The Kuramoto model is a mathematical model of a large collection of coupled oscillators, each with its own natural frequency, in which every oscillator's phase is pulled toward the average phase of all the others by a coupling term whose strength is controlled by a single parameter shared across the whole system. It was introduced in 1975 by the Japanese physicist Yoshiki Kuramoto as a simplified, mathematically tractable version of an earlier, more general model of coupled oscillators proposed by Arthur Winfree, with the specific goal of capturing how large populations of independently rhythmic units, from flashing fireflies to firing neurons, can spontaneously fall into a shared rhythm. The model's central result is that synchronization does not appear gradually as the coupling strength increases but instead switches on abruptly once the coupling passes a sharp critical threshold, below which the oscillators drift independently and above which a growing fraction of them lock into a common phase, a transition that can be worked out in closed mathematical form in the idealized case of infinitely many oscillators. Because so many natural and engineered systems, including networks of power-grid generators, pacemaker cells in the heart, and applause in a crowd falling into unison clapping, show this same kind of spontaneous synchronization, the Kuramoto model remains one of the most widely applied tools for studying collective rhythmic behavior across physics, biology, and engineering.
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1. Wikidata: Kuramoto Model
Wikidata Q604374, class allow-list match (w-wdresolver-0926)View the Source Kuramoto model (Wikipedia)
In Branch: Dynamical Systems, LeadQuote, In Branch: Dynamical Systems, Lead
is a mathematical model used in describing synchronization
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