The Kirchhoff–Helmholtz integral combines the Helmholtz equation with the Kirchhoff integral theorem to produce a method applicable to acoustics, seismology 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.
P ( w , z ) = ∬ d A ( G ( w , z | z ′ ) ∂ ∂ n P ( w , z ′ ) − P ( w , z ′ ) ∂ ∂ n G ( w , z | z ′ ) ) d z ′ {\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'}
See also Kirchhoff integral
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