definition 30.24 The elasticity tensor

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definition 30.24: The elasticity tensor30.24definition 30.6: Linear strain and infinitesimal rotation30.6theorem 30.18: Cauchy: the stress tensor exists30.18definition 30.37: Voigt notation30.37phenomenon 30.28: Hooke's law30.28proposition 30.25: Twenty-one constants30.25proposition 30.38: The Cauchy relations30.38remark 30.78: Anharmonicity: what the quadratic energy also suppresses30.78theorem A.675: Three constants for a cubic crystal, two for an isotropic solidA.675definition 13.91: Symmetric and antisymmetric parts13.91equation 30.2: eq:elast-displacement30.2definition A.680: Kirchhoff kinematicsA.680definition 30.11: Green strain30.11example 30.13: A rigid rotation forges a strain of -θ^2/230.13example 30.10: Simple shear and pure shear are the same strain30.10lemma A.681: Strains under the Kirchhoff hypothesisA.681proposition 30.14: Saint-Venant compatibility is necessary30.14proposition 30.8: The trace is the fractional volume change30.8proposition 30.9: Principal strains30.9proposition 30.7: Strain is a Cartesian tensor of rank two30.7definition 30.17: Traction30.17definition 13.5: Tensor under orthogonal transformations13.5definition 31.1: Fluid31.1proposition 30.19: The stress tensor is symmetric30.19proposition 30.74: The maximum shear stress, and its indifference to pressure30.74remark 30.72: Stress concentration30.72theorem A.695: Boussinesq's point-force solution, quotedA.695theorem 30.21: Cauchy's equation of motion30.21proof : ch:13-continuum-elasticity@proof-7proofremark 30.39: The rari-constant controversy, decided by measurement30.39lemma 30.26: Isotropic Cartesian tensors of rank four30.26phenomenon 30.32: Poisson contraction30.32proof : ch:13-continuum-elasticity@proof-12proofproposition 7.105: Clairaut–Schwarz7.105proof : ch:13-continuum-elasticity@proof-11proofproof : 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 Linear strain and infinitesimal rotation declared parts/03-classical-mechanics/13-continuum-elasticity.tex:778
depends_on Cauchy: the stress tensor exists declared parts/03-classical-mechanics/13-continuum-elasticity.tex:778
depends_on Voigt notation declared parts/03-classical-mechanics/13-continuum-elasticity.tex:1240
depends_on Hooke's law declared parts/03-classical-mechanics/13-continuum-elasticity.tex:868
depends_on Twenty-one constants declared parts/03-classical-mechanics/13-continuum-elasticity.tex:788
depends_on The Cauchy relations declared parts/03-classical-mechanics/13-continuum-elasticity.tex:1271
depends_on Anharmonicity: what the quadratic energy also suppresses declared parts/03-classical-mechanics/13-continuum-elasticity.tex:2776
depends_on Three constants for a cubic crystal, two for an isotropic solid declared appendices/A-long-proofs.tex:32876