The determination of the acoustic far field of a radiating body in an acoustic fluid from boundary measurements
The far field (FF) of a radiating or scattering object immersed in an acoustic fluid can be represented in the frequency domain as a finite dimension linear combination of basis functions, which are determined by the shape and the size of the object in acoustic wavelengths. The coefficients of the l...
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Veröffentlicht in: | The Journal of the Acoustical Society of America 1993-05, Vol.93 (5), p.2788-2797 |
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description | The far field (FF) of a radiating or scattering object immersed in an acoustic fluid can be represented in the frequency domain as a finite dimension linear combination of basis functions, which are determined by the shape and the size of the object in acoustic wavelengths. The coefficients of the linear combination are obtained as the outputs of a bank of spatial filters whose inputs are either the boundary normal velocity—for the radiation problem—or the boundary pressure and the normal velocity—for the scattering problem—measured by a dense set of sensors. The filter outputs provide the information sufficient to reconstruct the radiated or scattered far field, amplitude and phase. The structure of the filters is identified from the singular valve decomposition of the appropriate radiation or scattering operator, mapping the boundary normal velocity, or the combination of normal velocity and pressure, into the FF. Also, from the filter outputs, the efficiently radiating component of the boundary field can be extracted. For example the boundary total normal velocity may have a localized high peak, which however may be completely or almost completely absent in the radiating component. Selected results of an extensive simulation are presented illustrating the accuracy of the reconstruction of the FF from the spatial filtering of the boundary field. |
doi_str_mv | 10.1121/1.405826 |
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V ; JONES, K. E</creator><creatorcontrib>BORGIOTTI, G. V ; JONES, K. E</creatorcontrib><description>The far field (FF) of a radiating or scattering object immersed in an acoustic fluid can be represented in the frequency domain as a finite dimension linear combination of basis functions, which are determined by the shape and the size of the object in acoustic wavelengths. The coefficients of the linear combination are obtained as the outputs of a bank of spatial filters whose inputs are either the boundary normal velocity—for the radiation problem—or the boundary pressure and the normal velocity—for the scattering problem—measured by a dense set of sensors. The filter outputs provide the information sufficient to reconstruct the radiated or scattered far field, amplitude and phase. The structure of the filters is identified from the singular valve decomposition of the appropriate radiation or scattering operator, mapping the boundary normal velocity, or the combination of normal velocity and pressure, into the FF. Also, from the filter outputs, the efficiently radiating component of the boundary field can be extracted. For example the boundary total normal velocity may have a localized high peak, which however may be completely or almost completely absent in the radiating component. 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The structure of the filters is identified from the singular valve decomposition of the appropriate radiation or scattering operator, mapping the boundary normal velocity, or the combination of normal velocity and pressure, into the FF. Also, from the filter outputs, the efficiently radiating component of the boundary field can be extracted. For example the boundary total normal velocity may have a localized high peak, which however may be completely or almost completely absent in the radiating component. 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E</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c254t-7510fde22beee000b8448856da9de5b1acc60bbf0081e7e7eb9832281e7085b63</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1993</creationdate><topic>Acoustical measurements and instrumentation</topic><topic>Acoustics</topic><topic>Exact sciences and technology</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>BORGIOTTI, G. V</creatorcontrib><creatorcontrib>JONES, K. E</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>The Journal of the Acoustical Society of America</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>BORGIOTTI, G. V</au><au>JONES, K. E</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The determination of the acoustic far field of a radiating body in an acoustic fluid from boundary measurements</atitle><jtitle>The Journal of the Acoustical Society of America</jtitle><date>1993-05-01</date><risdate>1993</risdate><volume>93</volume><issue>5</issue><spage>2788</spage><epage>2797</epage><pages>2788-2797</pages><issn>0001-4966</issn><eissn>1520-8524</eissn><coden>JASMAN</coden><abstract>The far field (FF) of a radiating or scattering object immersed in an acoustic fluid can be represented in the frequency domain as a finite dimension linear combination of basis functions, which are determined by the shape and the size of the object in acoustic wavelengths. The coefficients of the linear combination are obtained as the outputs of a bank of spatial filters whose inputs are either the boundary normal velocity—for the radiation problem—or the boundary pressure and the normal velocity—for the scattering problem—measured by a dense set of sensors. The filter outputs provide the information sufficient to reconstruct the radiated or scattered far field, amplitude and phase. The structure of the filters is identified from the singular valve decomposition of the appropriate radiation or scattering operator, mapping the boundary normal velocity, or the combination of normal velocity and pressure, into the FF. Also, from the filter outputs, the efficiently radiating component of the boundary field can be extracted. For example the boundary total normal velocity may have a localized high peak, which however may be completely or almost completely absent in the radiating component. Selected results of an extensive simulation are presented illustrating the accuracy of the reconstruction of the FF from the spatial filtering of the boundary field.</abstract><cop>Woodbury, NY</cop><pub>Acoustical Society of America</pub><doi>10.1121/1.405826</doi><tpages>10</tpages></addata></record> |
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subjects | Acoustical measurements and instrumentation Acoustics Exact sciences and technology Fundamental areas of phenomenology (including applications) Physics |
title | The determination of the acoustic far field of a radiating body in an acoustic fluid from boundary measurements |
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