QiLing Tools

🌗Diffraction & Interference Simulator - Single/Double Slit, Grating, Airy Disk, Thin Film Colors, Malus's Law

A wave-optics bench that runs in your browser, in four parts. Slits and gratings: set the wavelength, slit width a, separation d, number of slits N and screen distance L to see the exact intensity I(θ) = I₀[sinβ/β]²[sinNγ/(N sinγ)]² and the pattern on the screen, with minima, bright orders and missing orders marked; white-light mode sums every wavelength through the D65 spectrum and CIE colour-matching functions to show the real coloured fringes. Circular apertures: two point sources imaged as Airy disks [2J₁(x)/x]², with a slider to watch them become just resolved, and Rayleigh limits for the eye, a phone camera, binoculars or the Hubble telescope. Thin films use the exact multiple-reflection formula to give reflectance spectra and colours for soap bubbles, oil slicks, MgF₂ coatings, wedges and Newton's rings. The polarizer bench lets you drag up to four polarizers to check Malus's law and the three-polarizer paradox.

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How to use Diffraction, Interference & Polarization

  1. 1Pick a module: slits and gratings, circular aperture, thin films or polarizers
  2. 2Choose a preset or move the sliders for wavelength, slit width, separation, aperture, film thickness, refractive index or polarizer angle
  3. 3Read the screen pattern, intensity curve, Airy image, reflected colour or transmitted intensity, along with minima positions, resolution limits, reflectance and the formulas used

FAQ

How do I calculate double-slit fringe spacing, and why do some bright fringes disappear?
For small angles the spacing between bright fringes is Δy ≈ λL/d, so a 632.8 nm laser with d = 0.25 mm and L = 1 m gives about 2.53 mm. The real pattern is the two-slit term multiplied by the single-slit envelope [sinβ/β]². When a bright order d sinθ = mλ lands exactly on an envelope minimum a sinθ = kλ, i.e. when m·a/d is a whole number, that order is missing. With d = 5a the ±5th and ±10th orders vanish.
What is the Rayleigh criterion, and how small an angle can the eye or a telescope resolve?
A circular aperture images a point as an Airy disk whose central spot has angular radius θ = 1.22λ/D. Two points are just resolved when the centre of one disk falls on the first dark ring of the other; the intensity between them then dips to about 73.5% of the peak. At 550 nm a 3 mm pupil gives about 46″ (the retina limits the eye to roughly 1′ in practice), and Hubble's 2.4 m mirror about 0.058″, enough to separate features about 100 m apart on the Moon.
Why are soap bubbles colourful, and why do they turn black just before popping?
Light reflected from the front and back of the film interferes. The path difference is 2nd cosθ, plus a half-wave phase shift at the front surface, so some wavelengths reinforce and others cancel, and the reflected light is coloured; the colours cycle as the thickness changes. When the film becomes much thinner than the wavelength (below about 30 nm) the two reflections differ by almost exactly half a wave and cancel, so the top of a draining bubble looks black. Very thick films overlap many orders and look white again.
Why is an anti-reflection coating a quarter wavelength thick?
On glass with n = 1.52, a MgF₂ layer with n ≈ 1.38 gives a half-wave shift at both surfaces, which cancel. The two reflections then interfere destructively when the round trip 2nd equals λ/2, i.e. nd = λ/4. Designed for 550 nm this means d ≈ 99.6 nm, and the reflectance falls from 4.3% for bare glass to about 1.3%; an ideal coating with n = √1.52 ≈ 1.23 would reach zero. Because the cancellation is complete only at the design wavelength, coated lenses often look faintly purple.
How can adding a third polarizer between two crossed ones let light through?
Malus's law says polarized light passing a polarizer at angle θ keeps I cos²θ. Unpolarized light leaves the first polarizer (0°) with I₀/2; meeting a 90° polarizer next gives cos²90° = 0, total darkness. A 45° polarizer in between first projects the light onto 45° (I₀/4) and the last one projects it onto 90° (I₀/8). The middle polarizer changes the polarization direction, so polarizers project rather than filter; with more polarizers in smaller steps the output approaches I₀/2.