proposition A.684 The plate energy

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proposition A.684: The plate energyA.684definition 30.63: Flexural rigidity30.63lemma A.681: Strains under the Kirchhoff hypothesisA.681proposition A.682: The plane-stress lawA.682lemma A.685: The Gaussian-curvature term is a null LagrangianA.685theorem A.688: The Kirchhoff plate equationA.688proof : app:A-long-proofs@proof-406proofproposition 30.33: Conversion among the moduli30.33proposition 30.51: Moment and curvature30.51proposition 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 A.680: Kirchhoff kinematicsA.680definition 30.6: Linear strain and infinitesimal rotation30.6proof : app:A-long-proofs@proof-404proofequation 30.21: eq:elast-hooke-isotropic30.21definition A.689: Edge resultantsA.689proof : app:A-long-proofs@proof-405proofproof : app:A-long-proofs@proof-407prooflemma A.687: Kinetic energyA.687lemma 16.18: Fundamental lemma16.18remark A.690: Poisson's count, and why it cannot be rightA.690theorem A.691: Kirchhoff's edge conditions and the corner forceA.691proof : app:A-long-proofs@proof-409proof

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typedirectionnode provenancewhere
depends_on Flexural rigidity declared appendices/A-long-proofs.tex:33260
depends_on Strains under the Kirchhoff hypothesis declared appendices/A-long-proofs.tex:33260
depends_on The plane-stress law declared appendices/A-long-proofs.tex:33260
depends_on The Gaussian-curvature term is a null Lagrangian declared appendices/A-long-proofs.tex:33344
depends_on The Kirchhoff plate equation declared appendices/A-long-proofs.tex:33446
proves app:A-long-proofs@proof-406 declared appendices/A-long-proofs.tex:33264