Equations for finite-difference, time-domain simulation of sound propagation in moving inhomogeneous media and numerical implementation
Finite-difference, time-domain (FDTD) calculations are typically performed with partial differential equations that are first order in time. Equation sets appropriate for FDTD calculations in a moving inhomogeneous medium (with an emphasis on the atmosphere) are derived and discussed in this paper....
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Veröffentlicht in: | The Journal of the Acoustical Society of America 2005-02, Vol.117 (2), p.503-517 |
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creator | OSTASHEV, Vladimir E WILSON, D. Keith LANBO LIU ALDRIDGE, David F SYMONS, Neill P MARLIN, David |
description | Finite-difference, time-domain (FDTD) calculations are typically performed with partial differential equations that are first order in time. Equation sets appropriate for FDTD calculations in a moving inhomogeneous medium (with an emphasis on the atmosphere) are derived and discussed in this paper. Two candidate equation sets, both derived from linearized equations of fluid dynamics, are proposed. The first, which contains three coupled equations for the sound pressure, vector acoustic velocity, and acoustic density, is obtained without any approximations. The second, which contains two coupled equations for the sound pressure and vector acoustic velocity, is derived by ignoring terms proportional to the divergence of the medium velocity and the gradient of the ambient pressure. It is shown that the second set has the same or a wider range of applicability than equations for the sound pressure that have been previously used for analytical and numerical studies of sound propagation in a moving atmosphere. Practical FDTD implementation of the second set of equations is discussed. Results show good agreement with theoretical predictions of the sound pressure due to a point monochromatic source in a uniform, high Mach number flow and with Fast Field Program calculations of sound propagation in a stratified moving atmosphere. |
doi_str_mv | 10.1121/1.1841531 |
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The second, which contains two coupled equations for the sound pressure and vector acoustic velocity, is derived by ignoring terms proportional to the divergence of the medium velocity and the gradient of the ambient pressure. It is shown that the second set has the same or a wider range of applicability than equations for the sound pressure that have been previously used for analytical and numerical studies of sound propagation in a moving atmosphere. Practical FDTD implementation of the second set of equations is discussed. 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The first, which contains three coupled equations for the sound pressure, vector acoustic velocity, and acoustic density, is obtained without any approximations. The second, which contains two coupled equations for the sound pressure and vector acoustic velocity, is derived by ignoring terms proportional to the divergence of the medium velocity and the gradient of the ambient pressure. It is shown that the second set has the same or a wider range of applicability than equations for the sound pressure that have been previously used for analytical and numerical studies of sound propagation in a moving atmosphere. Practical FDTD implementation of the second set of equations is discussed. Results show good agreement with theoretical predictions of the sound pressure due to a point monochromatic source in a uniform, high Mach number flow and with Fast Field Program calculations of sound propagation in a stratified moving atmosphere.</description><subject>Acoustics</subject><subject>Exact sciences and technology</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Linear acoustics</subject><subject>Physics</subject><issn>0001-4966</issn><issn>1520-8524</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNpF0VFrHCEQAGApDc0l7UP_QPGlhUA3dXbVXR9DSNtAoC_t8zLnjlfLqhfdLeQX5G_X3h0EH9Thc5gZGXsP4hqghS9wDYME1cErtgHVimZQrXzNNkIIaKTR-pxdlPKnXtXQmTfsHFSvjO7bDXu-e1xx8SkW7lLmzke_UDN55yhTtPSZLz7UQAroIy8-rPOB8-R4SWuc-D6nPe6OwUpC-uvjrp5-p5B2FCmthQeaPHKsOq6Bsrc4cx_2MwWKy-HpW3bmcC707rRfsl9f737efm8efny7v715aGzXm6VxTplpcnYSQhopHAq3lYMjtNCBJkJtJBoFoketSHdWGOm2KNGSHCaA7pJ9OuatZT-uVJYx-GJpnvFQ6ah7JTqpRYVXR2hzKiWTG_fZB8xPI4jx_9THuo5Tr_bDKem6ra2-yNOYK_h4Alhq7y5jtL68OK3a-m-m-wd4cI00</recordid><startdate>20050201</startdate><enddate>20050201</enddate><creator>OSTASHEV, Vladimir E</creator><creator>WILSON, D. 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Keith</creatorcontrib><creatorcontrib>LANBO LIU</creatorcontrib><creatorcontrib>ALDRIDGE, David F</creatorcontrib><creatorcontrib>SYMONS, Neill P</creatorcontrib><creatorcontrib>MARLIN, David</creatorcontrib><collection>Pascal-Francis</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>ComDisDome</collection><jtitle>The Journal of the Acoustical Society of America</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>OSTASHEV, Vladimir E</au><au>WILSON, D. 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Two candidate equation sets, both derived from linearized equations of fluid dynamics, are proposed. The first, which contains three coupled equations for the sound pressure, vector acoustic velocity, and acoustic density, is obtained without any approximations. The second, which contains two coupled equations for the sound pressure and vector acoustic velocity, is derived by ignoring terms proportional to the divergence of the medium velocity and the gradient of the ambient pressure. It is shown that the second set has the same or a wider range of applicability than equations for the sound pressure that have been previously used for analytical and numerical studies of sound propagation in a moving atmosphere. Practical FDTD implementation of the second set of equations is discussed. Results show good agreement with theoretical predictions of the sound pressure due to a point monochromatic source in a uniform, high Mach number flow and with Fast Field Program calculations of sound propagation in a stratified moving atmosphere.</abstract><cop>Woodbury, NY</cop><pub>Acoustical Society of America</pub><pmid>15759672</pmid><doi>10.1121/1.1841531</doi><tpages>15</tpages></addata></record> |
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title | Equations for finite-difference, time-domain simulation of sound propagation in moving inhomogeneous media and numerical implementation |
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