definition 30.31 The engineering moduli

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definition 30.31: The engineering moduli30.31definition 30.20: Pressure and deviatoric stress30.20equation 30.21: eq:elast-hooke-isotropic30.21phenomenon 30.70: Hertzian contact30.70phenomenon 30.60: Coulomb's law of torsion30.60proposition 30.33: Conversion among the moduli30.33proposition 30.51: Moment and curvature30.51remark A.676: The third cubic constant is measured, and it is not smallA.676theorem A.695: Boussinesq's point-force solution, quotedA.695proposition 30.19: The stress tensor is symmetric30.19theorem 5.79: Spectral theorem for a self-adjoint operator5.79definition 30.79: Maxwell viscoelasticity30.79proposition 30.74: The maximum shear stress, and its indifference to pressure30.74remark 30.75: Two criteria, one uncited30.75experiment : Coulomb: the torsion pendulumexperime…proposition A.682: The plane-stress lawA.682remark 30.72: Stress concentration30.72remark 30.29: The Lamé constants and the energy30.29theorem 30.40: Navier–Cauchy equations30.40proposition 30.23: Virtual work; the weak form30.23definition A.698: The Hertz contact problemA.698example A.703: The numbers of the chapter, recomputedA.703example 30.71: Contact stresses are enormous30.71proof : ch:13-continuum-elasticity@proof-34proofproof : ch:13-continuum-elasticity@prooflink-3proofexample 30.61: A torsion fibre as a force sensor30.61phenomenon 34.3: The stiffness of a twisted wire is geometric34.3remark 30.62: Saint-Venant's theory: non-circular sections warp30.62proof : ch:13-continuum-elasticity@proof-31proofphenomenon 30.32: Poisson contraction30.32definition 30.63: Flexural rigidity30.63example 30.35: From single crystals to the isotropic aggregate30.35proposition 30.44: The speed ratio is fixed by Poisson's ratio30.44remark 30.36: How the moduli are actually measured30.36proof : ch:13-continuum-elasticity@proof-15proofdefinition A.680: Kirchhoff kinematicsA.680phenomenon 30.52: Euler buckling30.52theorem 30.56: The beam equation30.56proof : ch:13-continuum-elasticity@proof-27prooftheorem A.675: Three constants for a cubic crystal, two for an isotropic solidA.675neighborhood truncated

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typedirectionnode provenancewhere
cites Mémoire sur l'équilibre et le mouvement des corps élastiques derived parts/03-classical-mechanics/13-continuum-elasticity.tex:962
cites A Course of Lectures on Natural Philosophy and the Mechanical Arts derived parts/03-classical-mechanics/13-continuum-elasticity.tex:960
depends_on Pressure and deviatoric stress declared parts/03-classical-mechanics/13-continuum-elasticity.tex:969
depends_on eq:elast-hooke-isotropic declared parts/03-classical-mechanics/13-continuum-elasticity.tex:969
depends_on Hertzian contact declared parts/03-classical-mechanics/13-continuum-elasticity.tex:2477
depends_on Coulomb's law of torsion declared parts/03-classical-mechanics/13-continuum-elasticity.tex:2186
depends_on Conversion among the moduli declared parts/03-classical-mechanics/13-continuum-elasticity.tex:1036
depends_on Moment and curvature declared parts/03-classical-mechanics/13-continuum-elasticity.tex:1895
depends_on The third cubic constant is measured, and it is not small declared appendices/A-long-proofs.tex:32962
depends_on Boussinesq's point-force solution, quoted declared appendices/A-long-proofs.tex:33755