结构动力学方程数值积分的三参数算法

本文提出计算结构动力响应的三参数单步数值积分法,它具有无条件稳定性质,并具有合适的算法阻尼.通过分析及与其他数值积分法比较,说明本文算法的精度有所提高.     

基于位移型Gurtin变分原理计算动力响应的逐步积分法

本文利用位移型Ｇｕｒｔｉｎ变分原理,在时间域上采用三次Ｈｅｒｍｉｔｅ插值函数进行离散,给出了一种计算结构动力响应的逐步积分方法。通过稳定性分析研究了该方法的稳定区情况表明,当１．６４≤θ≤２．０８时,该方法的数值计算精度很高,但是条件稳定积分格式。当θ≥４．１时,该方法是无条件稳定的积分格式,精度较高。     

负屈服刚度条件下数值积分的收敛性和稳定性

本文研究了结构非弹性动力分析中负刚度条件下数值积分法的收敛性和稳定性,讨论了相应的判断准则,作为应用实例的分析结果表明:Ncwmark平均常加速度法满足负刚度条件下数值积分法的收敛性和稳定性的要求;Houbolt方法满足收敛性的要求,但其稳定性依赖于刚度比及积分步长,与正刚度条件下迴然不同。     

一种无条件稳定的结构动力学显式算法

利用离散控制理论, 针对结构动力学方程时间积分提出了一种新的无条件稳定的显式算法. 新算法采用CR 算法的速度和位移递推格式, 同时利用Z变换获得算法对应的传递函数, 进而根据极点条件推导了递推格式系数的具体表达式. 然后, 在其系数中引入了一个控制周期延长率的变量s, 从而调节新算法的精度. 理论分析表明无条件稳定显式新算法具有二阶精度、零振幅衰减率、无超调和自起步特性, 且周期延长率可以用变量s控制, 而CR 算法只是本文新算法的特例. 最后, 确定了非线性刚度硬化系统的稳定性界限, 并给出了使新算法精度达到较高的变量s的区间. 算例分析表明, 在此变量区间内取值时, 新算法的精度要优于纽马克常平均加速度算法和CR 算法.      

一类带高频耗散的动力学显式算法

带数值耗散的算法因其能有效过滤虚假高频响应的影响而备受关注。基于离散控制理论Z变换,提出一类带数值耗散的结构动力学显式算法。该算法采用CR法的速度和位移递推式,满足零振幅衰减率,且对线性系统和非线性刚度软化系统为无条件稳定,对刚度硬化系统则是条件稳定的;该算法由单个参数ρ控制数值耗散能力。通过对振幅衰减和周期延长的理论分析表明,系数a可调节算法的精度和非线性稳定区间,给出精度最优时系数的取值。对特定的系数取值该算法可转变为CR法。通过算例对线性系统和非线性系统的分析验证了新算法具有良好的精度、稳定性和数值耗散,表明新算法是正确有效的。     

防护结构拟动力试验方法及其数值积分方法研究

近来发展起来的拟动力试验方法用于防护结构的抗爆试验是一项正在研究的技术￣［１］，针对于此项研究中数值积分方法部分进行了研究。分析了可用于防护结构拟动力试验的各种积分方法，讨论了已有方的数值特征及可行性。并提出一种修正的中心差分方法用来对因试验摩擦引起的能量损失进行补偿，同时研究了该方法的数值特性。     

岩土弹塑性有限元分析的隐式积分弹性刚度法

本文提出了用于岩土弹塑性有限元分析的隐式积分弹性刚度算法。该算法既具有隐式积分法精度好、效率高、无条件稳定等优点，也具有弹性刚度法中刚度矩阵正定、对称的特点，更重要的是它避免了传统切线刚度法在处理岩土非相关联塑性流动和屈服面“角点”所遇到的非对称性和奇异性计算问题。通过算例分析了该算法的精度、效率     

岩土弹塑性有限元分析的隐式积分弹性刚度法

本文提出了用于岩土弹塑性有限元分析的隐式积分弹性刚度算法。该算法既具有隐式积分法精度好，效率高，无条件稳定等优点，也具有弹性刚度矩阵正定、对称的特点，更重要的是它避免了传统切线刚度法在处理岩土非相关联塑性流动和屈服面“角角”所遇到的非对称性和奇异性计算问题。通过算例分析了该算法的精度、效率。     

拟协调等腰梯形壳元显式几何刚度阵及屈曲分析

采用拟协调元方法推导了等腰梯形薄壳元的显式几何刚度阵，用于组合结构屈曲分析的计算，结果表明，这种单元的几何刚度阵收敛快、精度好。     

拟协调等梯形壳元显式几何刚度阵及屈曲分析

采用拟协调元方法推导了等腰梯形薄壳元的显式几何刚度阵，用于组合结构屈曲分析的计算，结果表明，这种单元的几何刚度阵收敛快、精度好。     

一种基于直接计算高阶奇异积分的断裂力学双边界积分方程分析法

相对于有限元法,边界单元法在求解断裂问题上有着独特的优势,现有的边界单元法中主要有子区域法和双边界积分方程法.采用一种改进的双边界积分方程法求解二维、三维断裂问题的应力强度因子,对非裂纹边界采用传统的位移边界积分方程,只需对裂纹面中的一面采用面力边界积分方程,并以裂纹间断位移为未知量直接用于计算应力强度因子.采用一种高阶奇异积分的直接法计算面力边界积分方程中的超强奇异积分;对于裂纹尖端单元,提供了三种不同形式的间断位移插值函数,采用两点公式计算应力强度因子.给出了多个具体的算例,与现存的精确解或参考解对比,可得到高精度的计算结果.      

汶川地震诱发文家沟巨型滑坡 碎屑流基本特征及成因机制初步分析

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2008年5月12日,汶川M80地震在四川省绵竹市清平乡文家沟内诱发一巨型滑坡。通过现场调查得知,滑坡前后缘高差455m,厚度20～30m,滑面为基岩层面,初始方量2750×107m3。滑体在运动中转化为碎屑流。滑坡-碎屑流总的水平运动距离为4022m,垂直运动距离为1443m,遗留的堆积物体积达5×107m3。滑坡距映秀—北川断裂仅36km,位于其下盘,地震烈度达XI度。滑坡导致文家沟中48人遇害,并形成一条完整的地震次生地质灾害链。初步分析表明滑坡启动速度快,滑坡向碎屑流转化过程明显、地点明确。碎屑流运动过程复杂,伴有强烈的“气垫效应”和“前缘气浪冲击效应”。作者认为,文家沟滑坡的高启动速度是长持时强烈地震动作用的结果,与山体的猛烈碰撞是导致滑体解体并转化为碎屑流的原因。     

Preface: Orbits around asteroid

One of the core issues in modern celestial mechanics is the orbital dynamics in the near-regime gravitational field of as- teroids, which provides deep insights into the mathematical nature of a class of nonlinear systems, and plays as a critical basis for in situ explorations of different science goals. Lots of efforts have been made to reveal the characteristics of orbital motion in the vicinity of asteroids, and to improve the skills of asteroid research in methodology.     

Preface: Current research progress on mechanics of high speed rail

The construction and operation of high-speed rail（HSR）grid within the past two decades in China,in terms of the scale,may be possibly comparable to any national-wide construction in the history of China,even the Great Wall.By counting railways with commercial train service at the speed of200 km/h,China has the world’s longest HSR network with over 19 369.8 km of track in service today and this number     

ACTA MECHANICA SINICA 2014 ANNUAL SUBJECT INDEX

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Effet de l'anisotropie élastique cristalline sur la distribution des facteurs de Schmid à la surface des polycristauxInfluence of crystalline elasticity anisotropy on Schmid factor distribution at the free surface of polycrystals

Experimental studies of the plasticity mechanisms of polycrystals are usually based on the Schmid factor distribution supposing crystalline elasticity isotropy. A numerical evaluation of the effect of crystalline elasticity anisotropy on the apparent Schmid factor distribution at the free surface of polycrystals is presented. Cubic elasticity is considered. Order II stresses (averaged on all grains with the same crystallographic orientation) as well as variations between averages computed on grains with the same crystallographic orientation but with different neighbour grains are computed. The Finite Element Method is used. Commonly studied metals presenting an increasing anisotropy degree are considered (aluminium, nickel, austenite, copper). Concerning order II stresses in strongly anisotropic metals, the apparent Schmid factor distribution is drifted towards small Schmid factor values (the maximum Schmid factor is equal to 0.43 instead of 0.5) and the slip activation order between characteristic orientations of the crystallographic standard triangle is modified. The computed square deviations of the stresses averaged on grains with the same crystallographic orientation but with different neighbour grains are a bit higher than the second order ones (inter-orientation scatter). Our numerical evaluations agree quantitatively with several observations and measures of the literature concerning stress and strain distribution in copper and austenite polycrystals submitted to low amplitude loadings. Hopefully, the given apparent Schmid factor distributions could help to better understand the observations of the plasticity mechanisms taking place at the free surface of polycrystals. To cite this article: M. Sauzay, C. R. Mecanique 334 (2006).     

Nonlinear behavior of matrix-inclusion composites under high confining pressure: application to concrete and mortar

This paper is devoted to a micromechanics-based simulation of the response of concrete to hydrostatic and oedometric compressions. Concrete is described as a composite made up of a cement matrix in which rigid inclusions are embedded. The focus is put on the role of the interface between matrix and inclusion which represent the interfacial transition zone (ITZ). A plastic behavior is considered for both the matrix and the interfaces. The effective response of the composite is derived from the modified secant method adapted to the situation of imperfect interfaces. To cite this article: T.H. Le et al., C. R. Mecanique 336 (2008).