theorem 7.137 Helmholtz decomposition

open in the book · parts/02-mathematical-methods/05-real-analysis.tex:4652 · p. 260

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theorem 7.137: Helmholtz decomposition7.137proposition 7.123: Second-order identities of the nabla calculus7.123proposition 10.67: The Newtonian potential is the fundamental solution10.67theorem 7.109: Leibniz integral rule7.109remark A.527: The hypotheses, and what happens without themA.527remark 30.46: Why the plane-wave route, and not the potentials30.46remark 30.27: Two results this chapter borrows from Part II30.27remark 10.73: What compact support is doing, and the rate that replaces it10.73remark 10.74: Where the decomposition is used, and what it costs10.74proof : app:A-long-proofs@proof-317proofproof : ch:05-real-analysis@prooflink-4proofequation 7.127: eq:ana-nabla-laplacian7.127lemma 7.121: Contraction of two Levi-Civita symbols7.121proposition 7.105: Clairaut–Schwarz7.105remark 7.124: The Laplacian of a vector field is a Cartesian notion7.124theorem A.523: Helmholtz decomposition: existenceA.523theorem A.525: Helmholtz decomposition: uniquenessA.525proof : ch:05-real-analysis@proof-76proofdefinition 17.38: Schwartz space and tempered distributions17.38lemma 10.44: Green's identities10.44example 10.49: The method of images10.49lemma A.94: Fundamental solution of \pp_\bar zA.94proposition A.522: The Newtonian potential inverts the LaplacianA.522proposition 10.71: Green's representation formula10.71proof : ch:08-pdes@proof-27proofdefinition 7.125: Multiple integral7.125theorem 7.25: Heine–Cantor: uniform continuity7.25theorem 7.35: Mean value theorem7.35corollary 7.110: Variable limits of integration7.110lemma 7.116: Functions vanishing on a regular zero set7.116lemma A.607: A zero-free entire function is an exponentialA.607lemma A.599: One variable, complex coefficientA.599proposition A.524: Rate of decayA.524proposition A.521: Every derivative passes onto gA.521proof : ch:05-real-analysis@proof-67proofequation 7.126: eq:ana-nabla-curl7.126phenomenon 30.43: Two bulk wave speeds30.43theorem 30.40: Navier–Cauchy equations30.40theorem 5.133: Isotropic Cartesian tensors of rank at most four5.133

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typedirectionnode provenancewhere
depends_on Second-order identities of the nabla calculus declared parts/02-mathematical-methods/05-real-analysis.tex:4673
depends_on The Newtonian potential is the fundamental solution declared parts/02-mathematical-methods/05-real-analysis.tex:4673
depends_on Leibniz integral rule declared parts/02-mathematical-methods/05-real-analysis.tex:4673
depends_on The hypotheses, and what happens without them declared appendices/A-long-proofs.tex:25777
depends_on Why the plane-wave route, and not the potentials declared parts/03-classical-mechanics/13-continuum-elasticity.tex:1604
depends_on Two results this chapter borrows from Part II declared parts/03-classical-mechanics/13-continuum-elasticity.tex:851
depends_on What compact support is doing, and the rate that replaces it declared parts/02-mathematical-methods/08-pdes.tex:2003
depends_on Where the decomposition is used, and what it costs declared parts/02-mathematical-methods/08-pdes.tex:2026
proves app:A-long-proofs@proof-317 declared appendices/A-long-proofs.tex:25702
proves ch:05-real-analysis@prooflink-4 declared parts/02-mathematical-methods/05-real-analysis.tex:4677