Access the full text.
Sign up today, get DeepDyve free for 14 days.
A. Duncan, A. Gavrilov, R. McCauley, I. Parnum, J. Collis (2013)
Characteristics of sound propagation in shallow water over an elastic seabed with a thin cap-rock layer.The Journal of the Acoustical Society of America, 134 1
F. Jensen, C. Ferla (1990)
Numerical solutions of range-dependent benchmark problems in ocean acousticsJournal of the Acoustical Society of America, 87
A. Duncan, A. Gavrilov (2012)
Low frequency acoustic propagation over calcarenite seabeds with thin, hard caps.
J. Collis, Adam Metzler (2014)
Seismo-acoustic propagation near thin and low-shear speed ocean bottom sediments using a massive elastic interface.The Journal of the Acoustical Society of America, 135 1
F. Jensen, W. Kuperman, M. Porter, H. Schmidt, S. McKay (1994)
Computational Ocean AcousticsComputers in Physics, 9
C. Erbe (2013)
International Regulation of Underwater NoiseAcoustics Australia, 41
A. Duncan, A. Gavrilov, Fan Li (2009)
Acoustic propagation over limestone seabeds
E. Hamilton, R. Bachman (1982)
Sound velocity and related properties of marine sedimentsJournal of the Acoustical Society of America, 72
J. Goh, H. Schmidt, P. Gerstoft, Woojae Seone (1997)
Benchmarks for validating range-dependent seismo-acoustic propagation codesIEEE Journal of Oceanic Engineering, 22
(1994)
Ocean and Seabed Acoustics: A Theory ofWave Propagation
NP James, Y Bone (2011)
Neritic Carbonate Sediments in a Temperate Realm
N. James, Y. Bone (2010)
Neritic Carbonate Sediments in a Temperate Realm: Southern Australia
J. Hovem (2010)
Marine acoustics: the physics of sound in underwater environments
M. Collins (1991)
Higher-order Padé approximations for accurate and stable elastic parabolic equations with application to interface wave propagationJournal of the Acoustical Society of America, 89
F. Milinazzo, C. Zala, G. Brooke (1997)
Rational square-root approximations for parabolic equation algorithmsJournal of the Acoustical Society of America, 101
A. Tolstoy (2001)
WHAT ABOUT ADIABATIC NORMAL MODESJournal of Computational Acoustics, 9
N. James, Thomas Boreen, Y. Bone, D. Feary (1994)
Holocene carbonate sedimentation on the west Eucla Shelf, Great Australian Bight: a shaved shelfSedimentary Geology, 90
L. Collins (1988)
Sediments and history of the Rottnest Shelf, southwest Australia: a swell-dominated, non-tropical carbonate marginSedimentary Geology, 60
A. Duncan, A. Gavrilov, Tao Hu (2008)
Using offshore seismic surveys as acoustic sources of opportunity for geoacoustic inversionJournal of the Acoustical Society of America, 123
Evan Westwood, R. Koch (1998)
Elimination of branch cuts from the normal mode solution using gradient half‐spacesJournal of the Acoustical Society of America, 106
V. Gostin, A. Belperio, J. Cann (1988)
The Holocene non-tropical coastal and shelf carbonate province of southern AustraliaSedimentary Geology, 60
Evan Westwood, C. Tindle, N. Chapman (1996)
A normal mode model for acousto‐elastic ocean environmentsJournal of the Acoustical Society of America, 100
Large portions of the Australian continental shelf have a seabed composed of layered cemented or semi-cemented calcarenite. This work investigates the ability of a wavenumber integration sound propagation model, two normal mode sound propagation models, and a parabolic equation sound propagation model to consistently predict the acoustic field over four types of calcarenite style seabeds. The four geoacoustic models that are presented here represent seabed types that are likely to be found in the Australian marine environment. Transmission loss results for each geoacoustic model are computed using each sound propagation model, which are compared over a broad band of low frequencies in order to assess their relative performance. The performance of the wavenumber integration model, SCOOTER, and the two normal mode models over a broad band of low frequencies was found to be accurate and robust for all the tested scenarios. However, for one of the normal mode models, KRAKENC, long computational runtimes were incurred to produce accurate results. The parabolic equation model RAMSGeo produced accurate transmission loss results at some of the frequencies, but it also produced some unrealistic transmission loss predictions when thin layers were present in the seabed. The normal mode model ORCA was found to have the best balance between accuracy and efficiency because it had the shortest runtimes for most of the calculation frequencies and the shortest overall runtime.
Acoustics Australia – Springer Journals
Published: Sep 19, 2017
Read and print from thousands of top scholarly journals.
Already have an account? Log in
Bookmark this article. You can see your Bookmarks on your DeepDyve Library.
To save an article, log in first, or sign up for a DeepDyve account if you don’t already have one.
Copy and paste the desired citation format or use the link below to download a file formatted for EndNote
Access the full text.
Sign up today, get DeepDyve free for 14 days.
All DeepDyve websites use cookies to improve your online experience. They were placed on your computer when you launched this website. You can change your cookie settings through your browser.