尚轶伦 上海交通大学 数学系

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Synchronization in Networks of Coupled Harmonic Oscillators with Stochastic Perturbation and Time Delays. 尚轶伦 上海交通大学 数学系. Outline. Introduction ● Backgrounds ● Problem formulation Main result ● Synchronization of coupled harmonic oscillators - PowerPoint PPT Presentation

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  • Synchronization in Networks of Coupled Harmonic Oscillators with Stochastic Perturbation and Time Delays

  • OutlineIntroduction Backgrounds Problem formulationMain result Synchronization of coupled harmonic oscillators Methods of proofNumerical examples

  • Synchronized oscillatorsCellular clocks in the brainPacemaker cells in the heartPedestrians on a bridgeElectric circuitsLaser arraysOscillating chemical reactionsBubbly fluidsNeutrino oscillationsSynchronous firings of male fireflies

  • Kuramoto modelAll-to-all interactionIntroduced by Kuramoto in 1975 as a toy model of synchronization

  • We want to study synchronization conditions for coupled harmonic oscillators over general directed topologies with noise perturbation and communication time delays.

  • Basic definitions For a matrix A, let ||A||=sup{ ||Ax||: ||x||=1}. ||.|| is the Euclidean norm. Let G=(V, E, A) be a weighted digraph with vertex set V={1, 2,..., n} and edge set E. An edge (j, i) E if and only if the agent j can send information to the agent i directly. The in-degree neighborhood of the agent i : Ni ={ j V : (j, i) E}. A=(aij) Rnn is the weighted adjacency matrix of G. aij >0 if and only if j Ni. D=diag(d1,..., dn) with di=|Ni|. The Laplacian matrix L=(lij) =D-A.

  • Our model Consider n coupled harmonic oscillators connected by dampers and each attached to fixed supports by identical springs with spring constant k. The dynamical system is described as xi+kxi+jNiaij(xi-xj)=0 for i=1,, n where xi denotes the position of the ith oscillator, k is a positive gain, and aij characterizes interaction between oscillators i and j.

  • Here, we study a leader-follower version of the above system. Communication time delay and stochastic noises during the propagation of information from oscillator to oscillator are introduced. xi(t)+kxi(t)+jNiaij(xi(t-s)-xj(t-s))+bi(xi(t-s)-x0(t-s))+ [jNipij(xi(t-s)-xj(t-s))+qi(xi(t-s)-x0(t-s))]wi(t) = 0 for i=1,, n (1) x0(t)+kx0(t)=0, (2) where s is the time delay and x0 is the position of the virtual leader, labeled as oscillator 0.

  • Let B=diag(b1,, bn) be a diagonal matrix with nonnegative diagonal elements and bi>0 if and only if 0Ni. W(t):=(w1(t),,wn(t))T is an n dimensional standard Brownian motion. Let Ap=(pij) Rnn and Bp=diag(q1,, qn) be two matrices representing the intensity of noise. Let pi=jpij, Dp=diag(p1,, pn), and Lp=Dp-Ap.

  • Convergence analysis Let ri=xi and vi=xi for i=0,1,, n. Write r=(r1,, rn)T and v=(v1,,vn)T. Let r0(t)=cos(kt)r0(0)+(1/k)sin(kt)v0(0) v0(t)=-ksin(kt)r0(0)+cos(kt)v0(0) Then r0(t) and v0(t) solve Equation (2) x0(t)+kx0(t)=0

  • Let r*=r-r01 and v*=v-v01. we can obtain an error dynamics of (1) and (2) as follows dz(t)=[Ez(t)+Fz(t-s)]dt+Hz(t-s)dW(t) where, z= (r*, v*)T,

    E= , F= , H=

    and W(t) is an 2n dimensional standard Brownian motion.

    0 In-kIn 00 00 -L-B0 00 -Lp-Bp

  • The theorem Theorem: Suppose that vertex 0 is globally reachable in G. If ||H||2||P||+2||PF|| {8s2[(k1)2+||F||2]+2s||H||2}
  • Method of proof Consider an n dimensional stochastic differential delay equation dx(t)=[Ex(t)+Fx(t-s)]dt+g(t,x(t),x(t-s))dW(t) (3) where E and F are nn matrices, g : [0, ) RnRnRnm is locally Lipschitz continuous and satisfies the linear growth condition with g(t,0,0) 0. W(t) is an m dimensional standard Brownian motion.

  • Lemma (X. Mao): Assume that there exists a pair of symmetric positive definite nn matrices P and Q such that P(E+F)+(E+F)TP=-Q. Assume also that there exist non-negative constants a and b such that Trace[gT(t,x,y)g(t,x,y)] a||x||2+b||y||2 for all (t,x,y). If (a+b)||P||+2||PF||{2s(4s(||E||2+||F||2)+a+b)}
  • Simulations We consider a network G consisting of five coupled harmonic oscillators including one leader indexed by 0 and four followers.

  • Let aij=1 if jNi and aij=0 otherwise; bi=1 if 0Ni and bi=0 otherwise. Take the noise intensity matrices Lp=0.1L and Bp=0.1B. Take Q=I8 with Eigenvaluemin(Q)=1. Calculate to get ||H||=0.2466 and ||F||=2.4656. In what follows, we will consider two different gains k.

  • Firstly, take k=0.6 such that ||E||=1>k. We solve P from the equation P(E+F)+(E+F)TP=-Q and get ||P||=8.0944 and ||PF||=4.1688. Conditions in the Theorem are satisfied by taking time delay s=0.002. Take initial value z(0)=(-5, 1,4, -3, -8, 2, -1.5, 3)T.

  • ||r*||0

  • ||v*||0

  • Secondly, take k=2 such that ||E||=k>1. In this case, we get ||P||=8.3720 and ||PF||=7.5996. Conditions in the Theorem are satisfied by taking time delay s=0.001. Take the same initial value z(0).

  • ||r*||0

  • ||v*||0

  • The value of k not only has an effect on the magnitude and frequency of the synchronized states (as implied in the Theorem), but also affects the shapes of synchronization error curves ||r*|| and ||v*||.

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