2003
DOI: 10.1016/s0021-9991(02)00056-6
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A Laplace transform/potential-theoretic method for acoustic propagation in subsonic flows

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Cited by 6 publications
(2 citation statements)
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“…It can be treated subtracting off the singularity from the integrand function and using Hermite interpolation techniques for the successive integration. Using the convected nonreflecting boundary conditions equations (39) and (40) and the classical procedure to isolate the singularity parts of the modal Green’s function and its convected normal derivative equations (57) and (58) 41,49,85 , we get a new original form of the generalized modal boundary integral formulation with arbitrary uniform mean flow wearing on the modal acoustic field at any point m as follows in which c±(m) is a novel free term solving the singular integrals arising from the limit integral formulation. It is derived from the exterior and anterior acoustic media, rewritten by the following simplified integral form where θ(m) is the convected axisymmetric angle of center m and moving between two convected angles (θ1*,θ2*) such as θ=±(θ2*θ1*).…”
Section: Generalized and Improved Modal Boundary Element Methodsmentioning
confidence: 99%
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“…It can be treated subtracting off the singularity from the integrand function and using Hermite interpolation techniques for the successive integration. Using the convected nonreflecting boundary conditions equations (39) and (40) and the classical procedure to isolate the singularity parts of the modal Green’s function and its convected normal derivative equations (57) and (58) 41,49,85 , we get a new original form of the generalized modal boundary integral formulation with arbitrary uniform mean flow wearing on the modal acoustic field at any point m as follows in which c±(m) is a novel free term solving the singular integrals arising from the limit integral formulation. It is derived from the exterior and anterior acoustic media, rewritten by the following simplified integral form where θ(m) is the convected axisymmetric angle of center m and moving between two convected angles (θ1*,θ2*) such as θ=±(θ2*θ1*).…”
Section: Generalized and Improved Modal Boundary Element Methodsmentioning
confidence: 99%
“…7 Its based on a combination of Linearised Euler Equations in space variables. 85 To overcome the Helmoltz problem, the interior and exterior acoustic domains are necessary to impose boundary conditions at its closed boundaries. In order to relate the flow variables on the upper side Ω e of the boundary Γ to the variables on the lower side Ω i , the continuity of the acoustic field for the exterior and interior media can be given by Taylor and Myers conditions on the generator Γ.…”
Section: Modal Formulationsmentioning
confidence: 99%