BIFURCATIONS AND AMPLITUDE DEATH FROM DISTRIBUTED DELAYS IN COUPLED LANDAU STUART OSCILLATORS AND A CHAOTIC PARAMETRICALLY FORCED VAN DER POL-RAYLEIGH SYSTEM
{"title":"BIFURCATIONS AND AMPLITUDE DEATH FROM DISTRIBUTED DELAYS IN COUPLED LANDAU STUART OSCILLATORS AND A CHAOTIC PARAMETRICALLY FORCED VAN DER POL-RAYLEIGH SYSTEM","authors":"S. Choudhury, R. Roopnarain","doi":"10.17654/AM109020121","DOIUrl":null,"url":null,"abstract":"Distributed delays modeled by 'weak generic kernels' are introduced in the well-known coupled Landau-Stuart system, as well as a chaotic van der Pol-Rayleigh system with parametric forcing. The systems are close via the 'linear chain trick'. Linear stability analysis of the systems and conditions for Hopf bifurcation which initiates oscillations are investigated, including deriving the normal form at bifurcation, and deducing the stability of the resulting limit cycle attractor. The value of the delay parameter $a=a_{Hopf}$ at Hopf bifurcation picks out the onset of Amplitude Death(AD) in all three systems, with oscillations at larger values (corresponding to weaker delay). In the Landau-Stuart system, the Hopf-generated limit cycles for $a>a_{Hopf}$ turn out to be remarkably stable under very large variations of all other system parameters beyond the Hopf bifurcation point, and do not undergo further symmetry breaking, cyclic-fold, flip, transcritical or Neimark-Sacker bifurcations. This is to be expected as the corresponding undelayed systems are robust oscillators over wide ranges of their respective parameters. Numerical simulations reveal strong distortion and rotation of the limit cycles in phase space as the parameters are pushed far into the post-Hopf regime, and reveal other features, such as how the oscillation amplitudes and time periods of the physical variables on the limit cycle attractor change as the delay and other parameters are varied. For the chaotic system, very strong delays may still lead to the cessation of oscillations and the onset of AD (even for relatively large values of the system forcing which tends to oppose this phenomenon). Varying of the other important system parameter, the parametric excitation, leads to a rich sequence of dynamical behaviors, with the bifurcations leading from one regime (or type of attractor) into the next being carefully tracked.","PeriodicalId":89368,"journal":{"name":"Far east journal of applied mathematics","volume":"1 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2020-02-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Far east journal of applied mathematics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.17654/AM109020121","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
Abstract
Distributed delays modeled by 'weak generic kernels' are introduced in the well-known coupled Landau-Stuart system, as well as a chaotic van der Pol-Rayleigh system with parametric forcing. The systems are close via the 'linear chain trick'. Linear stability analysis of the systems and conditions for Hopf bifurcation which initiates oscillations are investigated, including deriving the normal form at bifurcation, and deducing the stability of the resulting limit cycle attractor. The value of the delay parameter $a=a_{Hopf}$ at Hopf bifurcation picks out the onset of Amplitude Death(AD) in all three systems, with oscillations at larger values (corresponding to weaker delay). In the Landau-Stuart system, the Hopf-generated limit cycles for $a>a_{Hopf}$ turn out to be remarkably stable under very large variations of all other system parameters beyond the Hopf bifurcation point, and do not undergo further symmetry breaking, cyclic-fold, flip, transcritical or Neimark-Sacker bifurcations. This is to be expected as the corresponding undelayed systems are robust oscillators over wide ranges of their respective parameters. Numerical simulations reveal strong distortion and rotation of the limit cycles in phase space as the parameters are pushed far into the post-Hopf regime, and reveal other features, such as how the oscillation amplitudes and time periods of the physical variables on the limit cycle attractor change as the delay and other parameters are varied. For the chaotic system, very strong delays may still lead to the cessation of oscillations and the onset of AD (even for relatively large values of the system forcing which tends to oppose this phenomenon). Varying of the other important system parameter, the parametric excitation, leads to a rich sequence of dynamical behaviors, with the bifurcations leading from one regime (or type of attractor) into the next being carefully tracked.
在著名的耦合Landau-Start系统以及具有参数强迫的混沌van der Pol-Rayleigh系统中引入了由“弱通用核”建模的分布式延迟。这两个系统通过“线性链技巧”接近。研究了系统的线性稳定性分析和引发振荡的Hopf分岔的条件,包括导出分岔处的正规形式,以及由此得到的极限环吸引子的稳定性。Hopf分岔处的延迟参数$a=a_{Hopf}$的值在所有三个系统中都选择了振幅死亡(AD)的开始,具有较大值的振荡(对应于较弱的延迟)。在Landau-Start系统中,$a>a_{Hopf}$的Hopf生成的极限环在Hopf分岔点以外的所有其他系统参数的非常大的变化下是非常稳定的,并且不经历进一步的对称性破坏、循环折叠、翻转、跨临界或Neimark-Sacker分岔。这是可以预期的,因为相应的未延迟系统在其各自参数的宽范围内是鲁棒振荡器。数值模拟揭示了当参数被推到后Hopf状态时,相空间中极限环的强烈畸变和旋转,并揭示了其他特征,如极限环吸引子上物理变量的振荡幅度和时间周期如何随着延迟和其他参数的变化而变化。对于混沌系统,非常强的延迟仍然可能导致振荡的停止和AD的开始(即使对于倾向于反对这种现象的相对较大的系统强迫值)。另一个重要的系统参数,即参数激励的变化,导致了一系列丰富的动力学行为,从一个状态(或类型的吸引子)到下一个状态的分叉被仔细跟踪。