Laboratoire Ondes et Acoustique, Institut Langevin, University Paris 7, Ecole Supérieure de Physique et de ChimieIndustrielles de la Ville de Paris, Centre National de la Recherche Scientifique UMR 7587, Paris, France.
IEEE Trans Ultrason Ferroelectr Freq Control. 2010 Aug;57(8):1804-12. doi: 10.1109/TUFFC.2010.1618.
The acoustic guided wave propagation for plate thickness measurement is generally treated in free space to simplify the formal approach. In this paper, propagation in a closed environment is treated by dealing with plates of finite dimensions and arbitrary geometries and linear boundary conditions. The present approach considers the plate Green's function to be composed of two terms. The first term corresponds to the Green's function of an infinite plate. The second term corresponds to a correction term which, in addition to the first term, satisfies all equations. Assuming the boundary conditions to be linear, it is found that the acoustic wave generated by a point source is proportional to that of a circular array of sources centered on it. By measuring the ratio between the two signals, either the plate velocity or plate thickness can be determined. This new method has been successfully applied to isotropic and anisotropic homogeneous plates of different geometries, on inhomogeneous plates, and also in a passive mode, without an active transmitter.
板厚测量中的声导波传播通常在自由空间中进行处理,以简化形式方法。本文通过处理具有任意几何形状和线性边界条件的有限尺寸板来处理封闭环境中的传播。本方法考虑将板格林函数由两个项组成。第一项对应于无限板的格林函数。第二项对应于校正项,除了第一项外,该校正项还满足所有方程。假设边界条件是线性的,发现由点源产生的声波与位于其中心的圆形源的圆形阵列产生的声波成比例。通过测量两个信号之间的比值,可以确定板的速度或厚度。这种新方法已成功应用于不同几何形状的各向同性和各向异性均匀板、非均匀板以及无源模式,无需有源发射器。