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计及不确定性参数的单约束输流管道固有特性分析

NATURAL CHARACTERISTICS OF A SINGLE CONSTRAINT PIPE CONVEYING FLUID WITH UNCERTAIN PARAMETERS

  • 摘要: 研究了参数不确定性对单约束输流管道系统固有特性的影响. 基于广义哈密顿原理得到了单约束两端固支输流管道的动力学方程和边界条件. 为更贴近工程实际中普遍存在的参数不确定性, 根据区间分析理论建立了考虑区间不确定参数的单约束输流管道动力学方程. 采用基于Lagrange代理模型的不确定性方法得到了计及不确定参数的单约束输流管道固有频率区间上下边界. 通过与扫描法的结果进行对比, 验证了基于Lagrange代理模型的不确定性方法结果的正确性. 详细讨论了卡箍位置、流速、卡箍的线性刚度和扭转刚度等参数的不确定性对输流管道系统固有频率的影响. 研究结果表明, 随着不确定性参数偏差系数的增大, 卡箍位置、流速及刚度参数的不确定性导致前四阶固有频率区间变宽, 其中卡箍位置的影响显著. 对于不同卡箍位置而言, 当不确定性卡箍位置的中值点位于管道的0.5 m和0.3 m处时, 随着偏差系数的增大, 前四阶固有频率区间上下边界呈现非单调非线性变化; 而中值点位于管道0.1 m处时, 前四阶固有频率区间呈现单调线性变化.

     

    Abstract: This paper investigates the effects of parameter uncertainties on the natural characteristics of a fluid-conveying pipe system with a single clamp constraint. Based on the generalized Hamilton principle, the dynamic equations and boundary conditions of a fluid-conveying pipe clamped at both ends and constrained by a single clamp are derived. To better reflect the parameter uncertainties commonly presented in engineering practice, the dynamic equations with interval uncertainties are established by the interval analysis theory. The upper and lower bounds of the natural frequency intervals of the single-clamped fluid-conveying pipe considering uncertain parameters are obtained using the uncertain analysis method based on the Lagrange surrogate model. The accuracy of the proposed method is verified by comparison with results obtained from the scanning method. The effects of uncertainties in parameters such as the clamp position, fluid speed, linear stiffness, and torsional stiffness of the clamp on the natural frequencies of the pipe system are discussed in detail. The results show that with increasing coefficient of variation of the uncertain parameters, the intervals of the first four natural frequencies become wider, with the clamp position having the significant effect. For different clamp positions, when the median value of the uncertain clamp position is located at 0.5 m and 0.3 m along the pipe, the upper and lower bounds of the first four natural frequency intervals exhibit non-monotonic and nonlinear variation as the coefficient of variation increases. In contrast, when the median value is located at 0.1 m, the intervals of the first four natural frequencies exhibit monotonic and linear variation.

     

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