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Kuramoto modelThe Kuramoto model, first proposed by Yoshiki Kuramoto (蔵本 由紀 Kuramoto Yoshiki), is a mathematical model used to describe synchronization. More specifically, it is a model for the behavior of a large set of coupled oscillators. Its formulation was motivated by the behavior of systems of chemical and biological oscillators, and it has found widespread applications. The model makes several assumptions, including that there is weak coupling, identical or nearly identical oscillators, and that interactions that depend sinusoidally on the phase difference between the two objects. Additional recommended knowledge
DefinitionIn the most popular version of the Kuramoto model, each of the oscillators is considered to have its own intrinsic natural frequency ω_{i}, and each is coupled equally to all other oscillators. Surprisingly, this fully nonlinear model can be solved exactly, in the infiniteN limit, with a clever transformation and the application of selfconsistency arguments. The most popular form of the model has the following governing equations:
where the system is composed of N limitcycle oscillators.
where ζ_{i} is the fluctuation and a function of time. If we consider the noise to be white noise, then
TransformationThe transformation that allows this model to be solved exactly (at least in the N → ∞ limit) is as follows. Define the "order" parameters r and ψ as
Here r represents the phasecoherence of the population of oscillators, and ψ indicates the average phase. Applying this transformation, the governing equation becomes
Thus the oscillators' equations are no longer explicitly coupled; instead the order parameters govern behavior. A further transformation is usually done, to a rotating frame in which the statistical average of phases over all oscillators is zero. That is, ψ = 0. Finally, the governing equation becomes
Large N limitNow consider the case as N tends to infinity. Take the distribution of intrinsic natural frequencies as g(ω) (assumed normalized). Then assume that the density of oscillators at a given phase θ, with given natural frequency ω, at time t is ρ(θ,ω,t). Normalization requires that The continuity equation for oscillator density will be where v is the drift velocity of the oscillators given by taking the infiniteN limit in the transformed governing equation, i.e., Finally, we must rewrite the definition of the order parameters for the continuum (infinite N) limit. θ_{i} must be replaced by its ensemble average (over all ω) and the sum must be replaced by an integral, to give SolutionsThe incoherent state with all oscillators drifting randomly corresponds to the solution ρ = 1 / (2π). In that case r = 0, and there is no coherence among the oscillators. They are uniformly distributed across all possible phases, and the population is in a statistical steadystate (although individual oscillators continue to change phase in accordance with their intrinsic ω). When coupling K is sufficiently strong, a fully synchronized solution is possible. In the fully synchronized state, all the oscillators share a common frequency, although their phases are different. A solution for the case of partial synchronization yields a state in which only some oscillators (those near the ensemble's mean natural frequency) synchronize; other oscillators drift incoherently. Mathematically, the state has for locked oscillators, and for drifting oscillators. The cutoff occurs when  ω  < Kr. ReferencesAcebrón, Juan A.; Bonilla, L. L.; Pérez Vicente, Conrad J.; Ritort, Félix; Spigler, Renato. The Kuramoto model: a simple paradigm for synchronization phenomena [1] Strogatz, S. From Kuramoto to Crawford: exploring the onset of synchronization in populations of coupled oscillators, Physica D 143 (2000) 1–20 

This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Kuramoto_model". A list of authors is available in Wikipedia. 