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dc.contributor.authorDeSanto, John Anthony
dc.date.accessioned2018-10-11T14:04:53Z
dc.date.available2018-10-11T14:04:53Z
dc.date.issued1975/10
dc.identifier343
dc.identifier.govdocCP-17/8
dc.identifier.urihttp://hdl.handle.net/20.500.12489/29
dc.description.abstractUsing a conformal mapping technique in a rectangular waveguide, we present an exact integral relation between the solutions of the Helmholtz equation whose sound speed c(x,y) varies as a function of both depth y and range x and the solutions of a parabolic equation whose sound speed varies in the mapped depth coordinate. The relation of the corresponding boundary value problems is also discussed, as well as the use of the . parabolic approximation in underwater sound propagation problems. The conformal transformation interrelates the sound speeds of the two equations. Several examples are discussed. When c(x,y) = c(y) is only a function of depth we get the recent result of Polyanskii. Other examples for a general conformal transformation are functions c(x»y) which are sinusoidal in depth and exponentially decrease to a constant in range. Several alternative methods of using these results are also discussed.
dc.format17 p. : ill. ; digital, PDF file
dc.languageEnglish
dc.publisherNATO. SACLANTCEN
dc.sourceIn: Ocean Acoustic Modelling (SACLANTCEN Conference Proceedings CP-17), Part 8, 1975, pp. 43-1 - 43-17.
dc.subjectAcoustic propagation
dc.subjectSound velocity in sea water
dc.subjectHelmholtz equation
dc.subjectParabolic equations
dc.subjectDifferential equations, Partial - Numerical solutions
dc.titleConnection between the solution of the Helmholtz and parabolic equations for sound propagation
dc.typePapers and Articles
dc.typeConference Proceedings (CP)


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