definition 30.63 Flexural rigidity

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definition 30.63: Flexural rigidity30.63proposition 30.33: Conversion among the moduli30.33proposition 30.51: Moment and curvature30.51proposition A.684: The plate energyA.684proposition A.682: The plane-stress lawA.682proposition 30.66: Chladni scaling30.66remark A.704: E^* in two roles, and one trapA.704remark A.686: Why the operator comes out as \nabla^4A.686remark A.683: Where the factor 1-ν^2 comes fromA.683remark 30.68: Shells carry load in a different way30.68theorem 30.64: The Kirchhoff plate equation30.64definition 30.31: The engineering moduli30.31phenomenon 30.32: Poisson contraction30.32example 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-15proofequation 30.21: eq:elast-hooke-isotropic30.21definition A.680: Kirchhoff kinematicsA.680phenomenon 30.52: Euler buckling30.52theorem 30.56: The beam equation30.56proof : ch:13-continuum-elasticity@proof-27prooflemma A.681: Strains under the Kirchhoff hypothesisA.681lemma A.685: The Gaussian-curvature term is a null LagrangianA.685theorem A.688: The Kirchhoff plate equationA.688proof : app:A-long-proofs@proof-406proofdefinition A.689: Edge resultantsA.689proof : app:A-long-proofs@proof-405proofphenomenon 30.65: Chladni figures30.65proof : ch:13-continuum-elasticity@proof-33prooftheorem A.702: Hertz's solutionA.702theorem 16.38: Euler–Poisson equation16.38remark 30.67: Germain, Kirchhoff, and the edge conditions30.67proof : ch:13-continuum-elasticity@prooflink-2proof

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typedirectionnode provenancewhere
depends_on Conversion among the moduli declared parts/03-classical-mechanics/13-continuum-elasticity.tex:2276
depends_on Moment and curvature declared parts/03-classical-mechanics/13-continuum-elasticity.tex:2276
depends_on The plate energy declared appendices/A-long-proofs.tex:33260
depends_on The plane-stress law declared appendices/A-long-proofs.tex:33171
depends_on Chladni scaling declared parts/03-classical-mechanics/13-continuum-elasticity.tex:2372
depends_on $E^{*}$ in two roles, and one trap declared appendices/A-long-proofs.tex:34167
depends_on Why the operator comes out as $\nabla^{4}$ declared appendices/A-long-proofs.tex:33386
depends_on Where the factor $1-\nu^{2}$ comes from declared appendices/A-long-proofs.tex:33239
depends_on Shells carry load in a different way declared parts/03-classical-mechanics/13-continuum-elasticity.tex:2431
depends_on The Kirchhoff plate equation declared parts/03-classical-mechanics/13-continuum-elasticity.tex:2293