多自由度Maxwell阻尼器减震结构(Ⅰ)——随机响应特性

对多自由度带支撑Maxwell粘滞阻尼器减震结构的随机响应特性进行了系统研究。建立了结构一般运动方程;将运动方程按原结构振型展开,将运动方程化为振型广义坐标的微分和积分混合地震响应方程组;基于多自由度随机平均法理论,获得了结构随机平均It方程组的解析式,推导出耗能结构各振型振子的振幅与相位瞬态联合概率密度函数、位移与速度瞬态联合概率密度函数、位移与速度瞬态响应方差的一般解析解;根据SRSS组合方法,给出了耗能结构随机地震响应方差的一般解析式,从而建立了此类耗能结构随机响应特性分析的完备解析解法。     

风向角对超高层建筑横风向效应的影响

随着建筑高度的增加,结构自振周期延长,抗侧刚度相对变小,风荷载效应增大。本文以200m高的高层建筑为研究对象,基于风洞试验所得的横风向风压时程数据对其结构进行了计算。试验模型缩尺比为1／400。试验取风向角从0°到45°,每级风向角增量为5°,模拟了两种地面粗糙度。对试验数据进行了迎风面和背风面气动效应的分析。考虑结构第一模态振型发生的位移,由振型分解法按Duhamel积分获得了结构顶点位移和顶点加速度,探讨了结构响应最大值和标准差与风向角、结构自振基频、地面粗糙度等因素的关系。研究表明：风荷载效应与风向角有密切的联系,结构最大响应一般发生在0°。     

环境随机激励下斜拉桥的模态分析

文章首先给出了利用环境随机激励实际工程结构输出响应自功率谱间接识别柔性结构模态参数的方法,并运用它对一斜拉桥现场测试结果进行了分析。然后建立了三维有限单元模型,得到了该桥自振频率和振型的理论值。脉动实验测得的结构自振频率和振型与用三维有限单元模型得到的理论值的对比发现,绝大部分模态吻合得较好,特别是竖向振型     

多点激励反应谱法的理论研究

基于虚拟激励原理建立了多点激励反应谱法。该方法所表示的结构地震动反应由三部分组成,即拟静力响应、动力响应及二者的耦合响应,其中拟静力响应是由地面各点输入位移不一致引起的;动力响应主要是由结构在地面加速度作用下引起的;当结构自振周期小于2s时,拟静力响应与动力响应之间的耦合项可以忽略。该方法计算公式形式简洁,物理意义明确,且与我国现行《抗震规范》中的一致激励反应谱建立了定量关系。在推导过程中,未做任何特殊简化,因而该方法在理论上是严密的。     

具有动应力和动位移约束的离散变量结构形状优化设计方法

讨论了动应力、动位移约束下离散变量状优化设计问题。首先用拟静力算法,将结构惯性力极值作为静载荷施加到结构上,求得结构的动位移和动内力,然后将考虑动应力约束和动作移约束的离散变量结构优化设计问题化为静应力和静位移约束的优化问题。在求解过程中,将单元内力作了一阶近似,并将多约束问题转化为单约束问题,然后利用两类变量统一考虑的离散变量结构形状优化设计的综合算法进行求解。     

土壤——多层结构相互作用体系地震位移响应的近似计算

土壤——多层结构相互作用体系地震位移响应基本上是由第一振型控制的,只要知道了体系的基本周期T_1及第一振型阻尼比D_1,即可由地震记录的位移反应谱求出该体系地震位移响应的近似值。因此,对相互作用体系的基频及第一振型阻尼比进行近似计算有着重要的工程意义。 关于基础有埋深的土壤——结构相互作用体系基频及第一振型阻尼比,Bielak曾经作过     

用振型分析法求响应时初始条件的变换

一个n自由度的系统受外力激励产生振动时,其响应往往以低频振动为主,高阶振动的分量只占次要地位.对实际工程结构来说,由于阻尼的作用,高频振动不但振幅小,而且衰减也快,因此可以略去不计.针对这种情况采用振型分析法来求响应是很有利的,此时只需先求出在响应中占主要地位的前s 阶固有频率和振型,再算出前s 阶振动在响应中各自所占的分量即可.因为s<相似文献   

随机振动问题的广义坐标合成法

工程中的随机振动分析多采用完全二次型组合法(CQC)及其改进算法,如虚拟激励法(PEM)和谐波激励法(HEM)。广义坐标合成法(GCS)提出了一种计算随机响应的新思路,其基本原理是将物理空间的计算转移到自由度较小的振型空间进行,从而缩减了计算量和计算规模。对于较大规模结构体系的随机振动问题,GCS方法计算响应协方差矩阵的计算量只相当于PEM的2r/sT,其中s、r和T分别为激励功率谱矩阵的秩、振型总数和离散频率点数。此外,对于给定激励时程的问题,由于GCS方法直接求解广义坐标运动方程,因而可以方便得出响应时程。通过对几种方法的详细对比,说明对于大多数只需要求解响应方差的随机振动问题,GCS是最优的计算方法。PEM只有在s相似文献   

平稳/非平稳激励下中厚圆柱壳随机振动响应的基准解

圆柱壳结构被广泛应用于航空航天、船舶、汽车工程等领域.由于服役环境复杂,圆柱壳会受到随机激励作用,从而产生随机振动响应.本文针对考虑横向剪切变形和转动惯量的中厚圆柱壳,将虚拟激励法拓展到连续体结构,高效获得了各类随机激励下响应均方根的基准解.首先,开展了简支条件下中厚圆柱壳的自由振动分析,精确求得各阶自振频率和解析振型...     

基础埋置深度对土壤——多层结构动力相互作用的影响

本文利用Baranov-Novak关于埋置基础水平与摆动耦合振动的结果及Veletsos与Verbic关于粘弹性地基振动的结果,给出了与埋置基础等效的无埋置基础的动力刚度系数及阻尼系数,并以钢筋混凝土框架结构为例来说明基础埋置深度对土壤——多层结构动力相互作用的影响。计算结果表明,结构体系第一振型的弹性位移及阻尼比并不总是随埋深比的增加而单调变化;在一定的范围内,结构体系基础有埋深时的基频与无埋深时的基频之比与埋深比之间有着近似的线性关系;结构体系的地震位移响应基本上是由第一振型控制的。     

Comparison of near- and far-fault ground motion effect on the nonlinear response of dam–reservoir–foundation systems

In this paper, it is aimed to compare the near- and far-fault ground motion effects on the nonlinear dynamic response of dams including dam–reservoir–foundation interaction. Two different types of dams, which are concrete arch and concrete faced rockfill dams, are selected to investigate the near- and far-fault ground motion effects on the dam responses. The behavior of reservoir water is taken into account using Lagrangian approach. The Drucker–Prager material model is employed in nonlinear analyses. Near and far-fault strong ground motion records, which have approximately identical peak ground accelerations, of Loma Prieta (1989) earthquake are selected for the analyses. Displacements, maximum and minimum principal stresses are determined using the finite element method. The displacements and principal stresses obtained from the analyses of dams subjected to each fault effect are compared with each other. It is clearly seen that there is more seismic demand on displacements and stresses when the dam is subjected to near-fault ground motion.     

Effects of the dynamic wheel–rail interaction on the ground vibration generated by a moving train

Based on Biot’s fully dynamic poroelastic theory, the dynamic responses of the poroelastic half-space soil medium due to quasi-static and dynamic loads from a moving train are investigated semi-analytically. The dynamic loads are assumed to be generated from the rail surface irregularities. The vehicle dynamics model is used to simulate the axle loads (quasi-static loads) and the dynamic loads from a moving train. The compatibility of the displacements at wheel–rail contact points couple the vehicle and the track–ground subsystem, and yield equations for the dynamic wheel–rail loads. A linearized Hertzian contact spring between the wheel and rail is introduced to calculate the dynamic loads. Using the Fourier transform, the governing equations for the poroelastic half-space are then solved in the frequency–wavenumber domain. The time domain responses are evaluated by the fast inverse Fourier transform. Numerical results show that the dynamic loads can make important contribution to dynamic response of the poroelastic half-space for different train speed, and the dynamically induced responses lie in a higher frequency range. The ground vibrations caused by the moving train can be intensified as the primary suspension stiffness of the vehicle increases.     

Stochastic seismic response of long-span structures

In this paper, dynamic responses of long-span structures subjected to the action of earthquake with realistic wave speed are analysed. The horizontal or vertical ground motion due to earthquakes is assumed to be a stationary stochastic process, and the seismic waves travel along a horizontal straight line. Expressions for calculating the psd(power spectral density) matrices of structural displacements and internal forces are derived based on three dimensional FEM structural models with the ground motion phase-lags taken into account. A numerical example is given which shows that it is of great importance to consider the effect of the ground motion phase-lags for long-span structures.This work was supported by the National Natural Science Foundation of China.     

Coupled rocking and sliding vibration response of a structure to harmonic horizontal ground motion

For a strip wall erected on a rigid strip foundation and supported by the surface of the ground, the dynamic soil-structure interaction under the action of the horizontal ground motion is investigated. The ground motion is idealized as vertically propagating, horizontal steady-state motion. Because the horizontal ground motion brings about the sliding vibration of the foundation as well as the rocking vibration, the coupled rocking and sliding vibration of the soil-structure system is considered in the present paper. For the contact between the ground and foundation, the following assumptions are made: 1) the contact is assumed to be welded, that is to say, the motion of the foundation is consistent with the ground; 2) the horizontal translation at each point on the bottom surface of the foundation is equal to a constant; 3) the distribution of the normal displacements under the foundation remains to be linear in the rocking vibration. For comparison, the case of uncoupled vibration is considered also. The use of Fourier transform method yields dual integral equations (for the case without coupling effect) or simultaneous dual integral equations (for the case with coupling effect). Both of them are solved by means of infinite series of orthogonal functions, the Jacobi polynomials. The numerical results show that there is a significant difference between the displacements of the foundation, the relative displacements of the top of the wall with respect to its base, and the distribution of contact stresses beneath the foundation, for the cases with and without coupling effect.     

设防烈度下非比例阻尼结构地震随机响应峰值区间估计方法

建立与抗震规范设防水准相一致的地震动随机模型,给出了非比例阻尼结构体系地震反应运动方程,推导了非比例阻尼结构体系分析的复振型时域闭合解和地震随机响应的闭合解.通过随机响应的峰值因子和变异系数获得了非比例阻尼结构体系的地震随机响应峰值均值和方差,提出了设防烈度下非比例阻尼结构体系随机响应峰值区间估计方法.计算31条实际地震记录的复振型时域闭合解,并与地震随机响应的闭合解进行了比较,算例结果表明随机响应峰值区间估计方法的合理性和有效性.地震响应区间分析方法将是工程抗震设计的一个重要方法.     

水浮力对浮桥动力响应特性的分析

为了研究水介质的浮力对桥梁静态响应、特别是动态响应的影响,了解水浮力在桥梁动力响应上的作用及其大小,利用虚功原理和振型叠加法对桥梁运动的控制方程进行求解,并编制了通用的求解程序,通过对比简支梁桥和浮桥各阶振型的传播速度、静力作用、单阶荷载作用以及移动荷载作用下的动力响应,得出水浮力的存在大大降低了浮桥的挠度,使得浮桥的动力响应存在临界长度,即简支梁桥的运动整体性强,而浮桥的运动局部性强,对浮桥进行动力分析时,可以在临界长度以内进行处理,而不必对整个桥梁进行求解.     

Thermo-mechanical nonlinear vibration analysis of a spring-mass-beam system

Thermo-mechanical vibrations of a simply supported spring-mass-beam system are investigated analytically in this paper. Taking into account the thermal effects, the nonlinear equations of motion and internal/external boundary conditions are derived through Hamilton’s principle and constitutive relations. Under quasi-static assumptions, the equations governing the longitudinal motion are transformed into functions of transverse displacements, which results in three integro-partial differential equations with coupling terms. These are solved using the direct multiple-scale method, leading to closed-form solutions for the mode functions, nonlinear natural frequencies and frequency–response curves of the system. The influence of system parameters on the linear and nonlinear natural frequencies, mode functions, and frequency–response curves is studied through numerical parametric analysis. It is shown that the vibration characteristics depend on the mid-plane stretching, intra-span spring, point mass, and temperature change.     

Quasi-static and dynamical analyses of a thermoviscoelastic Timoshenko beam using the differential quadrature method

The quasi-static and dynamic responses of a thermoviscoelastic Timoshenko beam subject to thermal loads are analyzed. First, based on the small geometric deformation assumption and Boltzmann constitutive relation, the governing equations for the beam are presented. Second, an extended differential quadrature method(DQM)in the spatial domain and a differential method in the temporal domain are combined to transform the integro-partial-differential governing equations into the ordinary differential equations. Third, the accuracy of the present discrete method is verified by elastic/viscoelastic examples, and the effects of thermal load parameters, material and geometrical parameters on the quasi-static and dynamic responses of the beam are discussed. Numerical results show that the thermal function parameter has a great effect on quasi-static and dynamic responses of the beam. Compared with the thermal relaxation time, the initial vibrational responses of the beam are more sensitive to the mechanical relaxation time of the thermoviscoelastic material.     

A Comment on the Low Speed Impact of a Clamped Beam by a Heavy Striker∗

ABSTRACT

An approximate theoretical analysis is presented for a rigid, perfectly plastic clamped beam struck transversely at the mid-span by a mass which produces Finite transverse displacements. An alternative quasi-static procedure is proposed for estimating the dynamic plastic response of a beam when struck by a heavy mass that travels at a low speed. The theoretical basis of this method is explained and the accuracy is examined by an error analysis. Finally, it is suggested that this quasi-static procedure could be used for estimating the dynamic plastic response of other structures that are struck by a heavy mass traveling at a low speed,     

Response of railway track system on poroelastic half-space soil medium subjected to a moving train load

Based on the dynamic poroelastic theory of Biot, dynamic responses of a track system and poroelastic half-space soil medium subjected to moving train passages are investigated by the substructure method. The whole system is divided into two separately formulated substructures, the track and the ground, and the rail is described by introducing the Green function for an infinitely long Euler beam subjected to the action of moving axle loads of the train and the reactions of the sleeper. Sleepers are represented by a continuous mass and the effect of the ballast is considered by introducing the Cosserat model for granular medium. Using the double Fourier transform, the governing equations of motion are then solved analytically in the frequency-wave-number domain. The time domain responses are evaluated by the inverse Fourier transform computation for a certain train speed. Computed results show that the shape of the rail displacements of the elastic and poroelastic soil medium are in good agreement with each other of the low train velocity, but the result of the poroelastic soil medium is significantly different to that of the elastic soil medium for the high train velocity which is higher than Rayleigh-wave speed in the soil. The influence of the soil intrinsic permeability on soil responses is discussed with great care in both time domain and frequency domain. The dynamic responses of the soil medium are considerably affected by the fluid phase as well as the load velocity.