任意激励关系下非保守耦合振子能量分布与功率流的一般特征

传统的统计能量分析(SEA)理论不能解决非保守耦合系统和保守或非保守耦合系统在相关输入时的能量分析问题。作为任意输入关系下非保守耦合系统统计能量分析的基础,本文研究了耦合振子在非保守耦合及任意输入条件下能量分布与功率流的一般特征,推导了功率平衡方程式及各有关功率项的计算式,讨论了振子间功率流的构成及各向功率流之间的关系。研究结果表明,耦合阻尼和输入形式对耦合振子能量平衡和功率总体特征有着显著的影响。     

柱体流激振动能量俘获理论与技术研究若干进展

潮流能分布广泛,且储量巨大,具备巨大的规模化开发利用价值.流激振动是一种常见的流固耦合现象,通过柱体流激振动能够在流速较低时实现有效的能量转换,基于柱体流激振动的能量俘获技术在未来具备广阔的工程应用前景.近年来,针对柱体结构流激振动特性和能量俘获性能,出现了大量的实验和数值仿真研究工作.文章全面阐述了多种截面形式的单个柱体、柱群结构流激振动能量俘获理论与技术方面的研究进展:对于单个圆柱流激振动能量俘获,目前已基本揭示了被动湍流控制器参数、系统阻尼、雷诺数和边界条件等因素对能量俘获性能的影响规律,基本完成了理论和技术积累;对于非圆截面柱体流激振动能量俘获,已初步明确特定来流攻角、系统质量比、系统阻尼、系统刚度和雷诺数条件下三角形、四边形、多边形与异形等多种截面形式柱体的流激振动作用机理和能量俘获能力;对于柱群的流激振动能量俘获,各柱体振子之间存在流场干涉,需要合理设计柱体排布形式、柱体间距和系统阻尼等参数,实现流体能量俘获最大化.通过综述国内外流激振动能量俘获理论和技术方面的研究进展,对今后该问题的研究进行了力所能及的展望,期望促进流激振动能量俘获理论的发展和流激振动能量转换装置的工程应...     

高频宽带随机激励下的结构减振

本文运用能量观点,利用统计能量分析法的基本结论,对受高频宽带随机激励的结构,按不同要求,提出了两种不同的振动控制理论。从理论上阐明了结构的高频宽带随机振动水平与输入功率、结构的损耗因子、耦合损耗因子等的关系;得出了合理控制输入功率的大小、作用部位及损耗因子的大小、分配方式可降低结构振动的结论;发现了根据各分系统单个模态平均储存能量及损耗因子的大小,合理改变各分系统间的耦合损耗因子可控制结构振动的一般规律;给出了几种不同的结构减振措施;提出了不同于常规隔振式高频宽带结构减振。实验表明,上述分析及结论是正确的。     

T形截面振子的流致振动特性试验研究

近年来人们将流致振动(FIV)作为一种新的能源利用手段,针对圆柱型振子开展了较多的研究。随着研究的深入,发现异型截面振子因振动特性不同于圆柱型振子而具有更好的能量汲取特性。本文利用自循环水槽进行T形截面振子流致振动特性试验研究,对比研究T形振子与圆柱振子的流致振动响应差异,分析其能量捕获能力的优劣及适用范围,以期揭示阻尼比对T形振子的振动特性的影响。结果表明:不同于圆形截面振子,T形截面振子的振动表现为"非自限制"特性,出现驰振分支;增大阻尼会抑制T形截面振子的振动与驰振发生的可能性;相对于圆柱型振子而言,T形振子更适用于大流速下的能量汲取。     

圆柱体振子纵径耦合振动频率的理论计算

振子的实际振动都是不同振动模式之间的耦合振动,薄板径向振动理论、变幅杆一维设计理论等都是三维弹性理论的简化形式,都有相应的适用范围,否则将产生大的计算误差。通过设定纵径耦合系数,由弹性动力学理论推导出了圆柱体振子纵径耦合振动的频率方程,并通过与有限元分析结果及实验测量值的比较,证明了该方法具有非常高的计算精度。在圆柱体振子的纵径耦合振动中,其长径比(或厚径比)越大,振子的纵向振动越强,反之振子的径向振动越强。     

相关激励下的统计能量分析法研究

传统的统计能量分析法的基本公式是在相互独立的激励下获得的.本文从相关激励下的功率流分析入手,引入相关功率流的概念,得出相关激励下保守耦合系统功率流的表达式,给出了结构在相关激励下的统计能量关系式,数值计算表明,文中分析及结论是正确的.     

欧拉-伯努利梁运动场的正交性及其能量传导特性分析

从无阻尼欧拉—伯努利梁振动方程解析解出发, 推导了有限长梁的关于谱系数的时间—空间平均能量和功率流表达式. 在此基础上, 从泛函分析观点, 探讨了弯曲运动场: 衰减振动、行波模式分解关于能量、功率泛函的正交性. 结果表明: 弯曲衰减振动模式和行波模式关于功率流、机械能时间—空间平均是相互独立的, 即关于场能和场功率互不干涉, 满足叠加原理; 衰减振动场导能与行波场导能的重要区别在于功率流关于右、左衰振动模式分解不满足叠加原理, 即弯曲衰减振动场间的相互"干涉"是使其具有能量传导能力的内在原因. 通过右端集中阻尼器支撑的梁的稳态功率流仿真分析计算, 表明低频区振动导能不可忽略, 同时, 衰减振动场和行波场间存在一定的能量交换现象, 但随着频率升高, 振动场传导能量不断下降, 同时能量传导效率也不断下降.      

套管-水泥浆系统流固耦合振动特性研究

已有文献在计算振动固井套管固有振动特性时,未充分考虑水泥浆和套管流固耦合的影响,难以准确地得出套管在水泥浆条件下的振动特性。本文进一步考虑了套管和水泥浆的耦合振动特性,基于Euler-Bernoulli梁柱理论及Hamilton变分原理推导了套管与水泥浆耦合振动控制方程,采用有限元方法计算了套管在水泥浆条件下的振动特性,综合分析了管内压力、水泥浆密度、套管长度、水泥浆阻尼等因素对耦合系统横向振动固有频率的影响。结果表明:套管-水泥浆系统的耦合特性不可忽略,随着水泥浆密度的增加,套管横向振动的固有频率降低;套管内流体压力、水泥浆的粘性阻尼和科氏阻尼对耦合系统的横向振动固有频率影响较小,可以忽略不计;随着套管长度的增加,套管横向振动固有频率减小。研究结果可为振动发生器的优化设计提供理论基础。     

高斯色噪声和谐波激励共同作用下耦合SD振子的混沌研究

耦合SD振子作为一种典型的负刚度振子, 在工程设计中有广泛应用. 同时高斯色噪声广泛存在于外界环境中, 并可能诱发系统产生复杂的非线性动力学行为, 因此其随机动力学是非线性动力学研究的热点和难点问题. 本文研究了高斯色噪声和谐波激励共同作用下双稳态耦合SD振子的混沌动力学, 由于耦合SD振子的刚度项为超越函数形式, 无法直接给出系统同宿轨道的解析表达式, 给混沌阈值的分析造成了很大的困难. 为此, 本文首先采用分段线性近似拟合该振子的刚度项, 发展了高斯色噪声和谐波激励共同作用下的非光滑系统的随机梅尔尼科夫方法. 其次, 基于随机梅尔尼科夫过程, 利用均方准则和相流函数理论分别得到了弱噪声和强噪声情况下该振子混沌阈值的解析表达式, 讨论了噪声强度对混沌动力学的影响. 研究结果表明, 随着噪声强度的增大混沌区域增大, 即增大噪声强度更容易诱发耦合SD振子产生混沌. 当阻尼一定时, 弱噪声情况下混沌阈值随噪声强度的增加而减小; 但是强噪声情况下噪声强度对混沌阈值的影响正好相反. 最后, 数值结果表明, 利用文中的方法研究高斯色噪声和谐波激励共同作用下耦合SD振子的混沌是有效的.本文的结果为随机非光滑系统的混沌动力学研究提供了一定的理论指导.      

圆柱涡激振动的结构-尾流振子耦合模型研究

建立了一个新的结构-尾流振子耦合模型. 流场近尾迹动力学特征被模化为非线性阻尼振子,采用van der Pol方程描述. 以控制体中结构与近尾迹流体间受力互为反作用关系来实现流固耦合. 采用该模型进行了二维结构涡激振动计算,得到了合理的振幅随来流流速的变化规律和共振幅值,并正确地预计了共振振幅值$A_{\max}^\ast$随着质量阻尼参数$\left( {m^\ast + C_A } \right)\zeta$的变化规律,给出了预测$A_{\max }^\ast$值的拟合公式. 采用该模型计算了三维柔性结构在均匀来流和简谐波形来流作用下的VIV响应. 结构在均匀来流作用下振动呈现由驻波向行波的变化过程, 并最后稳定为行波振动形态.在简谐波形来流作用下,结构呈现混合振动形态,幅值随时间呈周期变化.      

相关激励下的统计能量分析法（SEA）研究

目前相关激励下的统计能量关系实质是在比例相关或互谱密度为实数的相关激励下获得的，从分析普通相关激励下的功率流入手、给出相关激励下保守耦合系统及非保守耦合系统统计能量关系的普遍形式，实例表明：文中的分析和结论是正确的。     

Nonlinear dynamics of two harmonic oscillators coupled by Rayleigh type self-exciting force

The present paper reports some interesting phenomena observed in the nonlinear dynamics of two self-excitedly coupled harmonic oscillators. The system under consideration consists of two mechanical oscillators coupled by the Rayleigh type self-exciting force. Both autonomous and nonautonomous cases for weakly coupled systems are analyzed. When the natural frequencies of the two oscillators are close to each other, only one mode of oscillation exists. As two modes of oscillations get locked to a single mode, the system is said to be in a mode-locked condition. Under a mode-locked condition, the oscillators can oscillate with only a single frequency. However, when two oscillators are sufficiently detuned, the mode-locking condition does not persist and two distinct modes of oscillations emerge. Under these circumstances, particularly when detuning is large, one of the oscillators, depending on the initial conditions, oscillates with much larger amplitude as compared to the other oscillator, and hence mode localization is observed. When one of the oscillators is subject to a harmonic excitation, at two different frequencies, termed here as the decoupling frequencies, the coupling between the oscillators is almost lost, resulting in almost zero response of the unexcited oscillator. Analytical and numerical results are presented to analyze the above mentioned phenomena. Some potential applications of the aforesaid phenomena are also discussed.     

Heteroclinic motion and energy transfer in coupled oscillator with nonlinear magnetic coupling

In this paper, we consider two coupled oscillators exhibiting both transient chaos and energy transfer from mechanical to electrical oscillators. Melnikov method is applied to these oscillators with linear damping and strongly nonlinear coupling terms in order to study the possibility of existence of chaos and transversal heteroclinic orbits and their control in a dynamical system. The energy transfer is studied using a qualitative measure of the system which can be obtained by computing the energy dissipated in it. At last, the numerical simulation is carried out for this system.     

Investigation on a coupled Navier–Stokes–Direct Simulation Monte Carlo method for the simulation of plume flowfield of a conical nozzle

To assess the plume effects of space thrusters, the accurate plume flowfield is indispensable. The plume flow of thrusters involves both continuum and rarefied flow regimes. Coupled Navier–Stokes–Direct Simulation Monte Carlo (NS–DSMC) method is a major approach to the simulation of continuum‐rarefied flows. An axisymmetric coupled NS–DSMC solver, possessing adaptive‐interface and two‐way coupling features, is investigated in this paper for the simulation of the nozzle and plume flows of thrusters. The state‐based coupling scheme is adopted, and the gradient local Knudsen number is used to indicate the breakdown of continuum solver. The nitrogen flows in a conical nozzle and its plume are chosen as the reference case to test the coupled solver. The threshold value of the continuum breakdown parameter is studied based on both theoretical kinetic velocity sampling and coupled numerical tests. Succeeding comparisons between coupled and full DSMC results demonstrate their conformities, meanwhile, the former saves 58.8% computational time. The pitot pressure evaluated from the coupled simulation result is compared with the experimental data proposed in literatures, revealing that the coupled method makes precise predictions on the experimental pitot pressure. Copyright © 2014 John Wiley & Sons, Ltd.     

Contraction theory based synchronization analysis of impulsively coupled oscillators

Impulsively coupled oscillators which are assumed to interact with each other only at discrete times have many applications in practice. In this paper, we introduce the concept of partial contraction theory of impulsive systems, which is used to investigate the synchronization problem of impulsively coupled oscillators. Contraction analysis of two impulsively coupled oscillators and networked impulsively coupled oscillators is provided, respectively. Very simple but very general results for synchronization of impulsively coupled oscillators are derived. Numerical simulations show the effectiveness of our theoretical results.     

Regular oscillations,chaos, and multistability in a system of two coupled van der Pol oscillators: numerical and experimental studies

In this paper, the dynamics of a system of two coupled van der Pol oscillators is investigated. The coupling between the two oscillators consists of adding to each one’s amplitude a perturbation proportional to the other one. The coupling between two laser oscillators and the coupling between two vacuum tube oscillators are examples of physical/experimental systems related to the model considered in this paper. The stability of fixed points and the symmetries of the model equations are discussed. The bifurcations structures of the system are analyzed with particular attention on the effects of frequency detuning between the two oscillators. It is found that the system exhibits a variety of bifurcations including symmetry breaking, period doubling, and crises when monitoring the frequency detuning parameter in tiny steps. The multistability property of the system for special sets of its parameters is also analyzed. An experimental study of the coupled system is carried out in this work. An appropriate electronic simulator is proposed for the investigations of the dynamic behavior of the system. Correspondences are established between the coefficients of the system model and the components of the electronic circuit. A comparison of experimental and numerical results yields a very good agreement.     

Effects of gradient coupling on amplitude death in nonidentical oscillators

The effects of the gradient coupling on the amplitude death in an array and a ring of diffusively coupled nonidentical oscillators are explored, respectively. The gradient coupling plays a significant role on the amplitude death dynamics, however, it is strongly related to the boundary conditions of the coupled system. With the increment of the gradient coupling, the domain of the amplitude death is monotonically enlarged in an array of coupled oscillators. However, for a ring of coupled oscillators, it is firstly enlarged and then decreased as the gradient coupling increases. The domain of the amplitude death in parameter space is analytically predicted for a small number of gradiently coupled oscillators.     

Stable amplitude chimera states and chimera death in repulsively coupled chaotic oscillators

Amplitude chimera states, representing a spontaneous symmetry breaking of a population of coupled identical oscillators into two distinct clusters with one oscillating in spatial coherent amplitude, while the other displaying oscillations in a spatially incoherent manner, have been observed as a kind of transient dynamics in the process of transition to the in-phase synchronization in coupled limit-cycle oscillators. Here, we obtain a kind of stable amplitude chimera state in the chaotic regime of a system of repulsively coupled Lorenz oscillators. With the increment of the coupling strength, the coupled oscillators transit from spatiotemporal chaos to amplitude chimera states then to coherent oscillation death or chimera death states. Moreover, the number of clusters in amplitude chimera patterns has a power-law dependence on the number of coupled neighbors. The amplitude chimera and the chimera death states coexist at certain coupling strength. Moreover, the amplitude chimera and the amplitude death patterns are related to the initial condition for given coupling strength. Our findings of amplitude chimera states and chimera death states in coupled chaotic system may enrich the knowledge of the symmetry-breaking-induced pattern formation.     

Dynamical Order in Systems of Coupled Noisy Oscillators

We investigate a dynamical order induced by coupling and/or noise in systems of coupled oscillators. The dynamical order is referred to a one-dimensional topological structure of the global attractor of the system in the context of random skew-product flows. We show that if the coupling is sufficiently strong, then the system exhibits one dimensional dynamics regardless of the strength of noise. If the coupling is weak, then it is shown numerically that the system also exhibits one dimensional dynamics provided the noise is sufficiently strong. We also show that for any coupling and any noise, the system has a unique rotation number and hence all the oscillators tend to oscillate with the same frequency eventually (frequency locking). Dedicated to Professor Pavol Brunovsky on the occasion of his 70th birthday.