Synchronous states in time-delay coupled periodic oscillators: a stability criterion (Q375575)

From MaRDI portal





scientific article; zbMATH DE number 6221408
Language Label Description Also known as
English
Synchronous states in time-delay coupled periodic oscillators: a stability criterion
scientific article; zbMATH DE number 6221408

    Statements

    Synchronous states in time-delay coupled periodic oscillators: a stability criterion (English)
    0 references
    31 October 2013
    0 references
    chaotic behavior
    0 references
    delay differential equations
    0 references
    oscillators
    0 references
    stability
    0 references
    bifurcation
    0 references
    The authors consider two systems of two delay coupled oscillators represented by phase-locked loops with the measured phase differences \(\varphi^{(1,2)}(t)\) and \(\varphi^{(2,1)}(t)\). Firstly, for a node filter represented by a constant gain, the first order system NEWLINE\[NEWLINE \dot{\varphi}^{(i,j)}(t)=-\mu_{0}\varphi^{(i,j)}(t)-\mu_{1}[\sin(\varphi^{(i,j)}(t)+\omega_{M}\tau)-\sin(\varphi^{(j,i)}(t-\tau)+\omega_{M}\tau)],\;i\neq j, NEWLINE\]NEWLINE with positive constants \(\mu_{0}\) and \(\mu_{1}\) is obtained. Secondly, for a filter \(F(s)=\alpha_{0}/(s+\beta_{0})\), the second order system NEWLINE\[NEWLINE\ddot{\varphi}^{(i,j)}(t)=-\mu_{0}\dot{\varphi}^{(i,j)}(t)-\mu_{1}\varphi^{(i,j)}(t)-\mu_{2}[\sin(\varphi^{(i,j)}(t)+\omega_{M}\tau)-\sin(\varphi^{(j,i)}(t-\tau)+\omega_{M}\tau)],\;i\neq j,NEWLINE\]NEWLINE with positive constants \(\mu_{0}\), \(\mu_{1}\) and \(\mu_{2}\) is obtained.NEWLINENEWLINEFor both system a linear stability analysis of the trivial solution is carried out. For the first order system this shows that the trivial solution is always stable. For the second order system the trivial solution is stable for \(\tau=0\) and conditions for a first destabilizing Hopf-bifurcation are given. This is illustrated by numerical simulations. The authors also present simulations far from this bifurcation, where seemingly chaotic trajectories are presented.
    0 references

    Identifiers

    0 references
    0 references
    0 references
    0 references
    0 references
    0 references