Discretize and solve Chimera state model

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The discussion focuses on discretizing and solving the Chimera state model for coupled oscillators as presented by Daniel M. Abrams and Steven H. Strogatz. The key equation for discretization is given as \(\dot{\phi_i} = \omega_i - \frac{1}{N}\sum_{j=1}^N G(x_i-x_j')\sin[(\phi(x_i,t)-\phi(x_j',t)+\alpha]\), where \(G(x) = \frac{1}{2\pi}(1+A\cos x)\). The parameters include \(x = \pm \pi\), \(\alpha = \frac{\pi}{2} - 0.18\), \(A = 0.995\), and \(N=256\). The Runge-Kutta solver is recommended for implementation with a time step of \(dt = 0.025\) over 200,000 iterations, starting from \(\phi(x)=6rexp(-0.76x^2)\), where \(r\) is a random variable between -0.5 and 0.5.

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This discussion is beneficial for researchers in nonlinear dynamics, mathematicians studying differential equations, and physicists interested in the behavior of coupled oscillators and Chimera states.

Chaos08
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Hi all,

We are working on a paper - Chimera States for Coupled Osscillators from Daniel M. Abrams and Steven H. Strogatz.
We have the following formula of the simplest system that supports a chimera state:
[tex]\frac{\partial\phi}{\partial t} = \omega - \displaystyle\int^\pi_{-\pi} G(x-x')\sin[\phi(x,t)-\phi(x',t)+\alpha]dx'[/tex]
Now we have to discretize it and 'ODE' it.
Our discretization looks like:
[tex]\dot{\phi_i} = \omega_i - \frac{1}{N}\displaystyle\sum_{j=1}^N G(x_i-x_j')\sin[(\phi(x_i,t)-\phi(x_j',t)+\alpha][/tex]
Where [tex]\phi[/tex] is the phase of the oscilator at position x at time t, i is the current oscillator and j are the oscillators in the ring.
[tex]G(x) = \frac{1}{2\pi}(1+A\cos x)[/tex]
Now we have to solve this equation with [tex]x = \pm \pi \quad \alpha = \frac{\pi}{2} - 0.18 \quad A = 0.995 \quad N=256[/tex]
The solver Runge-Kutta has to be used with dt = 0.025 for 200000 iterations and starting from [tex]\phi(x)=6rexp(-0.76x^2)[/tex]. r is a random variable between -0.5 and 0.5

Who can help us.

Regards
 
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