基于延时反馈的电力非线性系统Hopf分岔反控制

针对无刷直流电机等效非线性动力系统,设计基于Washout滤波器辅助和延迟反馈相结合的控制器对系统进行Hopf分岔反控制.根据Hopf分岔理论讨论系统在稳定的平衡点处发生Hopf分岔时,延迟参数应满足的条件.讨论结果表明,当延迟参数满足一定条件时,可使系统在所期望的平衡点处发生Hopf分岔,从而实现系统的Hopf分岔反控制.此外,方法也可用于混沌控制.数值仿真证明了控制器的有效性.     

一个四维超混沌Lorenz系统的Hopf分岔分析

运用非线性动力学理论,对一类四维混沌Lorenz系统在平衡点的稳定性问题和Hopf分岔的存在性进行了研究.利用第一Lyapunov系数法给出系统Hopf分岔周期解的稳定性条件.最后,通过数值仿真验证了理论推导的正确性.     

一类具稀疏效应的Predator-Prey系统的分岔及混沌

得到了一类稀疏效应下的Predator-Prey系统发生静态分岔和Hopf分岔条件,证明了此类系统存在混沌现象.     

延迟积分-微分方程的敏感度和Hopf分岔分析

本文考虑了一类延迟积分-微分方程的Hopf分岔分析.利用敏感性方程,确定了一个合适的Hopf参数.基于Hopf分岔理论得到,当系统存在Hopf分岔时系统参数必须满足的条件.为了得到Hopf参数的精确值,进一步讨论了延迟积分-微分方程的离散形式,利用Newton迭代法,得到了参数的逼近值.最后,数值仿真说明了我们的理论的有效性.     

Rssler原型4系统的Hopf分岔及幅值控制

主要研究了一类Rssler原型4系统的Hopf分岔行为及极限环幅值控制问题.首先,利用Hopf分岔理论讨论系统发生Hopf分岔的条件,利用规范形理论判定系统的Hopf分岔类型,并给出极限环幅值算式;然后,对系统施加非线性反馈控制器,判定受控系统的Hopf分岔类型,并给出极限环幅值算式,讨论控制参数对极限环幅值的影响.最后,对讨论结果进行数值仿真,通过理论与仿真结果得出结论:非线性控制器可以改变极限环幅值大小,但不能改变Hopf分岔位置.     

单时滞类Chen系统Hopf分岔分析

根据非线性动力学理论,以一类新的单时滞Chen系统为分析对象,针对其平衡点的稳定性和Hopf分岔参数等问题进行研究.根据Routh-Hurwitz判据分析了其平衡点的稳定性,通过计算得到单时滞Chen系统特征根的分布,进一步分析得出系统在零平衡点附近是渐进稳定的.结合Hopf分岔理论,运用特征根的分布结果,确定出系统发生Hopf分岔的时滞参数,并给出Hopf分岔条件.通过多组实验仿真验证了理论分析的正确性.     

新三维指数系统及其控制系统的Hopf分岔分析

考虑了一个新三维指数系统的Hopf分岔,并且分析了指数系统添加非线性控制器后的Hopf分岔.通过严格的数学推导给出受控系统发生余维一,余维二和余维三的Hopf分岔的参数条件,证明了可以控制系统在指定区域内发生退化分岔和可调控分岔的稳定性,并且通过数值模拟验证了得出的结论.     

时滞扰动类Lorenz系统的Hopf分岔

通过非线性动力学理论,对时滞类Lorenz系统在平衡点的稳定性问题和发生Hopf分岔的条件进行了研究.首先计算得到系统的平衡点,然后通过分析系统在平衡点处的相应特征方程根的分布,得到系统在平衡点局部渐近稳定和产生Hopf分岔的时滞临界点.以时滞为分叉参数,研究了时滞系统存在Hopf分岔的条件.最后,利用Matlab程序进行仿真验证所得结论与理论分析一致.本文的结论是对一些已有文献研究成果的推广.     

一类SEIS模型的分岔及混沌

建立了一类更为符合实际疫情的种群动态变化下新的SEIS模型,得到了系统的平衡点渐近稳定条件、Hopf分岔以及稳定的极限环,给出了多参数变化对系统混沌的影响和易感种群增减对系统混沌区域伸缩的制约,并附有数值模拟和仿真.     

双摆内共振分岔分析

应用normal form理论,首先分析了复摆自治系统在1:1内共振临界点附近的Hopf分岔解及其在参数平面上的分岔转迁集的解析表达式,并与数值解进行了比较;然后,应用数值方法,得到了复摆非自治系统通向混沌的过程。     

Bifurcation of an eco-epidemiological model with a nonlinear incidence rate

A predator-prey system with disease in the prey is considered. Assume that the incidence rate is nonlinear, we analyse the boundedness of solutions and local stability of equilibria, by using bifurcation methods and techniques, we study Bogdanov-Takens bifurcation near a boundary equilibrium, and obtain a saddle-node bifurcation curve, a Hopf bifurcation curve and a homoclinic bifurcation curve. The Hopf bifurcation and generalized Hopf bifurcation near the positive equilibrium is analyzed, one or two limit cycles is also discussed.     

DYNAMICAL BEHAVIORS FOR A THREE－DIMENSIONAL DIFFERENTIAL EQUATION IN CHEMICAL SYSTEM

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HOPF BIFURCATION AND OTHER DYNAMICAL BEHAVIORS FOR A FOURTH ORDER DIFFERENTIAL EQUATION IN MODELS OF INFECTIOUS DISEASE

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HOPF BIFURCATION DIAGRAM OF TIME-DELAY LINARD EQUATION

In this paper, we provide a Hopf bifurcation diagram of Lienard equation with a discrete delay, by using the (?) - D decomposition, one can determine the stability domain of the equilibrium and Hopf bifurcation curves in the parameter space.     

Stochastic resonance induced by novel random transitions of motion of FitzHugh–Nagumo neuron model

In contrast to the previous studies which have dealt with stochastic resonance induced by random transitions of system motion between two coexisting limit cycle attractors in the FitzHugh–Nagumo (FHN) neuron model after Hopf bifurcation and which have dealt with the phenomenon of stochastic resonance induced by external noise when the model with periodic input has only one attractor before Hopf bifurcation, in this paper we have focused our attention on stochastic resonance (SR) induced by a novel transition behavior, the transitions of motion of the model among one attractor on the left side of bifurcation point and two attractors on the right side of bifurcation point under the perturbation of noise. The results of research show: since one bifurcation of transition from one to two limit cycle attractors and the other bifurcation of transition from two to one limit cycle attractors occur in turn besides Hopf bifurcation, the novel transitions of motion of the model occur when bifurcation parameter is perturbed by weak internal noise; the bifurcation point of the model may stochastically slightly shift to the left or right when FHN neuron model is perturbed by external Gaussian distributed white noise, and then the novel transitions of system motion also occur under the perturbation of external noise; the novel transitions could induce SR alone, and when the novel transitions of motion of the model and the traditional transitions between two coexisting limit cycle attractors after bifurcation occur in the same process the SR also may occur with complicated behaviors types; the mechanism of SR induced by external noise when FHN neuron model with periodic input has only one attractor before Hopf bifurcation is related to this kind of novel transition mentioned above.     

Hopf-flip bifurcations of vibratory systems with impacts

Two vibro-impact systems are considered. The period n single-impact motions and Poincaré maps of the vibro-impact systems are derived analytically. Stability and local bifurcations of single-impact periodic motions are analyzed by using the Poincaré maps. A center manifold theorem technique is applied to reduce the Poincaré map to a three-dimensional one, and the normal form map associated with Hopf-flip bifurcation is obtained. It is found that near the point of codim 2 bifurcation there exists not only Hopf bifurcation of period one single-impact motion, but also Hopf bifurcation of period two double-impact motion. Period doubling bifurcation of period one single-impact motion is commonly existent near the point of codim 2 bifurcation. However, no period doubling cascade emerges due to change of the type of period two fixed points and occurrence of Hopf bifurcation associated with period two fixed points. The results from simulation shows that there exists an interest torus doubling bifurcation occurring near the value of Hopf-flip bifurcation. The torus doubling bifurcation makes the quasi-periodic attractor associated with period one single-impact motion transit to the other quasi-periodic attractor represented by two attracting closed circles. The torus bifurcation is qualitatively different from the typical torus doubling bifurcation occurring in the vibro-impact systems.     

Hopf-Bifurkation bei Lasern

The semiclassical equations describing a ring laser show two successive bifurcations, one stationary and one Hopf bifurcation. This phenomenon is analyzed mathematically. The initial value problem for the laser equations and the stability of the stationary solutions are discussed in detail. The transition to ultrashort laser pulses is shown to be a Hopf bifurcation. The direction of the bifurcation is determined for a numerical example. It turns out that it depends on the parameters of the system.     

Effects of Hard Limits on Bifurcation, Chaos and Stability

An SMIB model in the power systems,especially that concering the effects of hard limits onbifurcations,chaos and stability is studied.Parameter conditions for bifurcations and chaos in the absence ofhard limits are compared with those in the presence of hard limits.It has been proved that hard limits can affectsystem stability.We find that (1) hard limits can change unstable equilibrium into stable one;(2) hard limits canchange stability of limit cycles induced by Hopf bifurcation;(3) persistence of hard limits can stabilize divergenttrajectory to a stable equilibrium or limit cycle;(4) Hopf bifurcation occurs before SN bifurcation,so the systemcollapse can be controlled before Hopf bifurcation occurs.We also find that suitable limiting values of hard limitscan enlarge the feasibility region.These results are based on theoretical analysis and numerical simulations,such as condition for SNB and Hopf bifurcation,bifurcation diagram,trajectories,Lyapunov exponent,Floquetmultipliers,dimension of attractor and so on.     

Synchronous dynamics of two coupled oscillators with inhibitory-to-inhibitory connection

We investigate the behaviour of a neural network model consisting of two coupled oscillators with delays and inhibitory-to-inhibitory connections. We consider the absolute synchronization and show that the connection topology of the network plays a fundamental role in classifying the rich dynamics and bifurcation phenomena. Regarding eigenvalues of the connection matrix as bifurcation parameters, we obtain codimension one bifurcations (including fold bifurcation and Hopf bifurcation) and codimension two bifurcation (including fold-Hopf bifurcations and Hopf–Hopf bifurcations). Based on the normal form theory and center manifold reduction, we obtain detailed information about the bifurcation direction and stability of various bifurcated equilibria as well as periodic solutions with some kinds of spatio-temporal patterns. Numerical simulation is also given to support the obtained results.     

Numerical solution of Hopf bifurcation problems

We present two numerical methods for the solution of Hopf bifurcation problems involving ordinary differential equations. The first one consists in a discretization of the continuous problem by means of shooting or multiple shooting methods. Thus a finite-dimensional bifurcation problem of special structure is obtained. It may be treated by appropriate iterative algorithms. The second approach transforms the Hopf bifurcation problem into a regular nonlinear boundary value problem of higher dimension which depends on a perturbation parameter ?. It has isolated solutions in the ?-domain of interest, so that conventional discretization methods can be applied. We also consider a concrete Hopf bifurcation problem, a biological feedback inhibition control system. Both methods are applied to it successfully.