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Petzval field curvature

From Wikipedia, the free encyclopedia

Optical aberration
Out-of-focus image of a spoke target..svg
Defocus

HartmannShack 1lenslet.svg Tilt
Spherical aberration 3.svg
Spherical aberration
Astigmatism.svg
Astigmatism
Lens coma.svg
Coma
Barrel distortion.svg
Distortion
Field curvature.svg
Petzval field curvature
Chromatic aberration lens diagram.svg
Chromatic aberration

Field curvature: the image "plane" (the arc) deviates from a flat surface (the vertical line).
Field curvature: the image "plane" (the arc) deviates from a flat surface (the vertical line).

Petzval field curvature, named for Joseph Petzval,[1] describes the optical aberration in which a flat object normal to the optical axis (or a non-flat object past the hyperfocal distance) cannot be brought properly into focus on a flat image plane.[citation needed]

It is not to be confused with flat-field correction, which refers to brightness uniformity.

Analysis

The image-sensor array of the Kepler space observatory is curved to compensate for the telescope's Petzval curvature.
The image-sensor array of the Kepler space observatory is curved to compensate for the telescope's Petzval curvature.

Consider an "ideal" single-element lens system for which all planar wave fronts are focused to a point at distance f from the lens. Placing this lens the distance f from a flat image sensor, image points near the optical axis will be in perfect focus, but rays off axis will come into focus before the image sensor, dropping off by the cosine of the angle they make with the optical axis. This is less of a problem when the imaging surface is spherical, as in the human eye.

Most current photographic lenses are designed to minimize field curvature, and so effectively have a focal length that increases with ray angle. Lenses of short focal lengths (ultra wide, wide and normal) below 50 mm typically suffer more from field curvature. Telephoto lenses typically have very little or no visible field curvature.[2] The Petzval lens is one design which has significant amount of field curvature; images taken with the lens are very sharp in the centre, but at greater angles the image is out of focus. Film cameras, may be able to bend their image planes to compensate, particularly when the lens is fixed and known. This also includes plate film, which could still be bent slightly. Digital sensors are difficult to bend, although experimental products have been produced.[3] By 2016 the only consumer cameras featuring curved sensors were "selfie" Sony Cybershot KW-1 and KW-11.[citation needed] Large mosaics of sensors (necessary anyway due to limited chip sizes) can be shaped to simulate a bend over larger scales.[citation needed]

The Petzval field curvature is equal to the Petzval sum over an optical system,

where is the radius of the i th surface and the n s are the indices of refraction on the first and second side of the surface.[4] Petzval curvature of a spherical mirror is double of its curvature and Petzval radius of a mirror is equal to its focal length.

Reduction of field curvature aberration

One method to reduce this aberration is to insert an aperture stop (iris) in order to remove edge light rays. This method, however, greatly decreases the light collecting power of the lens.[5]

See also

References

  1. ^ Riedl, Max J. (2001). Optical Design Fundamentals for Infrared Systems. SPIE Press. pp. 40–. ISBN 9780819440518. Retrieved 3 November 2012.
  2. ^ Mansurov, Nasim (February 12, 2018). "What is Field Curvature?". photographylife.com. Retrieved April 28, 2018.
  3. ^ Sanyal, Rishi (June 18, 2014). "Sony's curved sensors may allow for simpler lenses and better images". Digital Photography Review. Retrieved April 28, 2018.
  4. ^ Kingslake, Rudolf (1989). A History of the Photographic Lens. Academic Press. pp. 4–. ISBN 9780124086401. Retrieved 3 November 2012.
  5. ^ "Lens aberrations: field curvature". microscopy.berkeley.edu.
This page was last edited on 22 May 2021, at 01:32
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