proposition 30.25 Twenty-one constants

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proposition 30.25: Twenty-one constants30.25definition 30.24: The elasticity tensor30.24proposition 7.105: Clairaut–Schwarz7.105definition 30.37: Voigt notation30.37proposition 30.38: The Cauchy relations30.38theorem A.675: Three constants for a cubic crystal, two for an isotropic solidA.675proof : ch:13-continuum-elasticity@proof-11proofdefinition 30.6: Linear strain and infinitesimal rotation30.6theorem 30.18: Cauchy: the stress tensor exists30.18phenomenon 30.28: Hooke's law30.28remark 30.78: Anharmonicity: what the quadratic energy also suppresses30.78definition 7.20: Continuity at a point7.20theorem 7.35: Mean value theorem7.35definition 10.4: The second-order operator10.4lemma A.75: Differentiating a pullback along a flowA.75lemma 22.20: The symplectic condition22.20proposition 7.123: Second-order identities of the nabla calculus7.123proposition 30.14: Saint-Venant compatibility is necessary30.14proposition 22.30: Properties of the Poisson bracket22.30proposition 13.148: prop:mfd-torsion-tensor13.148proposition 10.16: Cauchy's characteristic strips10.16theorem 7.132: Stokes7.132theorem 7.106: Taylor's theorem in several variables7.106theorem 13.152: Riemann tensor; Ricci identity with torsion13.152theorem 13.112: Symmetric analogue of the converse Poincaré lemma13.112theorem 24.21: Liouville24.21proof : ch:05-real-analysis@proof-64proofremark 30.39: The rari-constant controversy, decided by measurement30.39proof : ch:13-continuum-elasticity@proof-17proofproposition A.673: Cubic tensors of rank fourA.673remark A.676: The third cubic constant is measured, and it is not smallA.676proof : app:A-long-proofs@proof-403proof

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typedirectionnode provenancewhere
depends_on The elasticity tensor declared parts/03-classical-mechanics/13-continuum-elasticity.tex:788
depends_on Clairaut–Schwarz declared parts/03-classical-mechanics/13-continuum-elasticity.tex:788
depends_on Voigt notation declared parts/03-classical-mechanics/13-continuum-elasticity.tex:1240
depends_on The Cauchy relations declared parts/03-classical-mechanics/13-continuum-elasticity.tex:1271
depends_on Three constants for a cubic crystal, two for an isotropic solid declared appendices/A-long-proofs.tex:32876
proves ch:13-continuum-elasticity@proof-11 declared parts/03-classical-mechanics/13-continuum-elasticity.tex:791