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An Inverse Method to Measure the Flexural Wave Properties of a Beam

机译:测量梁弯曲波特性的逆方法

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This paper describes an inverse method to measure the complex flexural wavenumber and wave propagation coefficients of a beam undergoing transverse motion. The formulation begins with the Bernoulli-Euler partial differential beam equation solved in terms of spatial trigonometric functions multiplied by a temporal harmonic response term. The resulting model is a nonlinear expression, which has five unknowns that consist of four wave propagation coefficients and the flexural wavenumber, and is written so that it is equal to data from seven equally spaced measurement locations on the beam. These equations, which are functions of the unknown parameters, are then inverted so that the unknowns become functions of the data. This operation allows the invevse method to be linear with respect to the beam parameters, yielding closed-form estimations. The method is independent of boundary conditions as it depends only on the measurements. An experiment is conducted in which a rectangular aluminum beam is vibrated transversely on a shaker table, with accelerometers recording the beam response data at the seven locations. The data were combined to estimate the flexural wavenumber, which was compared to a modeled wavenumber using assumed material properties for the beam, resulting in a very favorable comparison. Next, the wave propagation coefficients were estimated, although no comparison was made to the model because these coefficients depend on boundary conditions that are difficult to determine. Finally, the experimental response at a beam location is compared to a modeled response using the estimated parameters.
机译:本文介绍了一种逆方法,用于测量横向运动的梁的复杂弯曲波数和波传播系数。该公式从以空间三角函数乘以时间谐波响应项的形式求解的伯努利-欧拉偏微分方程开始。生成的模型是一个非线性表达式,它具有五个未知数,这些未知数由四个波传播系数和弯曲波数组成,并且被编写为等于来自波束上七个等间隔测量位置的数据。然后将这些作为未知参数的函数的方程式求反,以使未知数成为数据的函数。此操作使invevse方法相对于光束参数是线性的,从而产生封闭形式的估计。该方法与边界条件无关,因为它仅取决于测量。进行了一个实验,其中矩形铝梁在振动台上横向振动,加速度计在七个位置记录梁的响应数据。组合数据以估计弯曲波数,使用假定的梁材料特性将其与模拟波数进行比较,从而得到非常有利的比较。接下来,尽管没有对模型进行比较,但估计了波传播系数,因为这些系数取决于难以确定的边界条件。最后,使用估计的参数将光束位置的实验响应与模型响应进行比较。

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