The resolving power of a telescope is the smallest angular separation it can distinguish, set by the diffraction of light at its aperture. This tool computes both the empirical Dawes limit and the theoretical Rayleigh limit in arcseconds, so you can tell at a glance how tight a double star you can split.
How it works
Two standard formulas are used. The Dawes limit (empirical, for equal-brightness double stars) is:
Dawes (arcsec) = 116 / aperture_in_mm
The Rayleigh criterion (theoretical diffraction limit) is derived from the diffraction angle and converted from radians to arcseconds:
Rayleigh (rad) = 1.22 × wavelength / aperture
Rayleigh (arcsec) = Rayleigh_rad × 206265
Here 206265 is the number of arcseconds in one radian. Wavelength and aperture
must be in the same units, so the tool converts your aperture from mm and the
wavelength from nm to metres before dividing.
Why two different limits?
The Dawes limit was established empirically by William Rutter Dawes in the 19th century by observing many double stars through many apertures. It describes the minimum separation at which a skilled observer can detect a notch between two stars of similar brightness — the point where the Airy disks just touch. It assumes green-yellow light and good seeing.
The Rayleigh criterion comes from wave optics. Two point sources are considered resolved when the central maximum of one falls on the first minimum of the other. The Rayleigh number is consistently a few percent larger (coarser) than the Dawes limit, meaning it is a slightly more conservative standard.
In practice, visual observers with excellent seeing and equal-magnitude targets often reach or beat the Dawes limit. For unequal pairs — one star much brighter than the other — the glare of the primary makes the dimmer star harder to distinguish, and neither formula accounts for that; real splitting power on unequal pairs degrades noticeably.
Resolution across common apertures
For illustration (at 550 nm, the default green reference wavelength):
| Aperture | Dawes limit | Rayleigh limit |
|---|---|---|
| 60 mm | 1.93” | 2.32” |
| 100 mm | 1.16” | 1.39” |
| 150 mm | 0.77” | 0.93” |
| 200 mm | 0.58” | 0.70” |
| 300 mm | 0.39” | 0.46” |
These are the optical limits of the telescope alone. On a typical night, atmospheric turbulence (seeing) blurs detail to 1 to 2 arcseconds regardless of how large the aperture is. Scopes larger than about 150 mm rarely reach their theoretical limit from an average site; the benefit of more aperture shifts to light-gathering rather than splitting power.
When to use which limit
Use the Dawes limit when you want to know whether a specific visual double star is splittable — it is calibrated for that task. Use the Rayleigh limit for general diffraction calculations, astrophotography planning, and comparing results across wavelengths, since it changes correctly with wavelength (shorter blue light gives finer resolution; longer red light gives coarser).