Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Optical telescope
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
===Angular resolution=== Ignoring blurring of the image by turbulence in the atmosphere ([[astronomical seeing|atmospheric seeing]]) and optical imperfections of the telescope, the [[angular resolution]] of an optical telescope is determined by the diameter of the [[primary mirror]] or lens gathering the light (also termed its "aperture"). The [[Angular resolution#The_Rayleigh_criterion|Rayleigh criterion]] for the resolution limit <math>\alpha_R</math> (in [[radian]]s) is given by :<math>\sin(\alpha_R) = 1.22 \frac{\lambda}{D}</math> where <math>\lambda</math> is the [[wavelength]] and <math>D</math> is the aperture. For [[visible light]] (<math>\lambda</math> = 550 nm) in the [[small-angle approximation]], this equation can be rewritten: :<math>\alpha_R = \frac{138}{D}</math> Here, <math>\alpha_R</math> denotes the resolution limit in [[arcsecond]]s and <math>D</math> is in millimeters. In the ideal case, the two components of a [[double star]] system can be discerned even if separated by slightly less than <math>\alpha_R</math>. This is taken into account by the [[Dawes limit]] :<math>\alpha_D = \frac{116}{D}</math> The equation shows that, all else being equal, the larger the aperture, the better the angular resolution. The resolution is not given by the maximum [[magnification]] (or "power") of a telescope. Telescopes marketed by giving high values of the maximum power often deliver poor images. For large ground-based telescopes, the resolution is limited by [[astronomical seeing|atmospheric seeing]]. This limit can be overcome by placing the telescopes above the atmosphere, e.g., on the summits of high mountains, on balloons and high-flying airplanes, or [[space telescope|in space]]. Resolution limits can also be overcome by [[adaptive optics]], [[speckle imaging]] or [[lucky imaging]] for ground-based telescopes. Recently, it has become practical to perform [[aperture synthesis]] with arrays of optical telescopes. Very high resolution images can be obtained with groups of widely spaced smaller telescopes, linked together by carefully controlled optical paths, but [[List of astronomical interferometers at visible and infrared wavelengths|these interferometers]] can only be used for imaging bright objects such as stars or measuring the bright cores of [[active galaxies]].
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)