Single Slit Diffraction - Wave Optics Visualization

Interactive simulation demonstrating wave diffraction through a single aperture with real-time intensity visualization

Diffraction Optical Path

Slit Width a: 5 μm
Screen Distance L: 1.0 m
Central Fringe Width: 0 mm

Intensity Distribution I(θ) = I₀·[sin(β)/β]²

Dark Fringes (Minima):

Simulated Diffraction Pattern on Screen

Bright Dark

Diffraction Parameters

Slit Properties

Light Properties

Display Options

Quick Presets

Diffraction Formulas

Intensity: I(θ) = I₀·[sin(β)/β]²
Beta Parameter: β = (πa·sinθ)/λ
Dark Fringes: a·sinθ = mλ (m = ±1, ±2, ...)
Central Width: Δx = 2λL/a

What is Single Slit Diffraction?

Single slit diffraction is a wave phenomenon where light spreads out after passing through a narrow aperture. Unlike the ray model of light, which would predict a sharp shadow, wave optics predicts that light bends around corners and creates a characteristic pattern of bright and dark fringes on a screen.

Diffraction Mechanism

When a plane wave encounters a single slit of width a, each point in the slit acts as a source of secondary spherical wavelets (Huygens' principle). These wavelets interfere with each other, creating a pattern on the screen. The central maximum is the brightest and widest region where most of the light is concentrated. Secondary maxima appear on either side but are much dimmer (approximately 4.5%, 1.6%, 0.8% of central intensity for the first three orders). Dark fringes (minima) occur where destructive interference cancels the light.

Intensity Pattern

The intensity distribution follows the sinc² function: I(θ) = I₀·[sin(β)/β]² where β = (πa·sinθ)/λ. At θ = 0, β = 0 and using the limit sin(β)/β = 1, we get maximum intensity I₀. Minima occur when β = mπ (m = ±1, ±2, ...), corresponding to angles where a·sinθ = mλ. The central bright fringe has angular width 2λ/a (distance between first minima on both sides). Secondary maxima occur approximately at β ≈ (m + ½)π.

Effect of Slit Width

The slit width a inversely affects the spread of the diffraction pattern: narrower slits produce wider patterns (Δx ∝ 1/a), while wider slits produce narrower patterns. In the limit a ≫ λ, the diffraction becomes negligible and ray optics applies. Conversely, when a ≈ λ, the pattern becomes very wide with pronounced wave behavior. This is a general principle in wave physics: smaller apertures or obstacles cause more diffraction.

Effect of Wavelength

Longer wavelengths (red light) diffract more than shorter wavelengths (blue light), producing wider patterns. This is why Δx ∝ λ. This wavelength dependence is why we see rainbows from CD/DVD reflections (diffraction grating) and why prism effects occur. In white light diffraction, each wavelength creates its own pattern, resulting in colored fringes with red diffracted most on the outer edges.

Applications

Single slit diffraction has numerous applications: measuring the width of thin objects (hair, wire) by analyzing their diffraction pattern, determining the wavelength of unknown light sources, studying crystal structures using X-ray diffraction (though typically with multiple slits/gratings), optical instrument design (telescope and microscope resolution limits), and understanding the fundamental wave nature of light and matter. The diffraction limit determines the maximum resolution of any optical system: resolution ≈ 1.22λ/D for circular apertures.