1981
DOI: 10.1016/s0302-3524(81)80122-3
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Acoustic reflection from estuarine pycnoclines

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Cited by 8 publications
(9 citation statements)
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“…The reflection coefficients can be calculated from a measured profile of any shape and no assumptions about the processes creating the pycnocline need to be made, making Eq. (4) more comprehensive and simpler to implement than the Gupta (1966) and Penrose and Beer (1981) models.…”
Section: Weak-scattering Model For Oceanic Pycnoclinesmentioning
confidence: 99%
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“…The reflection coefficients can be calculated from a measured profile of any shape and no assumptions about the processes creating the pycnocline need to be made, making Eq. (4) more comprehensive and simpler to implement than the Gupta (1966) and Penrose and Beer (1981) models.…”
Section: Weak-scattering Model For Oceanic Pycnoclinesmentioning
confidence: 99%
“…Pycnoclines are important oceanographically (e.g., Mann and Lazier, 2006), and there is a long history of observations (e.g., Fisher and Squier, 1975;Penrose and Beer, 1981) of enhanced acoustic scattering at mid (1-10 kHz) and high frequencies (>10 kHz) associated with oceanic pycnoclines, defined as gradients in density, but which in the following discussion also refer to the accompanying sound speed gradients. The possibility of scattering from oceanic sound speed gradients was suggested decades ago (Munk and Garrett, 1973) and, around the same time, a scattering model that included sound speed and density gradients was developed (Gupta, 1966).…”
Section: Introductionmentioning
confidence: 99%
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“…The physical environment itself can also be examined acoustically. The target strength of pycnoclines can be measured by acoustic reflection and may have a target strength of -75 to -85 dB at 200 kHz [6]. Internal waves and their fine structure have been measured by acoustic methods [7,8].…”
mentioning
confidence: 99%