theorem 10.34 Separable systems for the Helmholtz operator

open in the book · parts/02-mathematical-methods/08-pdes.tex:944 · p. 349

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theorem 10.34: Separable systems for the Helmholtz operator10.34equation 10.25: eq:pde-helmholtz-equation10.25lemma 10.28: The separation constant10.28remark 23.19: The same conditions govern the Helmholtz equation23.19proof : app:A-long-proofs@proof-82proofproof : ch:08-pdes@prooflink-3proofdefinition A.116: Orthogonal curvilinear coordinates; scale factorsA.116definition 23.39: Eikonal23.39proposition 10.29: Time separation reduces the canonical equations to Helmholtz10.29definition 10.2: Linear, semilinear, quasilinear10.2definition A.118: Simple separation of the Helmholtz equationA.118example 10.31: Cartesian separation10.31example 10.32: Cylindrical separation10.32example 10.33: Spherical separation10.33proposition 23.9: Separation of the time23.9proof : ch:08-pdes@proof-9prooftheorem 23.17: Stäckel's conditions are sufficient23.17

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typedirectionnode provenancewhere
depends_on eq:pde-helmholtz-equation declared parts/02-mathematical-methods/08-pdes.tex:955
depends_on The separation constant declared parts/02-mathematical-methods/08-pdes.tex:955
depends_on The same conditions govern the Helmholtz equation declared parts/03-classical-mechanics/06-hamilton-jacobi.tex:617
proves app:A-long-proofs@proof-82 declared appendices/A-long-proofs.tex:7457
proves ch:08-pdes@prooflink-3 declared parts/02-mathematical-methods/08-pdes.tex:958