A Fast Method of Deriving the Kirchhoff Formula for Moving ... · Motivation and the Problem...

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A Fast Method of Deriving the Kirchhoff Formula for Moving Surfaces F. Farassat and Joe W. Posey NASA Langley Research Center Hampton, Virginia Presented at the 154th Meeting of the Acoustical Society of America 27 November- 1 December 2007, New Orleans, Louisiana 1 |14 https://ntrs.nasa.gov/search.jsp?R=20080002262 2019-12-31T09:30:11+00:00Z

Transcript of A Fast Method of Deriving the Kirchhoff Formula for Moving ... · Motivation and the Problem...

Page 1: A Fast Method of Deriving the Kirchhoff Formula for Moving ... · Motivation and the Problem Helicopter rotor noise prediction Kirchhoff formula for a moving surface gives p' in the

A Fast Method of Deriving the Kirchhoff

Formula for Moving Surfaces

F. Farassat and Joe W. PoseyNASA Langley Research Center

Hampton, Virginia

Presented at the 154th Meeting of the Acoustical Society of America27 November- 1 December 2007, New Orleans, Louisiana

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https://ntrs.nasa.gov/search.jsp?R=20080002262 2019-12-31T09:30:11+00:00Z

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Outline | Motivation and the Problem| The Imbedding Method| Generalized Differentiation Rules| Classical Kirchhoff Formula| Kirchhoff Formula for a Moving Surface| Concluding Remarks

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Motivation and the ProblemHelicopter rotor noise prediction

Kirchhoff formula for a moving surface gives p' inthe exterior region from surface data.

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Derivation of Kirchhoff Formulafor a Moving Surface

Classical Analysis| 4D Green's Theorem required| Some ambiguities working with 4D integrals| Extremely involved algebraic manipulations| Difficulties with physical meaning of some terms

References:

Classical analysis: W. R. Morgans: The Kirchhoff formula extended to a mov-ing surface, Philosophical Magazine, 9, 1930, 141-161

Modern analysis using generalized functions: F. Farassat and M. K. Myers: Extension of Kirchhoff's formula to radiation from moving sources, Journalof Sound and Vibration, 123 (3), 1988, 451-460

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The Imbedding Method- The Idea| When the Green's function G (x, y) of a differential equation u =f is known in the a domain S, then that Green's function can be uti-lized in solving the same differential equation in a smallerdomain S' Õ S.

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The Imbedding Method- The Idea| When the Green's function G (x, y) of a differential equation u =f is known in the a domain S, then that Green's function can be uti-lized in solving the same differential equation in a smallerdomain S' Õ S.

| The problem in the domain S' is imbedded in the larger domainS by giving a known value to the unknown function in theregion S \ S' which satisfies the boundary conditions of the prob-lem in S.

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The Imbedding Method- The Idea| When the Green's function G (x, y) of a differential equation u =f is known in the a domain S, then that Green's function can be uti-lized in solving the same differential equation in a smallerdomain S' Õ S.

| The problem in the domain S' is imbedded in the larger domainS by giving a known value to the unknown function in theregion S \ S' which satisfies the boundary conditions of the prob-lem in S.

| The imbedded problem, in general, has a discontinuous solu-tion at the boundary surface ∂S' of the domain S'. This means thatthe best tool to solve the imbedded problem is the generalizedfunction (GF) theory.

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The Imbedding Method (cont'd)| The Green's function method is applicable in find-ing the discontinuous solution of differential equa-tion as long as all the derivatives are viewed asgeneralized derivatives.

References:

F. Farassat, Introduction to Generalized Functions With Applications inAerodynamics and Acoustics, NASA Technical Paper 3428, 1994

F. Farassat: The Kirchhoff Formulas for Moving Surfaces in Aeroacoustics -The Subsonic and Supersonic Cases, NASA Technical Memorandum 110285,September 1996

F. Farassat, et. al: Working With the Wave Equation in Aeroacoustics- ThePleasures of Generalized Functions, AIAA-2007-3562, 2007

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An Example of the Imbedding MethodConsider l uHxL = u″ on [0, 1], BCs: u H0L - 2 u¢H0L = 0 &u H1L + u¢H1L = 0. The Green's function is

Use above Green's function to solve the same ODE

on [a, b] Ã [0, 1] by the imbeddingmethod. Let unknown function take value 0 on [0, 1] \ [a, b].

Then use generalized function (GF) theory to find newODE.

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Generalized Differentiation Rules

Generalized derivative (GD) of a differ-entiable function with a single jump discontinuityat x0 is

GD of a function k (x) in multidimensionswith a discontinuity Dk across a surface f = 0,—f = n, is

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An Example of the Imbedding Method (cont'd)

New ODE of example imbedded problemis:

with the following definitions:

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Classical Kirchhoff Formula

Imbed this problem in unbounded 3D space byassuming that the unknown function is 0 inside thesurface f = 0 (ı f = n ). Let

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Classical Kirchhoff Formula (cont'd)

New PDE to derive the classical Kirch-hoff formula is:

Next use the Green's function of the wave equationin the unbounded space to get the result.

The rest is simple algebraicmanipulations!

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Kirchhoff Formula for a Moving Surface

To solve in the exterior of themoving surface f = 0, imbed this problem inunbounded 3D space taking the value 0 inside themoving surface. Let:

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Kirchhoff Formula for a Moving Surface (cont'd)

New PDE to derive Kirchhoff formula fora moving surface is:

Use the Green's function of the wave equation inthe unbounded space to get the result.

The rest is again simple algebraicmanipulations!

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Concluding RemarksThe imbedding method increases the utility of aknown Green's function in solving new BV and IVproblems of acoustics and other applied fields.

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