三维运动接触问题的广义Галин定理

本文给出了求解一类相当普遍的三维运动接触问题的分析解法,并且把仅仅对静态接触问题成立的 定理推广到动力学情形,作了严格证明。作为例子,对接触区为椭圆的情形给出了积分形式的解,并且作了数值计算,由这些结果可以看出运动压体速度的效应。     

在摆动和移动耦联作用下结构物对周期性水平运动的反应

本文研究了在水平地面运动情况下,墙——刚性条形基础——地基系统的动力相互作用问题.文中考虑了土——结构物系统摆动和移动的耦联振动.对于地基与基础间的接触,作了如下一些假定:1)接触是焊固的,即基础的运动与地面运动相一致;2)基础底面上各点的水平位移是一常数;3)在摆动中,基础垂直位移的分布保持为一直线.为了比较起见,同样研究了非耦联情形.利用富里叶变换,问题归结为对偶积分方程(对于无耦联情形)和对偶积分方程组(对于耦联情形).借助于雅可比多项式的无限级数对此二种方程进行求解.数值结果表明,对于存在和不存在耦联影响,基础位移、墙顶对其底部的相对位移、基础底面的接触应力分布等等之间,存在着相当大的差异.     

Ляпунов直接方法在液体表面张力不稳定问题中的应用

本文应用连续系统的直接方法对于旋转液体柱,柱形液体环和柱面内外液体膜等各种情形下表面张力不稳定问题作了统一的处理,得到这些情形下旋转运动稳定的充要条件。     

大变形柔性多体系统非线性动力学数值仿真与实验研究

提出了一种作大范围运动柔性梁的非接触动态测试技术.在基于位移的柔性多体系统几何精确建模及非线性有限元分析技术的基础上,利用EAGLE-500运动分析系统及其相应的分析软件对作大范围运动钛合金柔性梁作了实验研究,并且利用之前提出的几何精确梁理论进行数值仿真.数值仿真结果与实验结果完全吻合,验证了作者所提的几何精确梁理论及...     

横观各向同性三维热弹性力学通解及其势理论法

通过引入两个位移函数，对用位移表达的运动平衡方程作了简化．利用算子理论，严格地导出了横观各向同性非耦合热弹性动力学问题的通解．对于静力学问题，通解的形式可进一步简化成用4个准调和函数来表示．具体考察了横观各向同性体内平面裂纹上下表面有对称分布温度作用的问题，推广了势理论方法，导出了一个积分方程和一个微分-积分方程．针对币状裂纹表面受均布温度作用情形，给出了具体的解。     

弹性接触问题的变分原理及参数二次规划求解

本文给出了平面与空间接触问题的带参变量的变分极值原理。接触是考虑库伦摩擦的。参变量二次规划可以用于精确求解,并且通过数例说明了计算方法。     

关于有间隙的弹性接触问题

本文对一类边界非线性的固体力学问题,即有间隙的弹性接触问题,给出了严格的数学描述,提出了三种型式:非线性边界的椭圆型边值问题,凸集上的变分不等式问题及凸集上的泛函极小问题;并且证明了它们的等价性.文章对数值解法也给出了简要说明.     

平面运动刚体两类瞬心轨迹之间关系的探讨

首先阐述了刚体运动的列阵-矩阵描述方法,然后在阐明刚体瞬心及两类瞬心轨迹等概念的基础上,经过简洁的数学推演,给出了平面运动刚体的动瞬心轨迹与定瞬心轨迹在固定坐标系中投影的运动方程.通过分析二者的运动方程,证明了结论:平面运动刚体任一时刻的动瞬心轨迹在定瞬心轨迹上作纯滚动,接触点即为刚体在该时刻的瞬心固连点.然后通过一个具体算例展示了瞬心轨迹运动方程的求解方法,并讨论了运动方程的物理意义.最后对一般运动刚体的情形进行了简要讨论.     

解三维摩擦接触问题的一个二阶锥线性互补法

针对三维摩擦接触问题的求解,给出了一种基于参变量变分原理的二阶锥线性互补法. 首先,基于三维Coulomb摩擦锥在数学表述上属于二阶锥的事实,利用二阶锥规划对偶理论,建立了三维Coulomb摩擦接触条件的参变量二阶锥线性互补模型,它是二维Coulomb摩擦接触条件参变量线性互补模型在三维情形下的自然推广;随后,利用参变量变分原理与有限元方法,建立了求解三维摩擦接触问题的二阶锥线性互补法. 较之于将三维Coulomb摩擦锥进行显式线性化的线性互补法,该方法无需对三维Coulomb摩擦锥进行线性化,因而在保证精度的前提下所解问题的规模要小很多. 最后通过算例展示了该方法的特点.      

第二种型式哈密顿原理的注记

讨论了苏联学者第二种型式的哈氏原理。给出了这种原理的四种新的型式。对于单一广义坐标的情形,用图形作了说明。最后给出了一应用简例。     

The stress on an elastic half-space due to sectionally smooth-ended punch

The axisymmetric contact problem for an elastic half-space and a rigid punch is considered using integral transform methods. The end of the punch is sectionally smooth and there is incomplete penetration. The normal stress under the punch is calculated and found to have an elliptic integral type of singularity.     

A moving punch on an infinite viscoelastic layer

Summary The problem of a rigid punch pressed against and moved on the surface of an elastic or viscoelastic layer is studied. It is shown that the governing equations reduce to the same integral equation for the elastic contact problem. Two particular motions of the punch are considered. In the first case the punch moves at a constant speed along a straight line on the surface of a viscoelastic layer. In the second case the punch moves at a constant speed along a circular path. Finally, the special case of a punch moving on a layer of a standard linear viscoelastic solid is studied. The equation is identical to a punch of modified shape pressed on an elastic layer.The work presented here was supported by the National Science Foundation under Grant GK 35163 with the University of Illinois.With 1 figure     

Contact problem for an orthotropic half-space

Numerical and analytical solutions of the 3D contact problem of elasticity on the penetration of a rigid punch into an orthotropic half-space are obtained disregarding the friction forces.A numericalmethod ofHammerstein-type nonlinear boundary integral equations was used in the case of unknown contact region, which permits determining the contact region and the pressure in this region. The exact solution of the contact problem for a punch shaped as an elliptic paraboloid was used to debug the program of the numerical method. The structure of the exact solution of the problem of indentation of an elliptic punch with polynomial base was determined. The computations were performed for various materials in the case of the penetration of an elliptic or conical punch.     

Galin's theorem holds for moving punch

This paper presents a formulation for solving three-dimensional moving punch problem. It proves that Galin's theorem holds for the punch. As an example, the study offers some results (including numerical data) of dynamic displacement over an ellipse contact region.     

Indentation of a Rigid Body into an Elastic Plate

The problem of a punch shaped like an elliptic paraboloid pressed into an elastic plate is studied under the assumption that the contact region is small. The action of the punch on the plate is modeled by point forces and moments. The method of joined asymptotic expansions is used to formulate the problem of one–sided contact for the internal asymptotic representation; the problem is solved with the use of the results obtained by L. A. Galin. The coordinates of the center of the elliptic contact region, its dimensions, and the angle of rotation are determined. The moments which ensure translational indentation of the punch are calculated and an equation that relates displacements of the punch to the force acting on it is given.     

Uniform motion of a plane punch on the boundary of an elastic half-plane

The dynamic contact problem of a plane punch motion on the boundary of an elastic half-plane is considered. The punch velocity is constant and does not exceed the Rayleigh wave velocity. The moving punch deforms the elastic half-plane penetrating into it so that the punch base remains parallel to itself at all times. The contact problem is reduced to solving a two-dimensional integral equation for the contact stresses whose two-dimensional kernel depends on the difference of arguments in each variable. A special approximation to the kernel is used to obtain effective solutions of the integral equation. All basic characteristics of the problem including the force of the punch elastic action on the elastic half-plane and the moment stabilizing the punch in the horizontal position in the process of penetration are obtained. A similar problem was considered in [1] and earlier in the “mode of steady-state motions” in [2, 3] and in other publications.     

Determination of optimal shape of a moving punch with friction taken into account

The optimization problem for the contact interaction between a rigid punch and an elasticmediumis considered. It is assumed that that the punch is under the action of some prescribed forces and momenta and moves along a surface bounding a half-space filled with an elastic medium. It is also assumed that themotion is quasistatic and the friction forces arising in the region of contact are taken into account. The punch shape is considered as the desired design variable, and the integral functional characterizing the discrepancy between the pressure distribution in the region of contact that corresponds to the optimized shape of the punch and a given goal distribution of pressure is taken as the minimizing criterion. The optimal shape can be determined efficiently by solving the following two problems: first, to obtain the optimal pressure distribution and then to solve a boundary value problemfor the elastic half-space under the action of the obtained normal pressure and friction forces. By way of example, the optimal shape is analytically determined for a punch of rectangular shape in horizontal projection.     

On a conical punch pressing into an elastic layer

A conical punch presses into an elastic layer resting on a rigid foundation. Precision numerical results for the radius of the circle of contact, the force required, and the displacement of the center of the punch are presented.     

Uniform indentation of the elastic half-space by a rigid rectangular punch

The problem considered is that of a rigid flat-ended punch with rectangular contact area pressed into a linear elastic half-space to a uniform depth. Both the lubricated and adhesive cases are treated. The problem reduces to solving an integral equation (or equations) for the contact stresses. These stresses have a singular nature which is dealt with explicitly by a singularity-incorporating finite-element method. Values for the stiffness of the lubricated punch and the adhesive punch are determined: the effect of adhesion on the stiffness is found to be small, producing an increase of the order of 3%.