example 30.10 Simple shear and pure shear are the same strain

open in the book · parts/03-classical-mechanics/13-continuum-elasticity.tex:288 · p. 1010

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example 30.10: Simple shear and pure shear are the same strain30.10definition 30.6: Linear strain and infinitesimal rotation30.6proposition 30.9: Principal strains30.9definition 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^2/230.13lemma 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 30.7: Strain is a Cartesian tensor of rank two30.7theorem 5.79: Spectral theorem for a self-adjoint operator5.79proof : ch:13-continuum-elasticity@proof-3proof

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depends_on Linear strain and infinitesimal rotation declared parts/03-classical-mechanics/13-continuum-elasticity.tex:313
depends_on Principal strains declared parts/03-classical-mechanics/13-continuum-elasticity.tex:313