计算倍分叉的一种方法

本文从Melnikov函数的物理意义出发,建立了一种计算倍分叉方法.利用这种方法,具体地讨论了软弹簧Duffing系统的倍分叉现象,发现了与次谐分叉相类似结论——即在阻尼小、外激励幅度大时,会出现倍分叉.这样的结果与物理事实是相吻合的.     

非线性参数振动系统的共振分叉解

本文研究了非线性参数激励振动系统在主共振、亚谐共振、超谐共振和分数共振等各种情况下的分叉解,给出了在非退化条件下分叉图的各种可能的拓扑结构,证明了在δ大于ε的条件下也可能存在分叉解,图1第1区域对应零解的事实,可作为非线性系统振动控制的理论基础.     

1:1内共振条件下矩形薄板的全局分叉和多脉冲混沌动力学

首次利用广义Melnikov方法研究了一个四边简支矩形薄板的全局分叉和多脉冲混沌动力学．矩形薄板受面外的横向激励和面内的参数激励．利用von Krmn模型和Galerkin方法得到一个二自由度非线性非自治系统用来描述矩形薄板的横向振动．在1∶1内共振条件下,利用多尺度方法得到一个四维的平均方程．通过坐标变换把平均方程化为标准形式,利用广义Melnikov方法研究该系统的多脉冲混沌动力学,并且解释了矩形薄板模态间的相互作用机理．在不求同宿轨道解析表达式的前提下,提供了一个计算Melnikov函数的方法．进一步得到了系统的阻尼、激励幅值和调谐参数在满足一定的限制条件下,矩形薄板系统会存在多脉冲混沌运动．数值模拟验证了该矩形薄板的确存在小振幅的多脉冲混沌响应．     

双霍普夫分叉规范型的计算

研究了一般四维系统的双霍普夫分叉的规范型,提出计算这类规范型的一种方法.作为应用,最后给出了一个例子.     

Z2等变奇点理论及参激系统的1/2亚谐分叉

从周期参数激励系统——Mathieu-Duffing方程的时间对称性出发,讨论了它的1/2亚谐分叉,利用Liapunov-Schmidt约化导出了Z₂等变的代数分叉方程,并建立与此对应的分析方法:Z₂等变的奇点理论,得到了1/2亚谐分叉的全体分叉图,数值计算验证了这些结果.     

一类具有二维分叉方程的积分方程的分叉

本文研究一类含参数的非线性积分方程的分叉问题,其中的积分算子的线性化算子在分叉值点处有二维零空间。利用Liapunov-Schmidt约化方法和基于系统的对称性的群论方法,得到了周期分叉解存在的充分条件。     

具有参数及受迫激励的二阶系统的次谐波与混沌解

具有受迫激励的二阶非线性振子由次谐波分叉导致混沌,已有许多文献讨论过。而具有脉冲非线性参数激励的二阶系统的次谐分叉现象曾由徐皆苏等作过系统讨论。本文则讨论在实际中更有价值的两种激励同时作用的二阶系统     

用集结坐标法对细杆中呼吸子状态的分析

研究了计入Peierls-Nabarro(P-N)力和材料粘性效应的一维无限长金属杆在简谐外力扰动下的动力响应,导出了类sine-Gordon 型的运动方程．在集结坐标(collective coordinate）下原控制方程可以用常微分动力系统描述,研究系统中呼吸子的运动．根据非线性动力学方法分析,P-N力的幅值和频率的变化将改变双曲鞍点的位置,并改变系统次谐分叉的阈值,但不改变由奇阶次谐分叉通向混沌的路径．通过实例给出了P-N力幅值和P-N力频率对细杆动力响应的详细影响过程,可见混沌发生的区域是一个半无限区域,并随着P-N力的增大而增大．P-N力的频率对系统有类似的影响．     

《非线性Mathieu方程亚谐共振分叉理论》的一些推广

在文[1]中,作者讨论了非线性Mathieu方程的亚谐共振分叉理论,得到的主要结果是,在参数α-β平面上,具有六种不同拓扑结构的分叉图.本文摧广了这一结果,指出:如果选取不同的芽来计算同样的分叉问题,则可以有十四种不同拓扑结构的分叉图.     

白噪声参激Hopf分叉系统的两次分叉研究

本文研究了白噪声参数激励下的Hopf分叉系统的两次分叉行为．明确了由于噪声的介入而使得系统的分叉类型产生了实质性的改变并导致了分叉点的漂移．     

Fold-Hopf bifurcation,steady state,self-oscillating and chaotic behavior in an electromechanical transducer with nonlinear control

We investigate the nonlinear dynamics of an electromechanical transducer formed by a ferromagnetic mobile piece subjected to harmonic base oscillations. The normal form theory is applied to analyze the stability conditions of a Fold-Hopf bifurcation generated by a nonlinear control law consisting of an excitation electric tension and an external force applied to the mobile piece. The self-oscillating behavior is studied from the Krylov–Bogoliuvov method to deduce an approximate equation for the frequency of the oscillation that arises from the Fold-Hopf bifurcation. This information is used to choose appropriate values for the amplitude and frequency of the harmonic base vibrations to obtain chaotic oscillations. The chaotic motions are examined by means of sensitivity dependence, Lyapunov exponents, power spectral density, Poincaré sections and bifurcation diagram. The chaotic oscillations are used in conjunction with the nonlinear control law to drive the mobile piece to a desired set point. A detailed computational study allows us to corroborate the analytical results.     

Bifurcation and chaos in escape equation model by incremental harmonic balancing

Periodic motions of the nonlinear system representing the escape equation with cosine and sine parametric excitations and external harmonic excitations are obtained by the incremental harmonic balance (IHB) method. The system contains quadratic stiffness terms. The Jacobian matrix and the residue vector for the type of nonlinearity with parametric excitation are explicitly derived. An arc length path following procedure is used in combination with Floquet theory to trace the response diagram and to investigate the stability of the periodic solutions. The system undergoes chaotic motion for increase in the amplitude of the harmonic excitation which is investigated by numerical integration and represented in terms of phase planes, Poincaré sections and Lyapunov exponents. The interpolated cell mapping (ICM) method is used to obtain the initial condition map corresponding to two coexisting period 1 motions. The periodic motions and bifurcation points obtained by the IHB method compare very well with results of numerical integration.     

Chaos and chaos synchronization for a non-autonomous rotational machine systems

Chaos and chaos synchronization of the centrifugal flywheel governor system are studied in this paper. By mechanics analyzing, the dynamical equation of the centrifugal flywheel governor system is established. Because of the non-linear terms of the system, the system exhibits both regular and chaotic motions. The characteristic of chaotic attractors of the system is presented by the phase portraits and power spectra. The evolution from Hopf bifurcation to chaos is shown by the bifurcation diagrams and a series of Poincaré sections under different sets of system parameters, and the bifurcation diagrams are verified by the related Lyapunov exponent spectra. This letter addresses control for the chaos synchronization of feedback control laws in two coupled non-autonomous chaotic systems with three different coupling terms, which is demonstrated and verified by Lyapunov exponent spectra and phase portraits. Finally, numerical simulations are presented to show the effectiveness of the proposed chaos synchronization scheme.     

非线性弹性梁中的混沌带现象

研究了非线性弹性梁的混沌运动,梁受到轴向载荷的作用。非线性弹性梁的本构方程可用三次多项式表示。计及材料非线性和几何非线性,建立了系统的非线性控制方程。利用非线性Galerkin法,得到微分动力系统。采用Melnikov方法对系统进行分析后发现,当载荷P₀和f满足一定条件时,系统将发生混沌运动,且混沌运动的区域呈现带状。还详尽分析了从次谐分岔到混沌的路径,确定了混沌发生的临界条件。     

Global chaos in a periodically forced, linear system with a dead-zone restoring force

The Poincare mapping and the corresponding mapping sections for global motions in a linear system possessing a dead-zone restoring force are introduced through switching planes pertaining to two constraints. The global periodic motions based on the Poincare mapping are determined, and the eigenvalue analysis for the stability and bifurcation of periodic motion is carried out. Global chaos in such a system is investigated numerically from the unstable global periodic motions analytically determined. The bifurcation scenario with varying parameters is presented. The mapping structures of periodic and chaotic motions are discussed. The Poincare mapping sections for global chaos are given for illustration. The grazing phenomenon embedded in chaotic motion is observed in this investigation.     

Dynamic analysis, controlling chaos and chaotification of a SMIB power system

The dynamic behaviors of a SMIB power system are studied in this paper. A single modal equation is used to analyze the qualitative behaviors of the system. The famous equation of motion is called “swing equation”. The Lyapunov direct method is applied to obtain conditions of stability of the equilibrium points of the system. The bifurcation of the parameter dependent system is studied numerically. Besides, the phase portraits, the Poincaré maps, and the Lyapunov exponents are presented to observe periodic and chaotic motions. Further, the addition of periodic force and the feedback control are used to control chaos effectively. Finally, the chaotification problem of the SMIB power system is also issued.     

带控制面机翼结构基于弧长数值连续法的颤振特征研究

以三自由度二元机翼为研究对象,将浮沉位移和俯仰位移方向的非线性刚度简化为立方非线性,对于存在间隙的控制面采用双线性刚度代替.考虑准定常气流,建立气动弹性运动方程,通过数值模拟构造峰值-峰值图,反映其在不同气流速度下的振动特征.通过弧长数值连续法构造系统的分岔图,结合Floquet算子研究其稳定性及其分岔类型,所得分岔图和数值模拟的结果相吻合.由分岔图可得系统由于控制面双线性的存在,导致机翼结构振动形态多变,存在多个分岔点和多个不稳定区间,不仅存在极限环振动和非光滑准周期振动,而且在某些不稳定区间出现混沌现象.     

Flow switchability and periodic motions in a periodically forced,discontinuous dynamical system

This paper presents the switchability of a flow from one domain into another one in the periodically forced, discontinuous dynamical system. The inclined line boundary in phase space is used for the dynamical system to switch. The normal vector field product for flow switching on the separation boundary is introduced. The passability condition of a flow to the separation boundary is achieved through such a normal vector field product, and the sliding and grazing conditions to the separation boundary are presented as well. Using mapping structures, periodic motions in such a discontinuous system are predicted analytically, and the corresponding local stability and bifurcation analysis are carried out. With the analytical conditions of grazing and sliding motions, the parameter maps of specific motions are developed. Illustrations of periodic and chaotic motions are given, and the normal vector fields are presented to show the analytical criteria. This investigation may help one better understand the sliding mode control. The methodology presented in this paper can be applied to discontinuous, nonlinear systems.     

Homoclinic bifurcation and chaos control in MEMS resonators

The chaotic dynamics of a micromechanical resonator with electrostatic forces on both sides are investigated. Using the Melnikov function, an analytical criterion for homoclinic chaos in the form of an inequality is written in terms of the system parameters. Detailed numerical studies including basin of attraction, and bifurcation diagram confirm the analytical prediction and reveal the effect of parametric excitation amplitude on the system transition to chaos. The main result of this paper indicates that it is possible to reduce the electrostatically induced homoclinic and heteroclinic chaos for a range of values of the amplitude and the frequency of the parametric excitation. Different active controllers are applied to suppress the vibration of the micromechanical resonator system. Moreover, a time-varying stiffness is introduced to control the chaotic motion of the considered system. The techniques of phase portraits, time history, and Poincare maps are applied to analyze the periodic and chaotic motions.     

A periodically forced,piecewise linear system. Part I: Local singularity and grazing bifurcation

A methodology for the local singularity of non-smooth dynamical systems is systematically presented in this paper, and a periodically forced, piecewise linear system is investigated as a sample problem to demonstrate the methodology. The sliding dynamics along the separation boundary are investigated through the differential inclusion theory. For this sample problem, a perturbation method is introduced to determine the singularity of the sliding dynamics on the separation boundary. The criteria for grazing bifurcation are presented mathematically and numerically. The grazing flows are illustrated numerically. This methodology can be very easily applied to predict grazing motions in other non-smooth dynamical systems. The fragmentation of the strange attractors of chaotic motion will be presented in the second part of this work.