用有限元方法模拟冰雪环境中声波的传播和混响

B. Simon, M. Isakson, M. Ballard
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引用次数: 6

摘要

建立了一个三维、纵向不变的冰覆盖浅水波导中声传播和混响的有限元模型。冰被建模为弹性介质和压力释放表面。计算并比较了冰的两种表现形式的传输损耗水平。使用傅立叶合成,频域声压结果被转换到时域,然后比较冰的两种表现形式的混响水平。时域结果显示了在频域中未捕获的每个冰表示之间的差异。最后,对这些模式差异提出了一些可能的解释,包括冰-水界面的压缩-剪切波转换和冰的陡入射角散射。建立了一个三维、纵向不变的冰覆盖浅水波导中声传播和混响的有限元模型。冰被建模为弹性介质和压力释放表面。计算并比较了冰的两种表现形式的传输损耗水平。使用傅立叶合成,频域声压结果被转换到时域,然后比较冰的两种表现形式的混响水平。时域结果显示了在频域中未捕获的每个冰表示之间的差异。最后,对这些模式差异提出了一些可能的解释,包括冰-水界面的压缩-剪切波转换和冰的陡入射角散射。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Modeling acoustic wave propagation and reverberation in an ice covered environment using finite element analysis
A three-dimensional, longitudinally invariant, finite element model of acoustic propagation and reverberation in an ice-covered shallow water waveguide has been developed. The ice is modeled as both an elastic medium and a pressure release surface. Transmission loss levels are calculated and compared for both representations of ice. Using Fourier synthesis, the frequency-domain acoustic pressure results are transformed into the time domain, and reverberation levels are then compared for both representations of ice. The time-domain results show differences between each ice representation that are not captured in the frequency domain. Finally, some possible explanations are presented for these model differences, including compressional-to-shear wave conversion at the ice-water interface and steep incident angle scattering from the ice.A three-dimensional, longitudinally invariant, finite element model of acoustic propagation and reverberation in an ice-covered shallow water waveguide has been developed. The ice is modeled as both an elastic medium and a pressure release surface. Transmission loss levels are calculated and compared for both representations of ice. Using Fourier synthesis, the frequency-domain acoustic pressure results are transformed into the time domain, and reverberation levels are then compared for both representations of ice. The time-domain results show differences between each ice representation that are not captured in the frequency domain. Finally, some possible explanations are presented for these model differences, including compressional-to-shear wave conversion at the ice-water interface and steep incident angle scattering from the ice.
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