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NONSYMMETRIC CAVITY FORMATION AT A CIRCULAR INCLUSION UNDER REMOTE EQUIBIAXIAL LOAD

机译:圆弧形夹杂在非等轴对称载荷下的非对称空洞形成

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This paper examines the phenomenon of cavity formation through an analysis of the problem of a plane circular elastic inclusion embedded in an unbounded elastic matrix subject to a remote equibiaxial load. Consistent with infinitesimal strain kinematics, nonlinear behavior is confined to a cohesive zone so that inclusion-matrix interaction is characterized by a nonlinear interface force-interface separation law requiring a characteristic length for its prescription. Equilibrium solutions for both rotationally symmetric and nonsymmetric cavity shapes are sought based on an integral equation formulation together with known elasticity solutions for circular domains. For values of remote load, interface strength and elastic moduli within certain bounds only rotationally symmetric cavities occur under decreasing characteristic length-inclusion radius ratio. At other parameter values the existence of nonsymmetric cavities is studied by performing a linearized bifurcation analysis about the rotationally symmetric equilibrium state. A post bifurcation analysis is carried out by reducing the governing integral equations to a truncated set of nonlinear algebraic equations and analysing those. Stability of equilibrium states is assessed with the Hadamard stability definition. Calculations for the interfacial tractions are carried out as well. The study reveals that rotationally symmetric cavities must give way to the abrupt formation of stable nonsymmetric cavities when the interface force attains its maximum value. Thus, the phenomenon of ductile decohesion, or the gradual opening of a cavity coincident with an unloading of the interface, cannot occur (for the system being studied) without artificially constraining the inclusion against rigid displacement. [References: 26]
机译:本文通过分析平面圆形弹性夹杂物嵌入无边界弹性基体中承受远等双轴载荷的问题,研究了空洞形成的现象。与无穷小应变运动学一致,非线性行为被限制在一个内聚区,因此包含-基体相互作用的特征在于非线性界面力-界面分离定律,要求其特征长度。基于积分方程公式以及圆域的已知弹性解,寻求旋转对称和非对称腔体形状的平衡解。对于一定范围内的远程载荷,界面强度和弹性模量,只有在减小特征长度-夹杂半径比的情况下才会出现旋转对称的空腔。在其他参数值下,通过对旋转对称的平衡态执行线性化的分叉分析,研究非对称腔的存在。通过将控制积分方程简化为一组截断的非线性代数方程并进行分析,可以进行分叉后分析。用Hadamard稳定性定义评估平衡态的稳定性。还进行了界面牵引力的计算。研究表明,当界面力达到最大值时,旋转对称腔必须让位于稳定的非对称腔的突然形成。因此,在没有人为地限制夹杂物抵抗刚性位移的情况下,就不会发生延性的内聚现象,或者与界面卸载同时发生的空腔逐渐打开的现象。 [参考:26]

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