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1.
有限应变下蠕变—弹塑性—损伤耦合本构模型的数值模拟   总被引:1,自引:0,他引:1  
本文提出了一个模拟有限元应变下各向同性蠕变-弹塑性-损伤耦合本构行为的数值模型。模型基于不可逆过程的热动力学和内状态变量理论、以及应力就变本构关系的超弹性形式描述和变形梯度的弹性及非弹性部分的乘式分解。  相似文献   

2.
以碳酚醛靶中的一维应变热击波为例,讨论本构模型对热击波数值模拟结果的影响.数值模拟采用3种本构模型,即各向同性理想弹塑性本构模型、各向异性理想弹塑性本构模型及各向异性动态弹塑性本构模型.结果表明:与各向同性理想弹塑性、各向异性理想弹塑性本构模型相比,利用各向异性动态弹塑性本构模型获得的热击波应力峰值较小、应力峰值衰减较...  相似文献   

3.
基于弹塑性力学和损伤理论,建立了一个与应力球张量有关的正交各向异性材料的混合硬化屈服准则,该准则无量纲化后与各向同性材料的Mises准则同构,在此基础上,进而建立了混合硬化正交各向异性材料的增量型弹塑性损伤本构方程,并以具局部损伤的正交各向异性矩形薄板为例,采用Galerkin法和迭代法,对其弹塑性屈曲问题进行了分析,讨论了局部损伤对正交各向异性矩形薄板弹塑性屈曲临界应力的影响.   相似文献   

4.
基于弹塑性力学和损伤理论,建立了一个与应力球张量有关的正交各向异性材料的混合硬化屈服准则,该准则无量纲化后与各向同性材料的Mises准则同构,进而建立了混合硬化正交各向异性材料的增量型弹塑性损伤本构方程和损伤演化方程.基于经典Kirchhoff板理论,获得了正交各向异性薄板的增量型运动控制方程,且采用有限差分法和迭代法进行求解.数值算例中,讨论了损伤演化、外载荷参数等因素对正交各向异性薄板弹塑性静动力性质的影响,数值结果表明,考虑结构的损伤和损伤演化时,结构的力学性质将发生显著的变化.  相似文献   

5.
含损伤材料的热粘塑性本构关系和柱壳破裂研究   总被引:3,自引:1,他引:2  
以含内变量的本构关系理论为基础 ,结合材料损伤演化方程 ,并考虑了温度和损伤对材料参数的影响 ,得到了增量形式的热粘塑性本构关系的普适显式表达式。然后使用Bodner幂函数型粘塑性模型 ,具体推导了其增量形式的热粘塑性本构方程。接着结合在实践中有重要意义的内部爆炸载荷作用下的柱壳破裂问题 ,建立了含损伤热粘塑性柱壳破裂问题的完备方程组 ,使用有限差分方法 ,完成了对问题的数值模拟 ,并对结果进行了分析。计算结果与实验结果符合良好。  相似文献   

6.
基于弹塑性力学和损伤理论,建立了一个与应力球张量有关的具损伤正交各向异性材料的混合硬化屈服准则,该准则无量纲化后与各向同性材料的Mises准则同构,在此基础上,建立了正交各向异性材料的增量型和全量型弹塑性损伤本构方程,并以具确定弱区域正交各向异性矩形薄板为例,根据屈曲时的能量准则和全量理论,以等效塑性应变为内变量,对其弹塑性屈曲问题进行了分析,讨论了几何参数和弱区域对正交各向异性薄板弹塑性屈曲临界应力的影响.  相似文献   

7.
变温场中具损伤粘弹性矩形板的非线性动力响应分析   总被引:6,自引:0,他引:6  
基于热粘弹性理论、Von Karman板理论和连续损伤力学,导出了二维状态下各向同性材料的变温粘弹性本构方程,建立了含损伤效应的各向同性粘弹性矩形板在变温场中的非线性运动控制方程,且应用有限差分法对问题进行求解.算例中,讨论了损伤演化及温度场等因素对粘弹性矩形板非线性动力学行为的影响,得出一些有意义的结论.  相似文献   

8.
各向同性弹性损伤的双标量描述   总被引:24,自引:1,他引:24  
损伤状态的描述是损伤力学中仍未完善解决的基本问题.我们旨在对此问题就最简单的一种情形——各向同性弹性损伤,进行较为全面的研究.首先,指出了古典各向同性损伤理论中,基于应变等效假设,用单个标量损伤变量描述损伤状态的局限性.然后,建立了一个用两个标量损伤变量描述的各向同性弹性损伤模型.此模型解除了古典理论的局限,能完全描述各向同性弹性损伤,并且得到本文数值实验的验证.最后,将本文模型与现有细观力学结果连接,给出了宏细观损伤变量之间的关系,使得细观量可以通过宏观量来反映,建立了一个用细观损伤材料常数描述细观缺陷特征的损伤本构模型  相似文献   

9.
本文从张量代数的观点提出了一类塑性本构方程,这类方程给出了塑性应变增量dε~p和立力增量dσ之间的一一对应关系。可证明,这类方程自然地表示出所谓的角点硬化模型。对这类塑性本构方程中的若干例子作了系统的表述。对塑性而言,应力的类时测度dσ=[(3/2)tr(dT~2)]~(1/2)和应变的类时测度dε=[(2/3)tr(de~p)~2]~(1/2),可用以有效地表示加载或应变的历史,其中dT是在Jaumann率意义下的偏应力增量,de~p表示塑性偏应变的增量。首先,把材料看成是初始各向同性的,但随着变形而变为各向异性。对这一情形,可以有效地应用Wang的对各向同性张量函数的表示定理。然而,在这情形中,各向异性是受到限制的。因此,这种理论应推广到初始及随后的一般各向异性起重要作用的情形。这样,把各向异性的屈服法则,如随动硬化、随动各向同性硬化以及其他一般无角点的各向异性硬化情形跟有角点硬化情形相结合就成为可能了。如引入自然时间测度dt,则理论可推广来表达跟自然时间有关的非弹性本构方程,如蠕变和/或粘弹性等。此外,如果同时引进自然时间测度和内部时间测度,即dt跟加dσ或dt跟dε的结合,则理论还可推广到同时跟自然时间和内部时间有关的非弹性本构方程,如粘塑性和/或动态塑性所需表达的情形。有些情形,还要考虑跟温度的  相似文献   

10.
针对准脆性材料的非线性特征:强度软化和刚度退化、单边效应、侧限强化和拉压软化、不可恢复变形、剪胀及非弹性体胀,在热动力学框架内,建立了准脆性材料的弹塑性与各向异性损伤耦合的本构关系。对准脆性材料的变形机理和损伤诱发的各向异性进行了诠释,并给出了损伤构形和有效构形中各物理量之间的关系。在有效应力空间内,建立了塑性屈服准则、拉压不同的塑性随动强化法则和各向同性强化法则。在损伤构形中,采用应变能释放率,建立了拉压损伤准则、拉压不同的损伤随动强化法则和各向同性强化法则。基于塑性屈服准则和损伤准则,构建了塑性势泛函和损伤势泛函,并由正交性法则,给出了塑性和损伤强化效应内变量的演化规律,同时,联立塑性屈服面和损伤加载面,给出了塑性流动和损伤演化内变量的演化法则。将损伤力学和塑性力学结合起来,建立了应变驱动的应力-应变增量本构关系,给出了本构数值积分的要点。以单轴加载-卸载往复试验识别和校准了本构材料常数,并对单轴单调试验、单轴加载-卸载往复试验、二轴受压、二轴拉压试验和三轴受压试验进行了预测,并与试验结果作了比较,结果表明,所建本构模型对准脆性材料的非线性材料性能有良好的预测能力。  相似文献   

11.
IntroductionSincethepioneeringworksbyKachanov[1]andRabotnov[2 ]forcreepfailureofmetals,thedamagemechanicshasbeengreatlydevelopedandhasbecomeamostactiveresearcharea[3- 6 ].Thedescriptionofdamageconstitutiverelationsisabasicproblemofthedamagemechan ics.Thestrai…  相似文献   

12.
本文研究混凝土、岩石一类工程中常用的应变软化材料的有限元分析方法。在作者以往有关粘塑性损伤本构模型的工作基础上,给出了一组便于有限元计算的本构方程表达式。包括损伤弹性矩阵和局部损伤软化矩阵,分别运用于计算硬化和软化阶段的有限元刚度矩阵;对所提出的本构方程的实验验证计算和一些算例的有限元数值分析,表明文中给出的本构方程是可行的,相应的有限元算法能较好地对损伤固体的局部软化效应进行数值分析,并可成功地追踪应力应变响应的软化曲线  相似文献   

13.
基于应变等效性假说的损伤定义的适用条件   总被引:8,自引:0,他引:8  
研究了基于应变等效性假说的损伤定义方法,分析了定义中“材料损伤前后弹性模量”的物理含义。指出该方法只适用于间接描述弹(脆)性材料损伤行为,不能简单地用受荷过程中的“卸载模量”代替假说中的“受损弹性模量”来描述具有不可逆塑性变形特征的弹塑性损伤行为,否则将可能导致对损伤行为的误判。此外,本文给出了一种耦合塑性形变和损伤机制影响的弹塑性损伤定义。  相似文献   

14.
Closed-form constitutive relations are given for the prediction of the overall response of unidirectional fiber-reinforced composites having constituents that are elastoplastic materials. In these equations the damage mode of imperfect bonding between the fiber and matrix phases is incorporated. The interface decohesion is represented by two parameters that completely determine the degree of adhession at the interfaces in thenormal and tangential directions. Perfect contact, perfectly lubricated contact, and complete debonding are obtained as special cases. In the elastic region, the average stress-strain relations are given in terms of the effective elastic moduli of the damaged composite, all of which are given by closed-form expressions. The derived constitutive equations can be readily implemented for the analysis of metal matrix composites.  相似文献   

15.
大型水轮发电机推力轴承热弹流润滑性能分析   总被引:9,自引:1,他引:9  
以巴氏合金瓦和弹性金属塑料瓦推力轴承为例,介绍了大型水轮发电机推力轴承热弹性流体动力润滑性能的有限元分析方法。物理模型包括润滑油膜、推力轴承和镜板推力头,采用ADINA(T)程序计算水口巴氏合金瓦和三峡弹性金属塑料瓦推力轴承和镜板推力头的热弹性变形,并对轴承性能的计算结果和测量结果进行了对比分析。结果表明,计算结果和实测结果吻合。  相似文献   

16.
In this paper, a structural damage identification method (SDIM) is developed to identify the line crack-like directional damages generated within a cylindrical shell. First, the equations of motion for a damaged cylindrical shell are derived. Based on a theory of continuum damage mechanics, a small material volume containing a directional damage is represented by the effective orthotropic elastic stiffness, which is dependent of the size and the orientation of the damage with respect to the global coordinates. The present SDIM is then derived from the frequency response function (FRF) directly solved from the equations of motion of a damaged shell. In contrast with most existing SDIMs which require the modal parameters measured in both intact and damaged states, the present SDIM may require only the FRF-data measured at damaged state. By virtue of utilizing FRF-data, one may choose as many sets of excitation frequency and FRF measurement point as needed to acquire a sufficient number of equations for damage identification analysis. The numerically simulated damage identification tests are conducted to study the feasibility of the present SDIM.  相似文献   

17.
Stability criteria for crack propagation have been analysed which are based on the second law of thermodynamics. The isothermal case has been studied both for elastic and viscoelastic materials. The non-isothermal criteria have been considered with particular attention to a fast adiabatic loading process.The thermodynamic constitutive equations which are demanded and their relationships with the elastic energy have been analyzed.  相似文献   

18.
In this contribution various aspects of an anisotropic damage model coupled to plasticity are considered. The model is formulated within the thermodynamic framework and implements a strong coupling between plasticity and damage. The constitutive equations for the damaged material are written according to the principle of strain energy equivalence between the virgin material and the damaged material. The damaged material is modeled using the constitutive laws of the effective undamaged material in which the nominal stresses are replaced by the effective stresses. The model considers different interaction mechanisms between damage and plasticity defects in such a way that two-isotropic and two-kinematic hardening evolution equations are derived, one of each for the plasticity and the other for the damage. An additive decomposition of the total strain into elastic and inelastic parts is adopted in this work. The elastic part is further decomposed into two portions, one is due to the elastic distortion of the material grains and the other is due to the crack closure and void contraction. The inelastic part is also decomposed into two portions, one is due to nucleation and propagation of dislocations and the other is due to the lack of crack closure and void contraction. Uniaxial tension tests with unloadings have been used to investigate the damage growth in high strength steel. A good agreement between the experimental results and the model is obtained.  相似文献   

19.
Based on the elasto-plastic mechanics and continuum damage theory, a yield criterion related to spherical tensor of stress is proposed to describe the mixed hardening of damaged orthotropic materials. Its dimensionless form is isomorphic with the Mises criterion for isotropic materials. Furthermore, the incremental elasto-plastic damage constitutive equations and damage evolution equations are established. Based on the classical nonlinear plate theory, the incremental nonlinear equilibrium equations of orthotropic thin plates considering damage effect are obtained, and solved with the finite difference and iteration methods. In the numerical examples, the effects of damage evolution and initial deflection on the elasto-plastic postbuckling of orthotropic plates are discussed in detail.  相似文献   

20.
The structural theory of microdamage of homogeneous and composite materials is generalized. The theory is based on the equations and methods of the mechanics of microinhomogeneous bodies with stochastic structure. A single microdamage is modeled by a quasispherical pore empty or filled with particles of a damaged material. The accumulation of microdamages under increasing loading is modeled as increasing porosity. The damage within a single microvolume is governed by the Huber-Mises or Schleicher-Nadai failure criterion. The ultimate strength is assumed to be a random function of coordinates with power-law or Weibull one-point distribution. The stress-strain state and effective elastic properties of a composite with microdamaged components are determined using the stochastic equations of elasticity. The equations of deformation and microdamage and the porosity balance equation constitute a closed-form system of equations. The solution is found iteratively using conditional moments. The effect of temperature on the coupled processes of deformation and microdamage is taken into account. Algorithms for plotting the dependences of microdamage and macrostresses on macrostrains for composites of different structure are developed. The effect of temperature and strength of damaged material on the stress-strain and microdamage curves is examined __________ Translated from Prikladnaya Mekhanika, Vol. 43, No. 6, pp. 3–42, June 2007.  相似文献   

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