The angle of diffraction is inversely proportional to the slit separation; as the slit separation increases, the angle decreases.

The angle of diffraction is inversely proportional to the slit width; as the slit width decreases, the angle increases.

The angular position of the first minimum is inversely proportional to the slit width; as the slit width decreases, the angle increases.

The angular width of the central maximum is inversely proportional to the slit width; as the slit width increases, the angular width decreases.

Longer wavelengths diffract more, leading to larger angles of diffraction in a diffraction grating.

When light passes through a circular aperture, it exhibits Fresnel diffraction, characterized by a pattern of concentric rings.

A circular aperture produces an Airy pattern, characterized by a central bright spot surrounded by concentric dark and bright rings.

A larger slit width results in less pronounced diffraction, leading to a narrower central maximum.

The angular width of a diffraction maximum is defined as the angle between the first minimum on either side of the central maximum.

The condition for the first minimum in a single-slit diffraction pattern is given by a sin(θ) = λ, where 'a' is the slit width and 'λ' is the wavelength.

The condition for the first minimum in single-slit diffraction is given by a sin(θ) = mλ, where m = 1 for the first minimum.

Diffraction is utilized in various applications including optical instruments, radio transmission, and medical imaging.

Diffraction is a phenomenon that leads to interference patterns, as it involves the bending of waves around obstacles.

Diffraction gratings can produce multiple orders of maxima due to the constructive interference of light waves.

Diffraction can occur with any type of wave, including sound, light, and water waves.

A circular aperture produces an Airy pattern, characterized by a central bright spot surrounded by concentric dark and bright rings.