront Distortion", J. Opt. Soc. Amer., 55:1427-1435.

See also