proposition 30.9 Principal strains

open in the book · parts/03-classical-mechanics/13-continuum-elasticity.tex:267 · p. 1010

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proposition 30.9: Principal strains30.9definition 30.6: Linear strain and infinitesimal rotation30.6theorem 5.79: Spectral theorem for a self-adjoint operator5.79example 30.10: Simple shear and pure shear are the same strain30.10proof : ch:13-continuum-elasticity@proof-3proofdefinition 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 two30.7corollary 5.72: Existence of an eigenvalue over ℂ5.72definition 5.41: Adjoint5.41theorem 5.40: Rank–nullity5.40definition 30.20: Pressure and deviatoric stress30.20theorem 5.80: Simultaneous diagonalization of commuting self-adjoint operators5.80theorem 5.84: Spectral theorem for a real symmetric operator5.84theorem 28.33: Normal modes28.33theorem 29.16: Principal axes29.16proof : ch:03-linear-algebra-representations@proof-31proof

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typedirectionnode provenancewhere
depends_on Linear strain and infinitesimal rotation declared parts/03-classical-mechanics/13-continuum-elasticity.tex:273
depends_on Spectral theorem for a self-adjoint operator declared parts/03-classical-mechanics/13-continuum-elasticity.tex:273
depends_on Simple shear and pure shear are the same strain declared parts/03-classical-mechanics/13-continuum-elasticity.tex:313
proves ch:13-continuum-elasticity@proof-3 declared parts/03-classical-mechanics/13-continuum-elasticity.tex:276