theorem 5.133 Isotropic Cartesian tensors of rank at most four

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theorem 5.133: Isotropic Cartesian tensors of rank at most four5.133lemma 5.33: Determinant through the Levi–Civita symbol5.33lemma 5.132: Parity constraint5.132proposition 5.130: An orthogonal transformation is an isometry5.130lemma A.742: Isotropic representationA.742lemma A.671: The three products are independentA.671lemma 30.26: Isotropic Cartesian tensors of rank four30.26remark A.677: The lower ranks, and why an isotropic solid is not piezoelectricA.677remark 30.27: Two results this chapter borrows from Part II30.27remark 13.7: What the classification is used for13.7proof : ch:03-linear-algebra-representations@proof-58proofdefinition 5.32: Levi–Civita symbol; cross product5.32equation 5.19: eq:lin-leibniz-det5.19proposition 5.35: The identities of the vector algebra of ℝ^35.35proof : ch:03-linear-algebra-representations@proof-8proofdefinition 5.131: Isotropic Cartesian tensor5.131equation 5.162: eq:rep-special-orthogonal5.162proof : ch:03-linear-algebra-representations@proof-57proofdefinition 5.18: Inner product5.18equation 5.44: eq:lin-norm-assoc5.44proposition 5.49: Injective, surjective, invertible5.49proof : ch:03-linear-algebra-representations@proof-56proofdefinition 14.26: The rotation group14.26corollary A.743: Two scalar functions instead of a tensor fieldA.743lemma A.747: The third-order structure functionsA.747lemma A.744: Vanishing of the pressure–velocity correlationA.744proof : app:A-long-proofs@proof-432proofequation 5.168: eq:rep-isotropic-45.168proposition A.673: Cubic tensors of rank fourA.673proof : app:A-long-proofs@proof-401proofdefinition 13.5: Tensor under orthogonal transformations13.5phenomenon 30.28: Hooke's law30.28proof : ch:13-continuum-elasticity@prooflink-1proofremark 5.134: What the theorem buys, and what it does not5.134theorem 7.137: Helmholtz decomposition7.137

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typedirectionnode provenancewhere
depends_on Determinant through the Levi–Civita symbol declared parts/02-mathematical-methods/03-linear-algebra-representations.tex:5750
depends_on Parity constraint declared parts/02-mathematical-methods/03-linear-algebra-representations.tex:5750
depends_on An orthogonal transformation is an isometry declared parts/02-mathematical-methods/03-linear-algebra-representations.tex:5750
depends_on Isotropic representation declared appendices/A-long-proofs.tex:35984
depends_on The three products are independent declared appendices/A-long-proofs.tex:32676
depends_on Isotropic Cartesian tensors of rank four declared parts/03-classical-mechanics/13-continuum-elasticity.tex:813
depends_on The lower ranks, and why an isotropic solid is not piezoelectric declared appendices/A-long-proofs.tex:32985
depends_on Two results this chapter borrows from Part II declared parts/03-classical-mechanics/13-continuum-elasticity.tex:851
depends_on What the classification is used for declared parts/02-mathematical-methods/11-manifolds-tensors-curvature.tex:625
proves ch:03-linear-algebra-representations@proof-58 declared parts/02-mathematical-methods/03-linear-algebra-representations.tex:5754