
First zero of the Airy disk for a circular apertureThe Airy disk is the bright central spot in the diffraction pattern produced by a point source of light passing through a circular aperture. The Airy disk constant is the angular radius at which the intensity of this pattern first drops to zero, marking the boundary between the central bright region and the surrounding rings. For a circular aperture, this first zero occurs at an angle given by 1.22 times the wavelength divided by the aperture diameter.
The pattern was first described by George Biddell Airy in 1835, who derived the mathematical form of the diffraction pattern for a circular aperture.
When light passes through a circular opening, it doesn't simply cast a sharp shadow; instead, diffraction causes the waves to spread and interfere. The resulting pattern on a screen shows a central bright spot surrounded by faint rings. The first dark ring, where intensity falls to zero, defines the Airy disk. The constant 1.22 arises from the mathematics of Bessel functions, which describe the wave interference for a circular geometry.
The Airy disk constant sets the fundamental resolution limit for optical instruments like telescopes and microscopes, known as the diffraction limit, which determines how close two point sources can be and still be distinguished.
The same 1.22 factor appears in the design of radio telescopes and even in the focusing of laser beams, making it a universal constant for any wave-based imaging system.
| θ | variable | angular resolution — angular resolution radian |
| λ | variable | wavelength of light — wavelength metre |
| D | variable | aperture diameter — diameter metre |
| 1.22 | constant | First zero of the Airy disk for a circular aperture — airy disk constant = 1.22 |






