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Kirchhoff–Helmholtz integral

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The Kirchhoff–Helmholtz integral combines the Helmholtz equation with the Kirchhoff integral theorem[1] to produce a method applicable to acoustics,[2] seismology[3] and other disciplines involving wave propagation. It states that the sound pressure is completely determined within a volume free of sources, if sound pressure and velocity are determined in all points on its surface.

[math]\displaystyle{ \boldsymbol{P}(w,z)=\iint_{dA} \left(G(w,z \vert z') \frac{\partial}{\partial n} P(w,z')- P(w,z') \frac{\partial}{\partial n} G(w,z \vert z') \right)dz' }[/math]

See also

References

  1. Kurt Heutschi (2013-01-25), Acoustics I: sound field calculations, https://people.ee.ethz.ch/~isistaff/courses/ak1/acoustics-sound-field-calculations.pdf 
  2. Oleg A. Godin (August 1998), "The Kirchhoff–Helmholtz integral theorem and related identities for waves in an inhomogeneous moving fluid", Journal of the Acoustical Society of America 99 (4): 2468–2500, doi:10.1121/1.415524, https://asa.scitation.org/doi/abs/10.1121/1.415524 
  3. Scott, Patricia; Helmberger, Don (1983), Applications of the Kirchhoff-Helmholtz integral to problems in seismology 





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