焊趾表面裂纹的形态发展曲线与疲劳寿命预测

以作者建立的焊地椭圆表面裂纹应力强度因子数据库以及复杂应力场中焊践半随圆表面裂纹前缘应力强度因子分布计算的基本模式法为基础上,给出了复杂应力场中焊践表面表纹在疲劳扩展过程中形态变化规律及寿命的工程分析方法。     

给定寿命下的焊趾疲劳裂纹深度尺寸分析

本文提供并用统计方法研究了焊趾疲劳裂纹扩展的Ｎ～α曲线族，给出了联系给定裂纹尺寸下的疲劳分布，给定疲劳寿命下的裂纹尺寸分布以及随机初始条件的概率相容条件。研究表明，给定寿命下的焊趾疲劳裂纹深度尺寸α服从分布Ф［（μ（ａ）－ｌｏｇＮ）／σ（ａ）］。     

脆性岩石断裂破坏机理的边界配位法分析

针对裂纹表面承受载荷时的应力条件，提出了新的应力函数，该应力函数对于各种裂纹模型、各种边界条件、各种边界形状、裂纹表面自由或承受均布载荷等均适用．并利用边界配位法，计算了在压缩载荷下，岩石内部裂纹的应力强度因子（ＳＩＦ），给出了关于岩石断裂破坏的一些新结论     

管节点表面裂纹应力强度因子的研究

本文分析了Ｔ、Ｋ、Ｙ型管节点应力分布特征，在三维光弹试验结果验证的基础上，提出了适用于断裂力学方法应用的Ｔ、Ｋ、Ｙ型管节点的应力强度因子（ＳＩＦ）表达式。     

裂纹表面承受均布载荷时的应力强度因子及裂纹张开位移的边界配位法

本文针对裂纹表面承受载荷时的应力条件，提出了新的应力函数，对于各种裂纹模型、各种边界条件、各种边界形状、裂纹表面自由或承受均布载荷等均适用。并利用边界配位法，计算了裂纹表面承受均布载荷时的方型板内中心裂纹的应力强度因子（ＳＩＦ）及裂纹的张开位移（ＣＯＤ）。     

The expression of stress and strain at the tip of three-dimensional notch

ＴＨＥＥＸＰＲＥＳＳＩＯＮＯＦＳＴＲＥＳＳＡＮＤＳＴＲＡＩＮＡＴＴＨＥＴＩＰＯＦＴＨＲＥＥ－ＤＩＭＥＮＳＩＯＮＡＬＮＯＴＣＨＱｉａｎＪｕｎ（钱俊）（ＥａｓｔＣｈｉｎａＩｎｓｔｉｔｕｔｅｏｆＴｅｃｈｍｏｌｏｇｙ）ＮａｎｊｉｎｇＬｏｎｇＹｕ－ｑｉｕ（龙驭...     

界面端附近裂纹的应力强度因子

结合材料的断裂形式可分为从界面端产生裂纹（沿界面或向母材内部层折）然后断裂与稍稍离开界面端处产生裂纹然后断裂这两种情况，在金属／陶瓷类结合材料中，后者出现的概率更大，本文利用结合材料界面端的奇异应力场和叠加原理，给出了界面端附近裂纹的应力强度因子近似计算公式，并用边界元数值计算验证了其有效性。     

残余应力对压力容器破坏模式的影响分析

破前漏(简称LBB)是压力容器、核电站设备结构设计与评价中的一个重要准则.表面裂纹准静态扩展的几何形貌变化规律的预测是破前漏(LBB)评判十分重要的课题之一.本文对特定焊接残余应力场加载作用下,含三维表面裂纹的压力容器模型,用有限元软件(ABAQUS)进行了表面裂纹准静态扩展模拟计算,得到在此残余应力场作用下应力强度因子沿裂纹前缘的分布规律.结合外载引起的应力强度因子,就可以判别裂纹的扩展形貌,从而判断结构是否满足LBB要求.     

MOTION EQUATIONS OF MULTILAYERED ELASTIC ELECTROCONDUCTIVE PLATES IN A MAGNETIC FIELD

ＭＯＴＩＯＮＥＱＵＡＴＩＯＮＳＯＦＭＵＬＴＩＬＡＹＥＲＥＤＥＬＡＳＴＩＣＥＬＥＣＴＲＯＣＯＮＤＵＣＴＩＶＥＰＬＡＴＥＳＩＮＡＭＡＧＮＥＴＩＣＦＩＥＬＤＧｏｕＸｉｎｇ－ｈｕａ（苟兴华）（ＳｉｃｈｕａｎＵｎｉｖｅｒｓｉｔｙ,Ｃｈｅｎｇｄｕ）ＺｈａｎｇＦａ...     

SH波对有部分脱胶衬砌的圆形孔洞的散射

本文研究了圆形孔洞内衬砌与孔洞部分脱胶时对ＳＨ波的散射．将脱胶区看作表面不相接触的弧形界面裂纹，利用波函数展开法，并引入裂纹面的位错密度函数，将问题归结为一组奇异积分方程．通过数值计算获得了动应力强度因子（ＤＳＩＦ）和远场位移及散射截面（ＳＣＳ）．结果显示：由于脱胶，ＤＳＩＦ和ＳＣＳ在较低的频率上发生共振．     

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).