Ferrofluid Interface: Fourier-Mode Dispersion
Interactive 2D Fourier-mode model of a ferrofluid/air interface: each angular perturbation mode grows or decays according to a real magnetic-vs-tension dispersion relation, and a cubic (Landau) saturation term selects the finger spacing you can watch emerge live.
This is the 2D counterpart to the 3D Hele-Shaw ferrofluid grid simulation. Instead of a cellular-automaton lattice, it represents the fluid/air boundary as a sum of angular Fourier modes and integrates each mode's amplitude directly from a magnetic-vs-tension dispersion relation, with a cubic saturation term that selects a stable finger spacing once growth saturates. The result is the same physical competition — magnetic surface energy elongating the interface, surface tension shortening it — computed as an explicit ODE system rather than approximated by local growth probabilities, so you can watch the dominant wavenumber shift live as you move the field and tension sliders.
A 2D Fourier-mode solver for the same ferrofluid Hele-Shaw instability: each angular boundary mode grows or decays under a real magnetic-vs-tension dispersion relation with cubic (Landau) saturation, so you watch the dominant finger-spacing wavenumber emerge from the ODEs themselves.
2D · HTML5 Canvas 2D · 60 FPS target · runs fully client-side, no install