lemma A.681 Strains under the Kirchhoff hypothesis

open in the book · appendices/A-long-proofs.tex:33100 · p. 3124

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lemma A.681: Strains under the Kirchhoff hypothesisA.681definition A.680: Kirchhoff kinematicsA.680definition 30.6: Linear strain and infinitesimal rotation30.6proposition A.684: The plate energyA.684proof : app:A-long-proofs@proof-404proofproposition 30.51: Moment and curvature30.51lemma A.687: Kinetic energyA.687definition 13.91: Symmetric and antisymmetric parts13.91equation 30.2: eq:elast-displacement30.2definition 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 strain30.10proposition 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 30.63: Flexural rigidity30.63proposition 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-406proof

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typedirectionnode provenancewhere
depends_on Kirchhoff kinematics declared appendices/A-long-proofs.tex:33112
depends_on Linear strain and infinitesimal rotation declared appendices/A-long-proofs.tex:33112
depends_on The plate energy declared appendices/A-long-proofs.tex:33260
proves app:A-long-proofs@proof-404 declared appendices/A-long-proofs.tex:33115