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1.
悬索是一种典型的大跨度低阻尼柔性系统,其包含平方和立方非线性特征,从而呈现出各种非线性动力学行为,尤其是在不同模态之间发生的耦合共振响应。此外实际工程中悬索受气温、太阳辐射、风等因素影响,周围温度场变化明显,而悬索线性和非线性振动特性对于温度变化较为敏感。本研究以悬索同时发生主共振和3∶1内共振为例,将之前忽略模态耦合的单自由度模型扩展到两自由度模型,并利用多尺度法求得系统直角坐标下的平均方程。基于所绘制的系统各类响应曲线,对温度变化下悬索模态耦合振动特性开展详细论述。数值算例结果表明:温度下降(上升)时,Irvine参数更大(更小)的悬索容易发生3∶1内共振;在内共振的区间,低阶模态响应幅值受温度变化的影响大于高阶模态的响应幅值;霍普夫分岔对于温度变化的敏感程度要高于鞍结点分岔;在耦合共振区间,系统周期运动对温度变化较为敏感,温度变化有可能导致系统的周期运动变为非周期。  相似文献   

2.
主要研究侧向风载荷作用下小垂度覆冰悬索的非线性非平面运动的复杂动力学. 根据分析力学、弹性力学和空气动力学理论, 建立覆冰悬索3个自由度非线性振动的偏微分运动方程,并对其进行无量纲化,运用Galerkin方法对偏微分运动方程进行离散得到3个自由度的常微分方程,再利用多尺度法得到面内主共振2:1内共振的平均方程. 利用数值方法研究悬索的非线性运动,结果表明系统呈现周期、多倍周期、概周期和混沌运动的规律.  相似文献   

3.
悬索在考虑1:3内共振情况下的动力学行为   总被引:2,自引:0,他引:2  
研究了悬索在受到外激励作用下考虑1:3内共振情况下的两模态非线性响应.对于一定范围内悬索的弹性-几何参数而言,悬索的第三阶面内对称模态的固有频率接近于第一阶面内对称模态固有频率的三倍,从而导致1:3内共振的存在.首先利用Galerkin方法把悬索的面内运动方程进行离散,然后利用多尺度法对离散的运动方程进行摄动得到主共振情况下的平均方程.接下来对平均方程的稳态解、周期解以及混沌解进行了研究.最后利用Runge-Kutta法研究了悬索两自由度离散模型的非线性响应.  相似文献   

4.
轴向运动梁非线性振动内共振研究   总被引:19,自引:2,他引:19  
采用多元L-P方法分析轴向运动梁横向非线性振动的内共振,首先根据哈密顿原理建立轴向运动梁的横向振动微分方程,然后利用Galerkin方法分离时间和空间变量,再采用多元L-P方法进行求解,推导了内共振条件下频率-振幅方程的求根判别式,理论分析发现内共振与强迫力的振幅有关,而且可以从理论上决定这一界乎不同内共振的强迫力振幅的临界值,典型算例获得了轴向运动梁横向非线性振动内共振复杂的频率一振幅响应曲线,揭示了很多复杂而有趣的非线性振动特有的现象,多元L-P方法的数值结果,在小振幅时与IHB法的结果一致。  相似文献   

5.
本文利用非线性时空有限方法和样条有限元技术对具有初内力的板的非线性频响特性进行了分析,计算了在不同初始内力下方板的大振幅自由振动、有阻尼强迫振动和矩形板的内共振。  相似文献   

6.
损伤是结构振动测试和运营维护中不可避免的问题,损伤效应会导致结构振动特性发生改变.本文以受损悬索为例,探究该非线性系统同时发生主共振和2:1内共振时,损伤效应对其面内耦合共振响应影响.首先基于哈密顿变分原理,引入与损伤程度、范围和位置相关的三个无量纲参数,建立受损悬索面内动力学模型,并推导其无穷维非线性运动微分方程.以2:1耦合共振为例,采用Galerkin法和多尺度法得到系统直角坐标形式的调谐方程.数值算例表明:损伤会导致悬索固有频率降低,使得频率间公倍关系发生改变,影响系统耦合共振响应;损伤会引发系统振动特性发生明显定量和定性改变,尤其是共振响应幅值及弹簧特性;损伤对直接激励模态响应幅值的影响比对内共振激发对响应幅值的影响要明显;损伤会导致霍普夫、鞍节点、叉形和倍周期分岔的位置发生偏移,从而影响分岔点附近系统的动力学行为;系统动态解和周期运动与损伤密切相关,损伤会导致系统展现出完全不同类型的吸引子.  相似文献   

7.
弹性体非线性振动多重共振的能量法   总被引:10,自引:1,他引:10  
邱家俊 《力学学报》1990,22(6):753-758
本论文以非线性振动理论的平均法为基础和力学的能量概念结合起来,找到了求解弹性体系非线性振动多重共振的能量法。应用本方法研究了电机轴系的双重共振等问题,证明了它是一个简易适用的方法。揭示了双重共振的一些新现象,理论得到了实验验证。  相似文献   

8.
研究了悬索在受到外激励作用和考虑1∶3内共振情况下的两模态非线性响应.对于一定范围内的悬索弹性-几何参数而言,悬索第三阶面内对称模态的固有频率接近于第一阶面内对称模态的固有频率的3倍,从而导致1∶3内共振的存在.首先利用Galerkin方法把悬索的面内运动方程进行离散,然后利用多尺度法对离散的运动方程进行摄动,可得到两组不同主共振情况下的平均方程.  相似文献   

9.
研究了悬索在受到外激励作用和考虑1∶3内共振情况下的两模态非线性响应。对于一定范围内的悬索弹性-几何参数而言,悬索第三阶面内对称模态的固有频率接近于第一阶面内对称模态的固有频率的3倍,从而导致1∶3内共振的存在。首先利用Galerkin方法把悬索的面内运动方程进行离散,然后利用多尺度法对离散的运动方程进行摄动,可得到两组不同主共振情况下的平均方程。  相似文献   

10.
非线性振子的主共振——基本参数共振   总被引:1,自引:0,他引:1  
在本文里我们用多尺度法和数值方法研究了非一性振动系统在主共振--基本参数共振时的分岔响应,得所结果说明在这个系统里存在着主共振与基本参数共振之间的相互作用。  相似文献   

11.
Chang  W. K.  Ibrahim  R. A. 《Nonlinear dynamics》1997,12(3):275-303
The random excitation of a suspended cable with simultaneous internal resonances is considered. The internal resonances can take place among the first in-plane and the first two out-of-plane modes. The external loading is represented by a wide-band random process. The response statistics are estimated using the Fokker-Planck-Kolmogorov (FPK) equation, together with Gaussian and non-Gaussian closures. Monte Carlo simulation is also used for numerical verification. The unimodal in-plane motion exists in regions away from the internal resonance condition. The mixed mode interaction is manifested within a limited range of internal detuning parameters, depending on the excitation power spectrum density and damping ratios. The Gaussian closure scheme failed to predict bounded solutions of mixed mode interaction. The non-Gaussian closure results are in good agreement with the Monte Carlo simulation. The on-off intermittency of the autoparametrically excited modes is observed in the Monte Carlo simulation over a small range of excitation levels. The influence of the cable parameters, such as damping ratios, sag-to-span ratio, internal detuning parameters, and excitation level on the autoparametric interaction, is studied. It is found that the internal detuning and excitation level are the two main parameters which affect the autoparametric interaction among the three modes. Due to the system's nonlinearity, the response of the three modes is strongly non-Gaussian and the coupled modes experience irregular modulation.  相似文献   

12.
In this paper, the along-wind and across-wind responses of suspended cables are studied. The mean wind direction is assumed to be perpendicular to the plane of the suspended cable. It is shown that the cable gallops in the across-wind direction, when the mean wind speed exceeds a critical wind speed. To control the galloping response, a vertical viscous damper, in the vertical plane of the cable, is introduced at a certain location on the cable to a near fixed platform such as a bridge deck. The efficiency of the vertical viscous damper and its location in controlling the galloping of the suspended cable is investigated.  相似文献   

13.
14.
Fluid Flow-Induced Nonlinear Vibration of Suspended Cables   总被引:2,自引:0,他引:2  
Chang  W. K.  Pilipchuk  V.  Ibrahim  R. A. 《Nonlinear dynamics》1997,14(4):377-406
The nonlinear interaction of the first two in-plane modes of a suspended cable with a moving fluid along the plane of the cable is studied. The governing equations of motion for two-mode interaction are derived on the basis of a general continuum model. The interaction causes the modal differential equations of the cable to be non-self-adjoint. As the flow speed increases above a certain critical value, the cable experiences oscillatory motion similar to the flutter of aeroelastic structures. A co-ordinate transformation in terms of the transverse and stretching motions of the cable is introduced to reduce the two nonlinearly coupled differential equations into a linear ordinary differential equation governing the stretching motion, and a strongly nonlinear differential equation for the transverse motion. For small values of the gravity-to-stiffness ratio the dynamics of the cable is examined using a two-time-scale approach. Numerical integration of the modal equations shows that the cable experiences stretching oscillations only when the flow speed exceeds a certain level. Above this level both stretching and transverse motions take place. The influences of system parameters such as gravity-to-stiffness ratio and density ratio on the response characteristics are also reported.  相似文献   

15.
Zheng  G.  Ko  J. M.  Ni  Y. Q. 《Nonlinear dynamics》2002,30(1):55-70
In this paper, super-harmonic and internal resonance characteristics ofa viscously damped cable with nearly commensurable natural frequenciesare investigated by use of a novel method. The proposed frequency-domainsolution method is based on the combined use of a three-dimensionalnonlinear finite element approach and the incremental harmonic balancetechnique. It is an accurate algorithm in the sense that it accommodatesmulti-harmonic components and no mode-based model reduction is utilizedin the solution process. The alternating frequency/amplitude-controlledalgorithm enables complete solution to the frequency-response curvesincluding unstable branches, sub- and super-harmonic resonance andinternal resonance. A suspended cable paradigm under internal resonancecondition is studied using the proposed method. Nonlinear response andmodal interaction characteristics of the cable at different frequencyregions are identified from analysis of response profiles and harmoniccomponent features. The super-harmonic and internal resonance responsesare respectively characterized based on the harmonic distribution. Underan in-plane harmonic excitation, the two-to-one internal resonancebetween the in-plane and out-of-plane modes and the super-harmonicresonance around the second symmetric in-plane mode are revealed. Strongnonlinear interaction among different modes in the parameter spaceranging from primary resonance to super-harmonic resonance is observed.  相似文献   

16.
Ockendon  H.  Ockendon  J.R. 《Meccanica》2001,36(3):297-321
This paper reviews the simplest mathematical theories that have been advanced to describe the effects of nonlinearity on fluid resonance in two paradigm situations, namely gas oscillating in a container and water sloshing in a tank. These configurations illustrate what can happen when nonlinearity competes with geometrical asymmetry, dispersion or various kinds of damping in limiting the resonant response. In all situations the qualitative form of the response depends crucially on whether or not the natural frequencies of the system are rationally related to each other. Sommario. Questo lavoro passa in rassegna le più semplici teorie matematiche disponibili per la descrizione degli effetti delle nonlinearità sulla risonanza dei fluidi in due situazioni paradigmatiche, un gas oscillante in un recipiente e l'acqua oscillante in una vasca. Queste configurazioni illustrano le situazioni che possono verificarsi quando le nonlinearità competono con l'asimmetrica geometrica, la dispersione o diversi tipi di smorzamento, nel limitare la risposta risonante. In tutte le situazioni, gli aspetti qualitativi della risposta dipendono in modo cruciale dall'esistenza o meno di rapporti razionali fra le frequenze naturali del sistema.  相似文献   

17.
Three-to-One Internal Resonances in Hinged-Clamped Beams   总被引:7,自引:0,他引:7  
Chin  Char-Ming  Nayfeh  Ali H. 《Nonlinear dynamics》1997,12(2):129-154
The nonlinear planar response of a hinged-clamped beam to a primary excitation of either its first mode or its second mode is investigated. The analysis accounts for mid-plane stretching, a static axial load and a restraining spring at one end, and modal damping. For a range of axial loads, the second natural frequency is approximately three times the first natural frequency and hence the first and second modes may interact due to a three-to-one internal resonance. The method of multiple scales is used to attack directly the governing nonlinear partial-differential equation and derive two sets of four first-order nonlinear ordinary-differential equations describing the modulation of the amplitudes and phases of the first two modes in the case of primary resonance of either the first or the second mode. Periodic motions and periodically and chaotically modulated motions of the beam are determined by investigating the equilibrium and dynamic solutions of the modulation equations. For the case of primary resonance of the first mode, only two-mode solutions are possible, whereas for the case of primary resonance of the second mode, single- and two-mode solutions are possible. The two-mode equilibrium solutions of the modulation equations may undergo a supercritical or a subcritical Hopf bifurcation, depending on the magnitude of the axial load. A shooting technique is used to calculate limit cycles of the modulation equations and Floquet theory is used to ascertain their stability. The limit cycles correspond to periodically modulated motions of the beam. The limit cycles are found to undergo cyclic-fold bifurcations and period-doubling bifurcations, leading to chaos. The chaotic attractors may undergo boundary crises, resulting in the destruction of the chaotic attractors and their basins of attraction.  相似文献   

18.
Nonlinear modal interactions in the forced vibrations of a thermally loaded pre-buckled annular plate with clamped–clamped immovable boundary conditions are investigated. The mechanism responsible for the interaction is a combination internal resonance involving the natural frequencies of the three lowest axisymmetric modes. The in-plane thermal load acting on the plate is assumed to be axisymmetric and the plate is externally excited by a harmonic force. The nonlinear von Kármán plate equations along with the heat conduction equation are combined to model the behavior of the system. An analytical/numerical approach is used to examine the plate vibrations to a harmonic excitation near primary resonance of one of the modes.  相似文献   

19.
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