Two speakers, one slit, and the geometry of agreement.
A room seen from above. Two sources hum at the same pitch and circular wavefronts spread from each. Where two crests arrive together you see a bright stripe; where a crest meets a trough, silence. Slide a wall in, pierce it once, then twice — and the famous fringes of the double-slit experiment appear on their own. Drag everything. Hold to freeze and look.
Notes from the workshop
§ 06 · ReadingHow it works
§ 06 · Method
Each pixel of the room samples a sum of sinusoids. For a source S and a receiver at
distance d, the field is sin(kd − ωt) / √d, with k = 2π/λ
and ω = 2πf. The square-root attenuation is the two-dimensional analogue of the
inverse-square law and keeps the picture honest near a source.
A wall, when present, is opaque except where you have cut slits. Past it, each open slit is treated as a fresh Huygens source — the path from speaker to receiver runs through one of the apertures, and we add the contributions from every open slit. This is the cleanest path to the familiar fringes without simulating a full wave-equation grid.
Bright cells are wave crests at the present instant, dark cells are troughs. The interference is not a render trick: shift either source by half a wavelength and watch a bright fringe slide precisely to where a dark one used to be.