可穿透楔形波导的三维解析解和数值解

Yang Chunmei, Lyu Liangang, Q. Fangli, Luo Wenyu
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引用次数: 1

摘要

本文首次给出了可穿透楔形海洋中由点源激发的三维声传播的精确解析解。虽然Deane和Buckingham已经提出了可穿透楔体水中声场的解析解(Journal of acoustic Society of America, 1993,93(3): 1319~1328),但解析解并不完整。它只适用于海水,不适用于海床,以下称为底部。本文提出了一种既适用于海水也适用于海底的解析场解。采用源图像法得到了解析解。对于可穿透楔体的水中声场,只需考虑声反射。以楔形顶点为中心的圆上的所有源图像都需要参与计算。然而,对于可穿透楔形底部的声场,需要同时考虑声反射和声折射。只有位于半圆底部上方的源图像需要参与计算。基于平面波反射和折射原理,可以得到整个海域的解析解。此外,还提出了基于波数积分法的三维数值模型,并以无条件稳定的直接全局矩阵耦合模式方法实现。然后,将三维数值模型应用于基准楔形波导中点源激励下的声音传播。三维模型的数值解与基准楔形波导的解析解吻合较好。因此,通过基准楔问题的解析解,验证了该三维模型的有效性。
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Three-dimensional analytical solution and numerical solution in a penetrable wedge-shaped waveguide
An exact analytical solution for three-dimensional sound propagation excited by a point source in a penetrable wedge-shaped ocean is first presented in this paper. Although Deane and Buckingham have proposed an analytical solution for the acoustic field in the water of a penetrable wedge (Journal of the Acoustical Society of America, 1993, 93(3): 1319~1328), the analytical solution is not complete. It is only applicable for sea water not for the seabed, hereafter called bottom. This paper presents an analytical field solution which not only applies to sea water but also the bottom. The analytical solution is obtained by using the method of source images. For the acoustic field in the water of a penetrable wedge, only acoustic reflection needs to be considered. All the source images on a circle centered on the wedge apex need to be involved in the computation. However, for the acoustic field at the bottom of a penetrable wedge, both acoustic reflection and acoustic refraction need to be considered. Only the source images above the bottom on a semicircle need to be involved in the computation. The analytical solution in the whole sea area can be obtained based on the plane wave reflection and refraction principles. In addition, a three-dimensional numerical model based on the wavenumber integration method is also presented and implemented in an unconditionally stable direct-global-matrix coupled-mode method. Afterwards, the three-dimensional numerical model is applied to sound propagation excited by a point source in a benchmark wedge waveguide. The numerical solutions from the three-dimensional model agree well with the analytical solutions in the benchmark wedge waveguide. Consequently, the present three-dimensional model is validated through the analytical solutions to the benchmark wedge problem.
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