120 oscillators, each with its own natural frequency, each nudged toward the group’s mean phase with strength K.
Drag K. Tap to scatter phases. The same ?seed= always gives the same run.
LITThe Kuramoto model (1975), Kc = 2/(πg(0)) for the Lorentzian spread used here. r must stay in [0, 1], or the page throws.
AMBERPhases are continuous, unlike the pulse-coupled Firefly sphere.