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1.
一般情况下平面应变问题归结为一个双调和方程、一个调和方程及轴向应变应满足平面坐标x、y 的线性函数条件下的求解.进一步分析证明,轴向载荷分布必须是x、y 的线性函数类问题都能按广义平面应变公式进行分析.  相似文献   

2.
平面弹性力学问题的离散元法   总被引:1,自引:0,他引:1  
根据离散元的基本原理,基于变形体的理论提出了适用于平面弹性力学问题的界面位移、应变和应力模式,建立了求解平面弹性力学问题的离散元方程和相应的迭代求解方法.通过界面位移可以简洁地将位移和力的边界条件引入离散系统的控制方程,也可以方便地求解节点位移.数值算例表明,与具有相同网格的有限元结果相比,离散元能同时给出精度相对较高的应力解和精度相当的位移解.  相似文献   

3.
以指数函数近似表示非线弹性材料的应力-应变关系, 推导出了非线弹性材料平面杆系结构应力应变计算的普遍表达式, 编制了通用程序, 使这一类问题有了一个通用的解题方法.  相似文献   

4.
关于弹性力学平面问题的协调方程几乎所有的弹性力学书都有所讨论,但没有一本书把平面问题的协调方程与空间问题联系起来讨论,因为任何实际问题都是空间问题,所谓平面问题只是空间问题的一种简化。专著[1]似乎想从空间同题的协调方程讨论平面阃题的协调方程。但是我们认为专著[1]关于平面应力问题协调方程的讨论尚有不妥之处,下面提出我们 ...  相似文献   

5.
平面应变断裂韧度测试的有效性研究   总被引:1,自引:0,他引:1  
针对平面应变断裂韧度测试厚度存在的问题,研究了几种材料测断裂韧度所需的实际厚度,拟合了平面应力到平面应变过渡状态下σz应力的分布,分析了过渡状态下的裂端应力场.通过分析不同材料特性和应力状态对断裂韧度KIC的影响,结合金属材料断裂的细观机理,认为平面应变断裂韧度KIC反映的是材料正断的性能,仅代表材料发生正断的指标.结果表明:对于某些高韧性材料,即使满足平面应变条件厚度要求,断裂以剪断为主,很难测出KIC;而对于偏脆性材料,即使不满足厚度要求,只要发生正断,也可测出KIC.结合已有试验结果,为平面应变断裂韧度KIC测定的厚度选择,提出一种合理的预测方法.借助三片模型的研究,给出平面应变断裂韧度的正断指标.  相似文献   

6.
将基于应变软化玻璃状高分子材料微观特征建立的BPA8-链分子网络模型引入UpdatingLagrange有限元方法,建立了适于变形局部化分析的大变形弹塑性有限元驱动应力法.在此基础上,数值模拟了初始各向同性高分子材料平面应变拉伸变形局部化的传播过程.探讨了BPA模型对具有加工硬化特性的结晶性高分子材料变形分析的适应性;分析了局部化传播过程中颈缩截面的非均匀应力三轴效应;最后,讨论了网格尺寸以及初始几何不均匀性对颈缩扩散以及应力三轴效应的影响  相似文献   

7.
板弯曲与平面弹性问题的多类变量变分原理   总被引:3,自引:0,他引:3  
钟万勰  姚伟岸 《力学学报》1999,31(6):717-723
进一步完善板弯曲与平面弹性问题的多类变量变分原理,给出了相关边界积分项的具体表达式.多类交量变分原理涵盖了平衡、应力函数、应力、位移一应变、协调和物性共五大类基本方程和所有边界条件,是一个具有更加广泛意义的变分原理.  相似文献   

8.
以严格平面应变解为基础,对简化平面应变土体模型即三个单元Voigt体串联模型的精度进行了研究.在各有关影响因素(如土体剪切模量、密度、剪切波速及结构物截面尺寸等)变化条件下,就两种模型土体作用于结构物交界面上的复刚度的实部和虚部分别进行了对比研究,全面地分析了两种模型复刚度的差异性,并进一步对桩顶受纵向激振力作用下的频域及时域动力响应进行了求解,研究了两种模型下桩顶动力响应的差别.结果表明,对土体复刚度而言,在大多数情况下,简化平面应变模型具有足够的精度,可以满足一般工程应用的需要;对桩顶频域响应和时域响应而言,简化平面应变模型已具有较高的精度,其误差可以忽略,具有很强的工程适用性,为该模型在相关领域的应用提供了坚实的理论依据.  相似文献   

9.
在航空航天、船舶、石油管道和核电等领域,服役结构或部件在长期极端条件下运行,不可避免地会产生裂纹,因此,为研究含裂纹结构的准静态断裂行为,必须了解裂纹尖端附近区域的应力应变场特点.对于幂律材料裂纹构元,研究平面应变和平面应力条件下Ⅰ型裂纹尖端应力场的解析分布.基于能量密度等效和量纲分析,推导了能量密度中值点代表性体积单元(representative volume element, RVE)的等效应力解析方程,并定义其为应力因子,进而针对有限平面应变和平面应力紧凑拉伸(compact tension, CT)试样和单边裂纹弯曲(single edge bend, SEB)试样,以应力因子作为应力特征量,并构造用于表征裂尖等效应力等值线的蝶翅轮廓式和扇贝轮廓式三角特殊函数,提出描述幂律塑性条件下平面I型裂纹尖端应力场的半解析模型.该半解析模型形式简单,对CT和SEB试样的裂尖应力场的预测结果与有限元分析的结果比较表明,两者之间均密切吻合,模型公式可直接用于预测Ⅰ型裂纹尖端应力分布,方便于断裂安全评价和理论发展.  相似文献   

10.
采用一个能描述材料压力敏感性和SD效应的抛物型屈服准则,运用正交流动法则给出了材料的本构方程.在平面应力条件下,得出了裂纹尖端弹塑性应力场的基本解.在不同受力状态下(表现在采用不同的塑性混合因子),给出裂纹尖端应力场解的构造.讨论了材料参数对裂纹尖端应力场分布的影响.在自相似假设下讨论了应变的奇异性.结果表明,对于纯Ⅰ...  相似文献   

11.
On condition that any perfectly plastic stress component at a crack tip is nothingbut the function ofθ.by making use of equilibrium equations,anisotropic plastic stress-strain-rate relations,compatibility equations and Hill anisotropic plastic yieldcondition,in the present paper,we derive the generally analytical expressions of theanisotropic plastic stress field at a mixed-mode crack tip under plane and anti-planestrain.Applying these generally analytical expressions to the mixed-mode cracks,wecan obtain the analytical expressions of anisotropic plastic stress fields at the tips ofmixed-modeⅠ-Ⅲ,Ⅱ-ⅢandⅠ-Ⅱ-Ⅲcracks.  相似文献   

12.
The torsional static and dynamic behaviors of circular nanosolids such as nanoshafts, nanorods and nanotubes are established based on a new nonlocal elastic stress field theory. Based on a new expression for strain energy with a nonlocal nanoscale parameter, new higher-order governing equations and the corresponding boundary conditions are first derived here via the variational principle because the classical equilibrium conditions and/or equations of motion can- not be directly applied to nonlocal nanostructures even if the stress and moment quantities are replaced by the corresponding nonlocal quantities. The static twist and torsional vibration of circular, nonlocal nanosolids are solved and discussed in detail. A comparison of the conventional and new nonlocal models is also presented for a fully fixed nanosolid, where a lower-order governing equation and reduced stiffness are found in the conventional model while the new model reports opposite solutions. Analytical solutions and numerical examples based on the new nonlocal stress theory demonstrate that nonlocal stress enhances stiffness of nanosolids, i.e. the angular displacement decreases with the increasing nonlocal nanoscale while the natural frequency increases with the increasing nonlocal nanoscale.  相似文献   

13.
姚仰平  孙凯  路德春 《力学学报》2007,39(5):692-698
通过与金属材料的类比,分析了岩土材料的特征面(SMP面)的特性,提出了SMP面上的应力 决定岩土材料塑性应变增量流动方向的观点,并由此推导出计算公式. 通过增加一个材料参 数,还可以考虑存在黏聚力时的情况. 由该公式计算的塑性应变增量方向得到了 试验结果的验证. 该公式也在用变换应力修正的剑桥模型中得到应用,模型预测结果能够合理反映试验数据.  相似文献   

14.
Under the condition that any Perfectly plastic stress component at a crack tip isnothing but the function of θ only. making use of equilibrium equations, stress-strain-rate relations, compatibility equations and yield condition. in this paper. we derive thegeneral analytical expressions of the perfectly plastic stress field at a Mixed-Mode cracktip under plane and anti-plane strain. Applying this general analytical expressions to theMixed-Mode cracks. we can obtain the analytical expressions of perfectly plastic stressfields at the tips of Mixed-ModeⅠ-Ⅲ.Ⅱ-Ⅲ andⅠ-Ⅱ-Ⅲ cracks.  相似文献   

15.
A theoretical framework is presented for the statics and kinematics of discrete Cosserat-type granular materials. In analogy to the force and moment equilibrium equations for particles, compatibility equations for closed loops are formulated in the two-dimensional case for relative displacements and relative rotations at contacts. By taking moments of the equilibrium equations, micromechanical expressions are obtained for the static quantities average Cauchy stress tensor and average couple stress tensor. In analogy, by taking moments of the compatibility equations, micromechanical expressions are obtained for the (infinitesimal) kinematic quantities average rotation gradient tensor and average Cosserat strain tensor in the two-dimensional case. Alternatively, these expressions for the average Cauchy stress tensor and the average couple stress tensor are obtained from considerations of the equivalence of the continuum force and couple traction vectors acting on a plane and the resultant of the discrete forces and couples acting on this plane. In analogy, the expressions for the average rotation gradient tensor and the average Cosserat strain tensor are obtained from considerations of the change of length and change of rotation of a line element in the two-dimensional case. It is shown that the average particle stress tensor is always symmetrical, contrary to the average stress tensor of an equivalent homogenized continuum. Finally, discrete analogues of the virtual work and complementary virtual work principles from continuum mechanics are derived.  相似文献   

16.
In the present paper,the compatibility equation for the plane stress problems of power-law materials is transformed into a biharmonic equation by introducing the so-calledcomplex pseudo-stress function,which makes it possible to solve the elastic-plastic planestress problems of strain hardening materials described by power-law using the complexvariable function method like that in the linear elasticity theory.By using this generalmethod,the close-formed analytical solutions for the stress,strain and displacementcomponents of the plane stress problems’of power-law materials is deduced in the paper,which can also be used to solve the elasto-plastic plane stress problems of strain-hardeningmaterials other than that described by power-law.As an example,the problem of a power-law material infinite plate containing a circular hole under uniaxial tension is solved byusing this method,the results of which are compared with those of a known asymptoticanalytical solution obtained by the perturbation method.  相似文献   

17.
One considers a linear thermoelastic composite medium, which consists of a homogeneous matrix containing a statistically homogeneous random set of ellipsoidal uncoated or coated heterogeneities. It is assumed that the stress–strain constitutive relations of constituents are described by the nonlocal integral operators, whereas the equilibrium and compatibility equations remain unaltered as in classical local elasticity. The general integral equations connecting the stress and strain fields in the point being considered and the surrounding points are obtained. The method is based on a centering procedure of subtraction from both sides of a known initial integral equation their statistical averages obtained without any auxiliary assumptions such as, e.g., effective field hypothesis implicitly exploited in the known centering methods. In a simplified case of using of the effective field hypothesis for analyzing composites with one sort of heterogeneities, one proves that the effective moduli explicitly depend on both the strain and stress concentrator factor for one heterogeneity inside the infinite matrix and does not directly depend on the elastic properties (local or nonlocal) of heterogeneities. In such a case, the Levin’s (1967) formula in micromechanics of composites with locally elastic constituents is generalized to their nonlocal counterpart. A solution of a volume integral equation for one heterogeneity subjected to inhomogeneous remote loading inside an infinite matrix is proposed by the iteration method. The operator representation of this solution is incorporated into the new general integral equation of micromechanics without exploiting of basic hypotheses of classical micromechanics such as both the effective field hypothesis and “ellipsoidal symmetry” assumption. Quantitative estimations of results obtained by the abandonment of the effective field hypothesis are presented.  相似文献   

18.
提出一种计算广义平面应交状态下复合材料切口应力奇性指数的新方法.在切口尖端的位移幂级数渐近展开式被引入正交各向异性材料的物理方程后,将用位移表示的应力分量代入切口端部柱状邻域的线弹性理论控制方程,切口应力奇性指数的计算被转化为常微分方程组特征值的求解.采用插值矩阵法求解该常微分方程组,可一次性地获取切口尖端多阶应力奇性指数.本法适合平面和反平面应力场耦合或解耦的情形,并可退化计算裂纹或各向同性材料切口的应力奇性指数.算例表明,所提方法对分析复合材料切口应力奇性指数是一种准确有效的手段.  相似文献   

19.
A theory of thermoelastic composites with nonlocal properties of constituents is analyzed for multiphase elastic solids of arbitrary geometry and material symmetry. Due to their generality, one uses the nonlocal integral models because the gradient models are usually derived as approximations of corresponding integral models in the immediate (infinitely closed) vicinity of the point being considered. One explores a simplified theory for linear (macroscopically) elasticity, which differs from the classical local theory in the stress–strain constitutive relation only, whereas the equilibrium and compatibility equations remain unaltered. One obtains the new representation of the effective modulus and compliance through the mechanical influence function which does not explicitly depend (as opposed to its local counterpart) on the elastic operators of constituents. The representations for the effective eigenstrains and eigenstresses through either the mechanical influence functions or transformation influence functions are presented. The effective strain energy and potential energy are expressed in terms of only average values of the state variables and the effective properties. Representations of both the first and second statistical moments of stress and strain fields in the constituents are also performed. Many of the results were obtained as the straightforward generalizations of their local counterparts because the methods used for obtaining the mentioned results widely exploit the Hill’s (1963) condition which holds for any compatible strain field and equilibrium stress field not necessarily related to each other by a specific stress–strain relation.  相似文献   

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