The effect of sediment rigidity on bottom reflection loss in a typical deep sea sediment
The effect of sediment rigidity on bottom reflection loss, RL=−20 log10‖R‖, where R is the plane-wave reflection coefficient, is studied using a computational model. A single inhomogeneous turbidite layer overlying a homogeneous substrate is treated with an emphasis on low frequencies (10 to 200 Hz)...
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Veröffentlicht in: | J. Acoust. Soc. Am.; (United States) 1980-08, Vol.68 (2), p.634-638 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | The effect of sediment rigidity on bottom reflection loss, RL=−20 log10‖R‖, where R is the plane-wave reflection coefficient, is studied using a computational model. A single inhomogeneous turbidite layer overlying a homogeneous substrate is treated with an emphasis on low frequencies (10 to 200 Hz) and low grazing angles (0 ° to 45 °). We find that sediment rigidity can be neglected for thick layers (∠500 m) while it can produce significant increases in RL for thin layers (∠36 m). The frequency dependence of RL for thin layers has a low-frequency regime characterized by large peaks (∠25 dB) recurring at short (∠2 Hz) intervals. At high frequencies there remains a persistent increase in RL (∠4 dB). The most important mechanism for sediment S-wave excitation is found to be compressional wave conversion at the sediment–substrate interface. |
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ISSN: | 0001-4966 1520-8524 |
DOI: | 10.1121/1.384721 |