弹性介质中任意形状细长曲梁的Cosserat模型

COSSERAT MODELING OF THIN-LONG CURVE BEAMS WITH ARBITRARY SHAPE IN ELASTIC MEDIUM

  • 摘要: Kirchhoff动力学比拟理论使动力学的概念和方法进入弹性杆力学的研究领域。Cosserat弹性杆模型考虑Kirchhoff模型所忽略的截面剪切变形、中心线伸缩变形和分布载荷等因素,更适合工程中大变形细长梁的动力学建模。该文以弹性介质中任意形状中心线的圆截面细长曲梁为对象,基于Cosserat模型建立以截面的姿态角和挠度为未知变量的精确动力学方程。其直梁小变形特例为弹性介质中的Timoshenko梁。将Lyapunov运动稳定性理论的时间变量置换为空间变量,可用于判断梁的平衡稳定性。以弹性介质中轴向受压Timoshenko梁为例,讨论梁平衡状态的Lyapunov稳定性与欧拉失稳传统概念之间的区别和相互联系。导致梁屈曲的欧拉载荷可利用满足Lyapunov稳定性梁的受扰挠性线和端部约束条件导出。在一次近似条件下证明空间域内的Lyapunov 稳定性和欧拉稳定性是时间域内的Lyapunov稳定性的必要条件。

     

    Abstract: According to Kirchhoff’s kinetic analogy, the concepts and approaches of dynamics can be applied to mechanics of elastic rods. The Cosserat model of elastic rods considers factors neglected by the Kirchhoff model, such as the cross-sectional shear deformation, the tensile deformation of rod centerline and loadings, and therefore is more suitable to the modeling of thin-long beams with large deformation. In this study, the Cosserat model is applied to establish the exact dynamic equations of a thin-long curve beam with circular cross sections and an arbitrary shape of centerline. The attitude angles of rod cross sections and deflections of the centerline are selected as unknown variables. The Timoshenko beam in elastic medium represents the special case with beam of a straight centerline and small deformation. The Lyapunov’s stability theory is applied to analyze the equilibrium status of the beam when temporal variables are replaced by spatial variables. The stability of a Timoshenko beam in elastic medium subject to axial compression is analyzed to identify the difference and relationship between Lypunov’s stability and the traditional Euler’s buckling theory. The Euler’s load is obtained by using the perturbed centerline of the beam satisfying constraint conditions on beam ends when the Lyapunov’s stability conditions are satisfied. It is proven that the Lyapunov’s and Euler’s stability conditions in the spatial domain are the necessary conditions of Lyapunov’s stability in the time domain in the sense of the first-order approximation.

     

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