Understanding the telescope calculator — concept and principle
This calculator turns four numbers printed on a telescope and eyepiece into what you will actually see: magnification, true field, focal ratio, exit pupil, resolving power, faintest visible star and the highest useful magnification. Use it to choose eyepieces or compare telescopes.
How it is calculated
- Magnification = telescope focal length F ÷ eyepiece focal length f.
- True field ≈ eyepiece apparent field ÷ magnification (degrees).
- Focal ratio = F ÷ aperture D.
- Exit pupil = D ÷ magnification (mm).
- Dawes limit = 116 ÷ D(mm) arcseconds.
- Limiting magnitude ≈ 2.7 + 5 log₁₀ D(mm), one common rule of thumb.
- Maximum useful magnification ≈ 2 × D(mm).
The principle
The objective forms an image at its focal plane and the eyepiece magnifies it, so angles grow by F/f; dividing the eyepiece's fixed apparent angle by that factor gives the sky you see. Collected light leaves the eyepiece as a beam the width of the exit pupil; if it is wider than your pupil (about 7 mm when young and dark-adapted, less with age) light is wasted. Resolution is limited by diffraction: a larger aperture makes smaller star images, and William Dawes found empirically that equal double stars separated by 116/D arcseconds can just be split. Light grasp scales with aperture area, and each factor of 100 in brightness is 5 magnitudes, hence the 5 log D term.
Worked example
- Inputs: D = 200 mm, F = 1200 mm, f = 25 mm, apparent field 52°.
- Magnification = 1200 ÷ 25 = 48×.
- True field = 52 ÷ 48 = 1.083333333° (65′), two full Moons wide.
- Focal ratio = 1200 ÷ 200 = f/6.
- Exit pupil = 200 ÷ 48 = 4.166666667 mm.
- Dawes limit = 116 ÷ 200 = 0.58″.
- Limiting magnitude = 2.7 + 5 × log₁₀ 200 = 2.7 + 11.505 = 14.20514998.
- Maximum useful magnification = 2 × 200 = 400×.
| Eyepiece focal length (mm) | Magnification |
|---|---|
| 6.25 | 192 |
| 12.5 | 96 |
| 18.8 | 64 |
| 25 | 48 |
| 31.2 | 38.4 |
| 37.5 | 32 |
| 50 | 24 |
How to read the result
Exit pupils of 4–7 mm suit wide views of nebulae and galaxies, 1–2 mm suit planets and the Moon, and below about 0.5 mm the image becomes dim and blurry. The theoretical maximum of 400× is rarely usable, because atmospheric turbulence (seeing) usually limits sharp views to far less.
Common mistakes
- Judging a telescope by its magnification; aperture determines brightness and detail.
- Using a Barlow lens without multiplying the telescope focal length by its factor.
- Treating the limiting magnitude as guaranteed; light pollution can cut it by several magnitudes.
Frequently asked questions
What is the lowest useful magnification?
About D ÷ 7 (here roughly 29×), which makes the exit pupil equal to a 7 mm eye pupil. Lower power wastes light.
Is the Rayleigh criterion the same as the Dawes limit?
No. The Rayleigh criterion, 1.22 λ/D, is about 138/D(mm) arcseconds for green light, a stricter separation than Dawes' empirical 116/D.
Sources: W. R. Dawes, Catalogue of micrometrical measurements of double stars, Memoirs of the Royal Astronomical Society 35 (1867) · E. Hecht, Optics, 5th ed., Pearson, 2017 (telescopes and diffraction)