The stochastic response of a noisy system with non-negative restoring force is investigated. The generalized cell mapping （GCM） method compute the transient and stationary probability density functions （PDFs） real...The stochastic response of a noisy system with non-negative restoring force is investigated. The generalized cell mapping （GCM） method compute the transient and stationary probability density functions （PDFs） real-power is used to Combined with the global properties of the noise-free system, the evolutionary process of the tran- sient PDFs is revealed. The results show that stochastic P-bifurcation occurs when the system parameter varies in the response analysis and the stationary PDF evolves from bimodal to unimodal along the unstable manifold during the bifurcation.展开更多
应用广义胞映射图论方法(GCMD)研究SD(smooth and discontinuous systems)振子的内部激变现象.通过对SD常微分方程系统的全局分析发现周期解通向混沌的内部激变现象是由于周期吸引子与在其吸引域内部的混沌鞍碰撞产生的.混沌鞍是胞空间...应用广义胞映射图论方法(GCMD)研究SD(smooth and discontinuous systems)振子的内部激变现象.通过对SD常微分方程系统的全局分析发现周期解通向混沌的内部激变现象是由于周期吸引子与在其吸引域内部的混沌鞍碰撞产生的.混沌鞍是胞空间中的瞬态自循环胞集,周期吸引子与混沌鞍发生碰撞后,混沌鞍转化为混沌吸引子新增的一部分;内部激变不会改变原来吸引域的形状且具有可逆性和对扰动的不敏感性.同时改进广义胞映射图论方法,提出盒子维数的广义胞映射图论方法的近似计算方法.展开更多
The generalized cell mapping(GCM) method is used to obtain the stationary response of a single-degree-of-freedom.Vibro-impact system under a colored noise excitation. In order to show the advantage of the GCM method, ...The generalized cell mapping(GCM) method is used to obtain the stationary response of a single-degree-of-freedom.Vibro-impact system under a colored noise excitation. In order to show the advantage of the GCM method, the stochastic averaging method is also presented. Both of the two methods are tested through concrete examples and verified by the direct numerical simulation. It is shown that the GCM method can well predict the stationary response of this noise-perturbed system no matter whether the noise is wide-band or narrow-band, while the stochastic averaging method is valid only for the wide-band noise.展开更多
运用广义胞映射图方法研究两个周期激励作用下Duffing-van der Pol系统的全局特性.发现了系统的混沌瞬态以及两种不同形式的瞬态边界激变,揭示了吸引域和边界不连续变化的原因.瞬态边界激变是由吸引域内部或边界上的混沌鞍和分形边界上...运用广义胞映射图方法研究两个周期激励作用下Duffing-van der Pol系统的全局特性.发现了系统的混沌瞬态以及两种不同形式的瞬态边界激变,揭示了吸引域和边界不连续变化的原因.瞬态边界激变是由吸引域内部或边界上的混沌鞍和分形边界上周期鞍的稳定流形碰撞产生.第一种瞬态边界激变导致吸引域突然变小,吸引域边界突然变大;第二种瞬态边界激变使两个不同的吸引域边界合并成一体.此外,在瞬态合并激变中两个混沌鞍发生合并,最后系统的混沌瞬态在内部激变中消失.这些广义激变现象对混沌瞬态的研究具有重要意义.展开更多
利用广义胞映射方法,研究了加性和乘性泊松白噪声联合作用下SD振子(smooth and discontinuous oscillator)的随机响应问题.基于图分析算法,获得确定SD振子的吸引子、吸引域、域边界、鞍和不变流形等全局特性.基于矩阵分析算法,计算了SD...利用广义胞映射方法,研究了加性和乘性泊松白噪声联合作用下SD振子(smooth and discontinuous oscillator)的随机响应问题.基于图分析算法,获得确定SD振子的吸引子、吸引域、域边界、鞍和不变流形等全局特性.基于矩阵分析算法,计算了SD振子在泊松白噪声激励下的瞬态和稳态响应.结果表明:随机响应的概率密度函数演化方向和确定情况下的不稳定流形形状之间存在密切联系.蒙特卡罗模拟结果表明,所使用的方法是有效且准确的.展开更多
Crisis and stochastic bifurcation of the hardening Helmholtz-Duffing oscillator are studied by means of the generalized cell mapping method using digraph.For the system subject to a single deterministic harmonic excit...Crisis and stochastic bifurcation of the hardening Helmholtz-Duffing oscillator are studied by means of the generalized cell mapping method using digraph.For the system subject to a single deterministic harmonic excitation,our study reveals that a series of crisis phenomena can occur when the system parameter passes through different critical values,including chaotic boundary crisis,regular boundary crisis and interior crisis.A chaotic boundary crisis due to the collision of regular attractor with chaotic saddle embedded in a fractal basin boundary and an interior crisis due to the collision of regular attractor with chaotic saddle of its attraction basin are discovered.A new phenomenon,namely the global properties of dynamical system show symmetric as system parameter is varied,can be also revealed according to our analysis.For the system subject to a combination of a deterministic harmonic excitation and a random excitation,it is found that stochastic bifurcation,defined as a sudden change in character of a stochastic attractor,can occur one after another when the noise intensity passes through different critical values.This kind of stochastic bifurcation corresponds to stochastic crisis essentially.Our study also reveals that the generalized cell mapping method using digraph is a powerful tool not only for the crisis behavior analysis of deterministic system,but also for the global property analysis of stochastic bifurcation.展开更多
Stochastic bifurcations of the SD （smooth and discontinuous） oscillator with additive and/or multiplicative bounded noises are studied by the generalized cell mapping method using digraph analysis algorithm. From th...Stochastic bifurcations of the SD （smooth and discontinuous） oscillator with additive and/or multiplicative bounded noises are studied by the generalized cell mapping method using digraph analysis algorithm. From the global viewpoint, stochastic bifur- cation can be described as a sudden change in shape and size of a random attractor as the system parameter valies. The evolu- tionary process of stochastic bifurcation in the SD oscillator is shown in detail. Meanwhile, we show the phenomenon that un- der stochastic excitation the shape and size of random attractor and random saddle change along with the direction of unstable manifold. A plane stochastic bifurcation diagram is included.展开更多
基金Project supported by the National Natural Science Foundation of China(Nos.11172233,11302169,11302170,and 11472212)the Fundamental Research Funds for the Central Universities(No.3102014JCQ01079)
文摘The stochastic response of a noisy system with non-negative restoring force is investigated. The generalized cell mapping （GCM） method compute the transient and stationary probability density functions （PDFs） real-power is used to Combined with the global properties of the noise-free system, the evolutionary process of the tran- sient PDFs is revealed. The results show that stochastic P-bifurcation occurs when the system parameter varies in the response analysis and the stationary PDF evolves from bimodal to unimodal along the unstable manifold during the bifurcation.
文摘应用广义胞映射图论方法(GCMD)研究SD(smooth and discontinuous systems)振子的内部激变现象.通过对SD常微分方程系统的全局分析发现周期解通向混沌的内部激变现象是由于周期吸引子与在其吸引域内部的混沌鞍碰撞产生的.混沌鞍是胞空间中的瞬态自循环胞集,周期吸引子与混沌鞍发生碰撞后,混沌鞍转化为混沌吸引子新增的一部分;内部激变不会改变原来吸引域的形状且具有可逆性和对扰动的不敏感性.同时改进广义胞映射图论方法,提出盒子维数的广义胞映射图论方法的近似计算方法.
基金supported by the National Natural Science Foundation of China (Grant No. 11772149)the Research Fund of State Key Laboratory of Mechanics and Control of Mechanical Structures,Nanjing University of Aeronautics and Astronautics,China (Grant No. MCMS-I-19G01)the Project Funded by the Priority Academic Program Development of Jiangsu Higher Education Institutions (PAPD),China。
文摘The generalized cell mapping(GCM) method is used to obtain the stationary response of a single-degree-of-freedom.Vibro-impact system under a colored noise excitation. In order to show the advantage of the GCM method, the stochastic averaging method is also presented. Both of the two methods are tested through concrete examples and verified by the direct numerical simulation. It is shown that the GCM method can well predict the stationary response of this noise-perturbed system no matter whether the noise is wide-band or narrow-band, while the stochastic averaging method is valid only for the wide-band noise.
文摘运用广义胞映射图方法研究两个周期激励作用下Duffing-van der Pol系统的全局特性.发现了系统的混沌瞬态以及两种不同形式的瞬态边界激变,揭示了吸引域和边界不连续变化的原因.瞬态边界激变是由吸引域内部或边界上的混沌鞍和分形边界上周期鞍的稳定流形碰撞产生.第一种瞬态边界激变导致吸引域突然变小,吸引域边界突然变大;第二种瞬态边界激变使两个不同的吸引域边界合并成一体.此外,在瞬态合并激变中两个混沌鞍发生合并,最后系统的混沌瞬态在内部激变中消失.这些广义激变现象对混沌瞬态的研究具有重要意义.
文摘利用广义胞映射方法,研究了加性和乘性泊松白噪声联合作用下SD振子(smooth and discontinuous oscillator)的随机响应问题.基于图分析算法,获得确定SD振子的吸引子、吸引域、域边界、鞍和不变流形等全局特性.基于矩阵分析算法,计算了SD振子在泊松白噪声激励下的瞬态和稳态响应.结果表明:随机响应的概率密度函数演化方向和确定情况下的不稳定流形形状之间存在密切联系.蒙特卡罗模拟结果表明,所使用的方法是有效且准确的.
基金supported by the National Natural Science Foundation of China (Grant No.10872165)
文摘Crisis and stochastic bifurcation of the hardening Helmholtz-Duffing oscillator are studied by means of the generalized cell mapping method using digraph.For the system subject to a single deterministic harmonic excitation,our study reveals that a series of crisis phenomena can occur when the system parameter passes through different critical values,including chaotic boundary crisis,regular boundary crisis and interior crisis.A chaotic boundary crisis due to the collision of regular attractor with chaotic saddle embedded in a fractal basin boundary and an interior crisis due to the collision of regular attractor with chaotic saddle of its attraction basin are discovered.A new phenomenon,namely the global properties of dynamical system show symmetric as system parameter is varied,can be also revealed according to our analysis.For the system subject to a combination of a deterministic harmonic excitation and a random excitation,it is found that stochastic bifurcation,defined as a sudden change in character of a stochastic attractor,can occur one after another when the noise intensity passes through different critical values.This kind of stochastic bifurcation corresponds to stochastic crisis essentially.Our study also reveals that the generalized cell mapping method using digraph is a powerful tool not only for the crisis behavior analysis of deterministic system,but also for the global property analysis of stochastic bifurcation.
基金supported by the National Natural Science Foundation of China (Grant Nos.10932009 and 11172233)the Natural Science Foundation of Shaanxi Province (Grant No.2012JQ1004)the Northwestern Polytechnical University Foundation for Fundamental Research (Grant Nos.JC201266 and JC20110228)
文摘Stochastic bifurcations of the SD （smooth and discontinuous） oscillator with additive and/or multiplicative bounded noises are studied by the generalized cell mapping method using digraph analysis algorithm. From the global viewpoint, stochastic bifur- cation can be described as a sudden change in shape and size of a random attractor as the system parameter valies. The evolu- tionary process of stochastic bifurcation in the SD oscillator is shown in detail. Meanwhile, we show the phenomenon that un- der stochastic excitation the shape and size of random attractor and random saddle change along with the direction of unstable manifold. A plane stochastic bifurcation diagram is included.
