definition 30.6 Linear strain and infinitesimal rotation

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definition 30.6: Linear strain and infinitesimal rotation30.6definition 13.91: Symmetric and antisymmetric parts13.91equation 30.2: eq:elast-displacement30.2definition A.680: Kirchhoff kinematicsA.680definition 30.24: The elasticity tensor30.24definition 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 31.8: Rate of strain and vorticity31.8definition 13.142: Killing tensor13.142definition 13.111: Linearised curvature of a symmetric field13.111proposition 30.51: Moment and curvature30.51lemma A.687: Kinetic energyA.687theorem 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.675proposition 30.12: The Green strain measures length exactly30.12proposition A.684: The plate energyA.684proof : app:A-long-proofs@proof-404proofproposition 7.105: Clairaut–Schwarz7.105theorem 30.15: Compatibility is sufficient on a simply connected body30.15proof : ch:13-continuum-elasticity@proof-5proofproof : ch:13-continuum-elasticity@proof-2prooftheorem 5.79: Spectral theorem for a self-adjoint operator5.79proof : ch:13-continuum-elasticity@proof-3proofdefinition 13.5: Tensor under orthogonal transformations13.5proof : ch:13-continuum-elasticity@proof-1proof

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typedirectionnode provenancewhere
depends_on Symmetric and antisymmetric parts declared parts/03-classical-mechanics/13-continuum-elasticity.tex:205
depends_on eq:elast-displacement declared parts/03-classical-mechanics/13-continuum-elasticity.tex:205
depends_on Kirchhoff kinematics declared appendices/A-long-proofs.tex:33097
depends_on The elasticity tensor declared parts/03-classical-mechanics/13-continuum-elasticity.tex:778
depends_on Green strain declared parts/03-classical-mechanics/13-continuum-elasticity.tex:331
depends_on A rigid rotation forges a strain of $-\theta^{2}/2$ declared parts/03-classical-mechanics/13-continuum-elasticity.tex:384
depends_on Simple shear and pure shear are the same strain declared parts/03-classical-mechanics/13-continuum-elasticity.tex:313
depends_on Strains under the Kirchhoff hypothesis declared appendices/A-long-proofs.tex:33112
depends_on Saint-Venant compatibility is necessary declared parts/03-classical-mechanics/13-continuum-elasticity.tex:402
depends_on The trace is the fractional volume change declared parts/03-classical-mechanics/13-continuum-elasticity.tex:250
depends_on Principal strains declared parts/03-classical-mechanics/13-continuum-elasticity.tex:273
depends_on Strain is a Cartesian tensor of rank two declared parts/03-classical-mechanics/13-continuum-elasticity.tex:215