Teaching · For Teachers · Astronomy
Type the telescope’s aperture and focal length and the eyepieces in the box. The calculator gives the magnification and the slice of sky each one shows, and says whether the full Moon will fit.
The worked example is made up: a 130 mm, 650 mm focal length reflector, the kind many schools and libraries lend, with three eyepieces. Nothing you type leaves this browser.
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Aperture and focal length are printed on the tube or in the manual, usually in millimeters.
Focal length is printed on the eyepiece. Apparent field is in its specifications; 52° is common for Plössl eyepieces.
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Three divisions for every eyepiece.
Magnification is the telescope’s focal length, times the Barlow factor, divided by the eyepiece’s focal length. The true field, the patch of sky you see, is close to the eyepiece’s apparent field divided by the magnification. The exit pupil, the beam of light leaving the eyepiece, is the aperture divided by the magnification. The Dawes limit, 116 divided by the aperture in millimeters, gives the closest pair of equal stars the telescope can split, in arcseconds.
About twice the aperture in millimeters (50× per inch) is the most magnification a telescope can use, and the air on most nights allows less. An exit pupil wider than about 7 mm, the most a young dark-adapted eye opens, wastes light, which sets the lowest useful power. The widest field is best for finding objects and for large ones such as the Pleiades; higher power is for the Moon’s craters, planets and double stars.
The worked example is made up. The true field is the common apparent-field approximation, close to within a few percent; field-stop measurements are more exact. Your figures stay in this browser. Support: team@caveatacademic.com.