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首页> 外文期刊>Journal of Fluids and Structures >Nonlinear vibrations of fluid-filled clamped circular cylindrical shells
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Nonlinear vibrations of fluid-filled clamped circular cylindrical shells

机译:充液夹紧圆柱壳的非线性振动

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摘要

In this study, the nonlinear vibrations are investigated of circular cylindrical shells, empty or fluid-filled, clamped at both ends and subjected to a radial harmonic force excitation. Two different theoretical models are developed. In the first model, the standard form of the Donnell's nonlinear shallow-shell equations is used; in the second, the equations of motion are derived by a variational approach which permits the inclusion of constraining springs at the shell extremities and taking in-plane inertial terms into account. In both cases, the solution includes both driven and companion modes, thus allowing for a travelling wave in the circumferential direction; they also include axisymmetric modes to capture the nonlinear inward shell contraction and the correct type (softening) nonlinear behaviour observed in experiments. In the first model, the clamped beam eigenfunctions are used to describe the axial variations of the shell deformation, automatically satisfying the boundary conditions, leading to a 7 degree-of-freedom (dof) expansion for the solution. In the second model, rotational springs are used at the ends of the shell, which when large enough reproduce a clamped end; the solution involves a sine series for axial variations of the shell deformation, leading to a 54 dof expansion for the solution. In both cases the modal expansions satisfy the boundary conditions and the circumferential continuity condition exactly. The Galerkin method is used to discretize the equations of motion, and AUTO to integrate the discretized equations numerically. When the shells are fluid-filled, the fluid is assumed to be incompressible and inviscid, and the fluid-structure interaction is described by linear potential flow theory. The results from the two theoretical models are compared with existing experimental data, and in all cases good qualitative and quantitative agreement is observed.
机译:在这项研究中,研究了两端被夹紧并受到径向谐波力激励的空的或充满流体的圆柱壳的非线性振动。建立了两种不同的理论模型。在第一个模型中,使用了Donnell非线性浅壳方程的标准形式。在第二种方法中,运动方程是通过变分方法得出的,该方法允许在壳的末端包括约束弹簧并考虑平面内惯性项。在这两种情况下,解决方案都包括驱动模式和伴随模式,因此允许在圆周方向上传播。它们还包括轴对称模式,以捕获非线性向内壳收缩和在实验中观察到的正确类型(软化)非线性行为。在第一个模型中,夹紧梁的本征函数用于描述壳体变形的轴向变化,自动满足边界条件,从而导致解的7自由度(dof)扩展。在第二种模型中,在壳体的端部使用了旋转弹簧,当弹簧足够大时,会产生一个夹紧的端部。该解决方案涉及一个用于壳体变形轴向变化的正弦序列,从而导致该解决方案扩展了54自由度。在这两种情况下,模态展开都精确地满足边界条件和周向连续性条件。 Galerkin方法用于离散化运动方程,AUTO用于数字化离散化方程。当壳体充满流体时,假定流体不可压缩且不粘稠,并且通过线性势流理论描述了流固耦合。将两个理论模型的结果与现有的实验数据进行比较,并且在所有情况下都观察到良好的定性和定量一致性。

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