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Plastic buckling of thin hemispherical shell subjected to concentrated load at the apex

机译:半球形薄壳的塑性屈曲在顶点处承受集中载荷

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This study presents the analytical, numerical, and experimental results of thin hemispherical metal shells into the plastic buckling range illustrating the importance of geometry changes on the buckling load. The hemispherical shell is rigidly supported around the base circumference against horizontal and vertical translation and the load is vertically applied by a rigid cylindrical boss at the apex. Kinematics stages of initial buckling and subsequent propagation of plastic deformation for rigid-perfectly plastic shells are formulated on the basis of Drucker-Shield's limited interaction yield condition. The effect of the radius of the boss, used to apply the loading, on the initial and subsequent collapse load is studied. In the numerical model, the material is assumed to be isotropic and linear elastic perfectly plastic without strain hardening obeying the Tresca or Von Mises yield criterion. Both axisymmmetric and 3D models are implemented in the numerical work to verify the presence of non-symmetric deformation modes in the case of thin shells. In the end, the results of the analytical solution are compared and verified with the numerical results using ABAQUS software and experimental findings. Good agreement is observed between the load-deflection curves obtained using three different approaches. A secondary bifurcation point is detected in thin shells in which the deformation degenerates from symmetric to non-symmetric behavior. The bifurcation point depends on the (R/t_o) ratio and the material parameters.
机译:这项研究提出了在塑料屈曲范围内的半球形薄金属壳的分析,数值和实验结果,说明了几何形状变化对屈曲载荷的重要性。半球形壳体被牢固地支撑在基部圆周周围,以抵抗水平和垂直平移,并且载荷由顶点处的刚性圆柱状凸起垂直施加。在Drucker-Shield有限的相互作用屈服条件的基础上,提出了刚度完美的塑料壳的初始屈曲和随后塑性变形传播的运动学阶段。研究了用于施加载荷的凸台半径对初始和后续坍塌载荷的影响。在数值模型中,假定材料为各向同性且线性弹性完美的塑料,没有遵循Tresca或Von Mises屈服准则的应变硬化。在数值研究中同时实现了轴测线和3D模型,以验证薄壳情况下是否存在非对称变形模式。最后,使用ABAQUS软件和实验结果将分析溶液的结果与数值结果进行比较和验证。使用三种不同方法获得的载荷-挠度曲线之间观察到良好的一致性。在薄壳中检测到第二个分叉点,其中变形从对称行为退化为非对称行为。分叉点取决于(R / t_o)比和材料参数。

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