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1.
The angular distribution functions of HRR singularity fields are analyzed via conservation integrals. Two functional equations are proved for the angular distribution functions and can be used for their solutions. The detailed forms of the functional equations and the final governing equations for solutions are given for the cases of plane strain and plane stress. Accurate numerical results are also given for some typical parameters and the equivalence of different governing equations is proved.  相似文献   

2.
Functional grading of rubber-like materials is suggested as a means of controlling their mechanical response within the context of finite thermoelasticity. To illustrate the concept of functional grading, we consider the axial shearing deformation of a radially heated, isotropic, incompressible, hollow rubber tube. The temperature stiffening, the strain stiffening, and the radially varying shear modulus of rubber tubes are modeled here by generalizing the Neo-Hookean and the Gent models. Local energy and momentum balance equations are solved to obtain the temperature and stress–strain fields in the sheared tube. The shear strain becomes highly inhomogeneous with an increase in temperature gradient, whereas functional grading of the tube can perfectly homogenize the strain. This paper indicates the potential of functionally grading rubbers to control their mechanical response in thermally hostile environments.  相似文献   

3.
The stability of equilibrium of non-linearly elastic rods, whose deformations obey the classical Kirchhoff’s equations, is considered. A variational formulation of the equilibrium problem is given, and the equilibrium equations for infinitesimal deformations superimposed to a finite transformation of a rod are deduced. The stability of annular rings, in which the twisting strain is non-null, is investigated by study of the second variation of the energy functional.  相似文献   

4.
Taking the strain tensor, the scalar damage variable, and the damage gradient as the state variables of the Helmholtz free energy, the general expressions of the firstorder gradient damage constitutive equations are derived directly from the basic law of irreversible thermodynamics with the constitutive functional expansion method at the natural state. When the damage variable is equal to zero, the expressions can be simplified to the linear elastic constitutive equations. When the damage gradient vanishes, the expressions can be simplified to the classical damage constitutive equations based on the strain equivalence hypothesis. A one-dimensional problem is presented to indicate that the damage field changes from the non-periodic solutions to the spatial periodic-like solutions with stress increment. The peak value region develops a localization band. The onset mechanism of strain localization is proposed. Damage localization emerges after damage occurs for a short time. The width of the localization band is proportional to the internal characteristic length.  相似文献   

5.
The viscoelastic relaxation modulus is a positive-definite function of time. This property alone allows the definition of a conserved energy which is a positive-definite quadratic functional of the stress and strain fields. Using the conserved energy concept a Hamiltonian and a Lagrangian functional are constructed for dynamic viscoelasticity. The Hamiltonian represents an elastic medium interacting with a continuum of oscillators. By allowing for multiphase displacement and introducing memory effects in the kinetic terms of the equations of motion a Hamiltonian is constructed for the visco-poroelasticity.
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6.
Summary The presented method to identify material parameters for inelastic deformation laws is based on the numerical analysis of inhomogeneous stress and strain fields received from suitable experiments. Tensile and bending tests were carried out to obtain elastic and hardening parameters. The deformation law for small elasto-plastic strains is presented as a system of nonlinear differential and algebraic equations (DAE) consisting of the stress–strain relation, evolution equations for the internal variables and the yield condition. Different rules for the evolution equations of isotropic, kinematic and distorsional hardening are proposed. The DAE are discretized using an implicit Euler method, and the resulting system of nonlinear algebraic equations is solved using the Newton method. Deterministic optimization procedures are preferred to identify material parameters from a least-squares functional of numerical and measured comparative quantities. The gradient of the objective function was calculated using a semianalytical sensitivity analysis. Due to measurement errors, the optimal sets of material parameters are non unique. The approximate estimation of confidence regions and the calculation of correlation coefficients is presented. The results of several optimization processes for material parameters of elasto-plastic deformation laws show a good agreement between measured and calculated values, but they show also problems which may occur if systematic errors will not be recognized and deleted. Received 30 September 1999; accepted for publication 8 March 2000  相似文献   

7.
The constitutive equations of motion of an elastic medium with given initial stresses are formulated in the form of a hyperbolic system of first order differential equations. Equations describing the propagation of small perturbations in a prestressed isotropic medium with an arbitrary dependence of the elastic strain energy on the strain tensor are derived, and equations for the quadratic dependence of elastic strain energy on the strain tensor are given.  相似文献   

8.
将正交曲线坐标下的格林应变张量引入到薄壳大变形分析,通过建立恰当的基本假设,直接导出了用格林应变张量表示的壳体变形几何方程,将该方程代入到本构方程,由能量原理得到了小应变非线性变形平衡方程、内力方程和边界条件,在此基础上提出了大应变变形的简化分析方法.文中导得的方程涵盖薄板壳大、小变形的全部方程,推导过程简捷、系统,所得结果规则、清晰,与此前有关分析方法的结果完全吻合.  相似文献   

9.
10.
在非局部弹性理论框架下对平面应变和平面应力状态重新界定.首先,分别在其相应简化假设下推导控制方程,并与经典局部情况进行比较.然后,引入变形协调条件对两类非局部平面问题的精确性进行讨论.其中,对于非局部平面应力状态,通过应变协调方程的Fourier变换形式来进行研究,使问题得以简化.通过以上分析,最终得到一些有价值的结论.  相似文献   

11.
For finite strain dynamics a variational model of crack evolution is formulated within the generalized oriented continuum methodology. In this approach position- and direction-dependent deformation and strain measures are used to describe the (macro)motion of the body with defects, which may evolve relative to the moving body. The inelastic behaviour of continua with evolving defects is represented by phenomenological equations including the transversal crack evolution. A strain-induced crack propagation criterion is defined by the difference between the strain energy release rate and the rate of the surface energy of the crack. A possible nucleation of microcracks in terms of the average drag coefficient of the crack configuration is proposed. Based on the crack growth criterion presented in this paper, the kinking of cracks is investigated using variational concepts. A constitutive damage model of Kachanov's type accounting for the crack density is derived in terms of the free energy functional and a dissipation potential.  相似文献   

12.
Viscoelastic constitutive equations are constructed by assuming that the stress is a nonlinear function of the current strain and of a set of internal variables satisfying relaxation equations of fractional order. The dependence of the relaxation equations on the strain can also be nonlinear. The resulting constitutive equations are examined as mapping between appropriate Sobolev spaces. The proposed formulation is easier to implement numerically than history-based formulations.   相似文献   

13.
Beltrami-Mitchell equations for non-linear elasticity theory are derived using the first Piola-Kirchhoff stress and the deformation gradient tensors as field variables so as to yield linear equilibrium and compatibility equations, respectively. In the derivation it is assumed that a strain energy density and, correspondingly, a complementary strain energy density exist, and satisfy the axiom of objectivity. Substitution for the deformation gradient in the compatibility equations yields non-linear differential equations in terms of the first Piola-Kirchhoff stress tensor which may be regarded as the Beltrami-Mitchell equations of non-linear elasticity. The equations are also derived for “semi-linear” isotropic elastic materials and the theory is illustrated by three simple examples.  相似文献   

14.
In this brief note we consider an elastic-plastic material whose strain energy depends not only on the plastic strain but also on spatial gradient. The governing equations of motion are obtained by maximizing the rate of global energy dissipation. The resulting differential equations are specialized for the case where the strain energy depends only upon the density of geometrically necessary dislocations.  相似文献   

15.
针对导弹适配器的结构特征,分别建立了可压缩橡胶泡沫和不可压橡胶圆筒轴对称平面应变问题有限变形的平衡方程,基于Blatz-Ko应变能函数和三次缩减多项式应变能函数,得到了相应的位移和应力模式;在此基础上求解了适配器受压问题的非线性方程组和导弹发射时适配器所受到的摩擦力.算例分析与有限元数值模拟比较表明:解析解与数值解非常吻合,径向应力在发射筒内外表面误差最大为0.558%,周向应力在粘合面误差最大为0.246%,导弹发射时的最大量纲为一的摩擦力为1.0228.适配器径向应力在材料粘合交界面上最小,在适配器外表面最大,均为压应力;橡胶泡沫和不可压橡胶的周向应力均为压应力,橡胶泡沫的周向应力由内向外变大,不可压橡胶的周向应力由内向外变小.橡胶泡沫的径向受压大于周向受压,不可压橡胶的周向受压大于径向受压.研究不同过盈量对应力和摩擦力的影响表明:过盈量每增加0.0013,橡胶泡沫 层和不可压橡胶层的径向应力约增加0.13,不可压橡胶层的周向应力约增加2.14,而摩擦力约增加0.22.过盈量对不可压橡胶层的周向应力和导弹所受到的摩擦力影响非常大,对橡胶泡沫的径向应力有一定的影响,周向应力变化很小.  相似文献   

16.
The problem considered is that of determining the maximum strain produced in a linearly elastic falling horizontal wire by the instantaneous arrest of its ends at time t=0, and the time t1 at which this maximum strain occurs. An upper bound estimate of the maximum strain, based on conservation of energy, is easily obtained if one assumes that the wire attains an extreme configuration completely devoid of kinetic energy, as in a standing wave vibration. In the present paper, however, a more accurate approach is employed. The partial differential equations are first written governing the velocity v and slope s as functions of position x and time t. These equations (which are non-linear because the time-varying tension in the wire is a functional of the slopes) are then solved numerically by the method of characteristics. To facilitate the numerical solution, a separate analysis is made of the behavior of v and s near the ends of the wire for small t.  相似文献   

17.
各向同性率无关材料本构关系的不变性表示   总被引:2,自引:1,他引:1  
陈明祥 《力学学报》2008,40(5):629-635
在内变量理论的框架下,针对各向同性率无关材料,使用张量函数表示理论建立了塑性应变全量及增量本构关系的最一般的张量不变性表示. 它们均由3个完备不可约的基张量组合构成,这3个基张量分别是应力的零次幂、一次幂和二次幂. 因此得出,塑性应变、塑性应变增量与应力三者共主轴. 通过对基张量的正交化,给出了本构关系式在主应力空间中的几何解释. 进一步,全量(或增量)本构关系中3个组合因子被表达为应力、塑性应变(或塑性应变增量)的不变量的函数. 当塑性应变(或塑性应变增量)的3个不变量之间满足一定关系时,所给出的本构关系将退化为经典的形变理论(或塑性势理论).最后,还讨论它与奇异屈服面理论的关系,当满足一定条件时,两者是一致的.   相似文献   

18.
The problem of determining the stress—strain state of a multilayered shell is solved. It is assumed that the layer material is nonlinearly elastic and the strain—displacement relations are nonlinear. The displacements are expanded in terms of the functions of transverse coordinate that contain unknown parameters. The governing equations are derived with the use of the Lagrange variational principle. A technique for minimizing the energy functional is proposed. An example of a three–layered beam is considered, calculation results are compared with the exact solution, and the specific features of the approach proposed are analyzed.  相似文献   

19.
This paper is concerned with a constrained theory of shells in the presence of small strain accompanied by moderate rotation. The constrained theory accounts for the effect of transverse normal strain and includes, of course, the special case (corresponding to the Kirchhoff-Love theory of shells) in which the effect of transverse normal strain is absent. After precise estimates for (local) moderate rotation and relative displacement gradients in terms of infinitesimal strain have been effected, a complete theory is formulated with the use of linear constitutive equations. The nature of the complete theory is further examined when initially the shell-like body is a plate; and it is shown that our kinematical formulae (strain-displacement relations), as well as the relevant differential equations of the theory in the absence of the effect of transverse normal strain, systematically reduce to those used in the von Kármán plate equations. Also, in the light of the present results, an assessment of kinematical aspects of previously developed theories of shells undergoing small strain and moderate rotation is indicated.  相似文献   

20.
The theory of defects in Cosserat continua is sketched out in strict analogy to the theory of line defects in anisotropic elasticity (Stroh theory). This rewrite of the second order equilibrium equations of elasticity in a 3-dimensional space as first order equations in a 6-dimensional space is analogous to replacing the Laplace equation by the Riemann–Cauchy equations. For generalized plane strain of anisotropic micropolar (Cosserat) elasticity one obtains a 14-dimensional coupled linear system of differential equations of first order and for plane strain of anisotropic micropolar (Cosserat) elasticity we obtain a 6-dimensional coupled linear system of differential equations of first order.  相似文献   

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