圆柱杆侵彻过程及应力波传播分析

研究了初始侵彻速度为１０００ｍ／ｓ～２０００ｍ／ｓ的圆锥杆对半无限厚水泥靶的垂直侵彻过程及其应力波传播。针对初始侵彻速度范围内的撞击特点,发展了计算撞击力的刚体－流体撞击模型和计算靶体变形的法向膨胀理论。模拟动量定理和功能守恒定律,建立了圆锥杆垂直侵彻半元限厚水泫靶时的动力学模型。结非线性动力学方程的数值解,确定了撞击力。在些基础上,根据牛顿第二定律建立了圆锥杆的波动方程,研究了应力波在圆锥中的传     

双层复合材料杆的温度应力

基于平面弹性理论，用两个任意函数表示双层复合材料杆的应力，运用最小余能原理，求得了双层复合材料杆温度应力的封闭解。     

矩形截面杆的翘曲正应力

矩形截面杆的翘曲正应力申向东,康德基（内蒙古农牧学院水利系,呼和浩特０１００１８）杆在平面弯曲时,因剪切使横截面翘曲而产生的正应力,这里称为翘曲正应力,在材料力学教材中一般未给出计算表达式。本文用材料力学的一般方法求得了矩形截面杆在任意分布荷载作用下...     

双层复合材料杆的温度应力

基于平面弹性理论,用两个任意函数表示双层复合材料杆的应力。运用最小余能原理,求得了双层复合材料杆温度应力的封闭解。     

应力脉冲在变截面SHPB锥杆中的传播特性

为研究混凝土材料的动态力学性能 ,将原有的SHPB装置改装成直锥变截面式SHPB。系统分析了应力脉冲在直锥变截面杆中的传播特性 ,讨论了大小端杆径、过渡段长度以及锥角等对波传播的影响 ,为合理设计直锥变截面式SHPB装置提供了理论依据。     

杆中嵌入薄板的应力波传播行为

采用一维理论分析和二维有限元模拟,研究了杆中嵌入薄板的应力波传播行为.首先根据一维弹性应力波理论,推导了反射波,透射波以及板中应力的表达式.结合算例,分析了薄板厚度对应力波传播的影响,然后采用有限元方法,验证了一维理论分析结果,同时也研究了不同界面处理方式对结果的影响.结果表明板越薄,对应力波传播的影响越小,薄板中应力越能真实地反映杆中的应力状态;在SHPB实验中,嵌入薄片/薄膜传感器测量微弱应力信号是可行的.     

圆杆中弹性应力波的傅立叶弥散分析

基于Ｐｏｃｈｈａｍｍｅｒ和Ｃｈｒｅｅ关于无限长圆杆中纵向谐波的三维弹性解析解,得到了关于圆杆中应力波弥散效应的快速傅立叶波谱分析方法和程序（ＦＦＴＤＳＰ）,并利用二维轴对称动力学有限元分析程序（ＡＤＩＮＡ）,论证了弥散分析方法和程序的有效性。利用这一弥散分析方法和程序（ＦＦＴＤＳＰ）,研究了圆杆的物理和几何参数的变化对弹性波在圆杆中传播的弥散效应的影响。     

标准霍普金森压杆配置下的应力波分离及无时限实验数据处理

在经典一维应力波理论基础上以及试件受力平衡假定成立的条件下,提出了一种在标准霍普金森压杆实验配置下实现杆中左、右行应力波分离的新方法,可简单有效地解决常规霍普金森压杆在长时实验时左、右行波信号重叠的问题,从而保证实验中的全部应变测试数据都可以加以利用,显著提高了霍普金森压杆的测试能力。给出了新的基于杆中左、右行应力波信号的实验数据处理公式。作为霍普金森压杆实验中经典数据处理公式的扩展,在测试信号不需要进行波分离处理的情况下,新的数据处理公式等同于经典公式。利用ABAQUS 有限元软件对霍普金森压杆实验进行了数值模拟,采用虚拟实验的方式,利用模拟测试点的应变信号进行了多种实验条件下的数据处理,对该应力波分离方法的有效性及误差进行了验证与评价。数值模拟结果表明,该应力波分离方法可以给出很好的数据处理结果。在标准霍普金森压杆上进行了部分实验并利用新的波分离方法及公式对数据进行处理,所得结果令人满意。     

杆系结构多荷载识别的三角级数分析法

本文提供了一种识别杆系结构受到多荷载的作用的三角级数识别方法.将集中荷载展成三角级数且借助结构力学中的位移法建立了单根基本梁(梁单元)的位移方程,利用位移测量值反演所受到的集中荷载大小和位置.算例表明本文所用级数收敛性较好,可获得稳定的收敛值.     

有初应力钢筋混凝土压弯扭构件非线性有限元分析

钢管初应力是钢管混凝土在大跨度桥梁,高层超高层建筑应用中广大工程技术人员关心的问题,本文在钢材随动强化模型和混凝土边界模型的基础上编制了计算有初应力的钢管钢混凝压弯扭构件全过程曲线的非线性有元程序。     

抽油杆表面感应淬火引起的残余应力

本文讨论了抽油杆通过感应线圈和水冷装置时的温度场和由温度场引起的相变。在有限元计算中，通过与实验数据对比，认为考虑温度对弹性模量有影响的计算模型更合理，并用此模型计算了由温度和相变共同作用的弹塑性应力场，及最终的残余应力。结果表明淬火层超过一定厚度后，残余应力分布的合理性降低；淬火前抽油杆的强度与残余应力的大小关系较弱。     

Wave Propagation along Axes of Symmetry in Linearly Elastic Media with Initial Stress

The proofs of the Fedorov–Stippes and Fedorov's theorems, which hold for linearly elastic homogeneous bodies in natural configurations, remain valid for any linearly elastic medium with initial stress provided that Hooke's tensor be replaced by a suitable elasticity tensor.     

Stress waves in a rod subjected to a moving load

The wave processes in a semi-infinite rod located in an elastic medium and subjected to a point load moving at a constant velocity are considered. The system of two differential equations of motion of Timoshenko beam theory is solved using the Laplace transform in time. The integrals obtained are determined numerically. Variation of the bending moment on the longitudinal coordinate behind the elastic-wave front and the region of action of the point force at various times is shown. The results of the solution are influence functions. __________ Translated from Prikladnaya Mekhanika i Tekhnicheskaya Fizika, Vol. 48, No. 2, pp. 112–122, March–April, 2007.     

Axial vibration analysis of nanocones based on nonlocal elasticity theory

Carbon nanocones have quite fascinating electronic and structural properties,whose axial vibration is seldom investigated in previous studies.In this paper,based ona nonlocal elasticity theory,a nonuniform rod model is applied to investigate the small-scale effect and the nonuniformeffect on axial vibration of nanocones.Using the modifiedWentzel-Brillouin-Kramers(WBK) method,an asymptoticsolution is obtained for the axial vibration of general nonuniform nanorods.Then,using similar procedure,the axial vibration of nanocones is analyzed for nonuniform parameters,mode number and nonlocal parameters.Explicit expressionsare derived for mode frequencies of clamped-clamped andclamped-free boundary conditions.It is found that axial vibration frequencies are highly overestimated by the classicalrod model because of ignorance of the effect of small lengthscale.     

Contact interaction of an elastic punch and an elastic half-space with initial (residual) stresses

The contact interaction of an elastic punch of arbitrary cross-section and an elastic semi-space with initial (residual) stresses is studied. A general method to solve the problem is proposed. It allows solving contact problems for bodies with initial (residual) stresses when the solution of the corresponding elastic problem is known __________ Translated from Prikladnaya Mekhanika, Vol. 43, No. 12, pp. 28–40, December 2007.     

Waves in a rod under pulsed loading

Wave processes in a semi-infinite rod located in an elastic medium under pulsed loading by an external distributed force are considered. A system of two differential equations of motion of Timoshenko’s beam theory is solved with the use of the Laplace transform in time. The resultant integrals are determined numerically. The changes in bending and bending moment over the longitudinal coordinate at different times are demonstrated. __________ Translated from Prikladnaya Mekhanika i Tekhnicheskaya Fizika, Vol. 49, No. 2, pp. 178–184, March–April, 2008.     

轴对称组合弹性体初应力分析的边界元传递矩阵法

基于边界元与传递矩阵法耦合基础上，提出了一种分析轴对称组合弹性体初应力的新方法。利用边界元和传递矩阵进行分域计算轴对称组合弹性体的初应力，无需在整个结构上进行矩阵组装，只需在轴对称子午面的边界上进行离散。故该方法具有输入数据少，计算精度高及所需计算机内存小等优点，适合在微机上求解大型复杂轴对称组合结构问题。文中给出了一个组合厚壁圆筒的计算实例，分别与有限元解和理论解进行比较；结果表明：本文所提出的     

Solitary waves in initially stressed thin elastic tubes

In the present work, we study the propagation of non-linear waves in an initially stressed thin elastic tube filled with an inviscid fluid. Considering the physiological conditions of the arteries, in the analysis, the tube is assumed to be subjected to a uniform inner pressure P₀ and an axial stretch ratio λ_z. It is assumed that due to blood flow, a finite dynamical displacement field is superimposed on this static field and, then, the non-linear governing equations of the elastic tube are obtained. Using the reductive perturbation technique, the propagation of weakly non-linear waves in the longwave approximation is investigated. It is shown that the governing equations reduce to the Korteweg-deVries equation which admits a solitary wave solution. It is observed that the present model equations give two solitary wave solutions. The results are also discussed for some elastic materials existing in the literature.