theorem 30.21 Cauchy's equation of motion

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theorem 30.21: Cauchy's equation of motion30.21theorem 7.133: Gauss7.133theorem 30.18: Cauchy: the stress tensor exists30.18definition 30.22: Boundary conditions of elastostatics30.22proposition 30.23: Virtual work; the weak form30.23proposition 31.16: Hydrostatic balance31.16remark 30.69: Saint-Venant's principle, and its exact status30.69theorem 30.40: Navier–Cauchy equations30.40theorem 31.22: Euler's equations of motion31.22proof : ch:13-continuum-elasticity@proof-9proofdefinition 7.127: Simple regions7.127remark 7.128: What the derivations below take as given7.128theorem 7.43: Fundamental theorem of calculus, II7.43lemma A.708: The disturbance flux vanishesA.708lemma A.712: The force is a far-field integralA.712lemma A.117: Laplacian in orthogonal coordinatesA.117lemma 44.10: Divergence theorem on (M,g)44.10lemma 31.11: Transport theorem for a material volume31.11lemma 106.86: A shift of a divergent integral leaves a surface term106.86lemma 10.44: Green's identities10.44lemma 10.58: Darboux's equation for spherical means10.58proposition 23.54: The geometrical amplitude diverges23.54proposition 10.57: Energy in a backward cone10.57theorem 16.36: Euler–Lagrange equations for several independent variables16.36theorem 32.6: Evolution of phase volume32.6proof : ch:05-real-analysis@proof-79proofdefinition 30.17: Traction30.17definition 13.5: Tensor under orthogonal transformations13.5definition 30.24: The elasticity tensor30.24definition 31.1: Fluid31.1proposition 30.19: The stress tensor is symmetric30.19proposition 30.74: The maximum shear stress, and its indifference to pressure30.74remark 30.72: Stress concentration30.72theorem A.695: Boussinesq's point-force solution, quotedA.695proof : ch:13-continuum-elasticity@proof-7proofdefinition 10.24: Well-posed problem10.24proposition 30.50: Love waves need a slow surface layer30.50proposition 30.48: Rayleigh's secular equation30.48phenomenon 30.70: Hertzian contact30.70proposition 30.34: Minimum of the potential energy30.34neighborhood truncated

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typedirectionnode provenancewhere
depends_on Gauss declared parts/03-classical-mechanics/13-continuum-elasticity.tex:668
depends_on Cauchy: the stress tensor exists declared parts/03-classical-mechanics/13-continuum-elasticity.tex:668
depends_on Boundary conditions of elastostatics declared parts/03-classical-mechanics/13-continuum-elasticity.tex:703
depends_on Virtual work; the weak form declared parts/03-classical-mechanics/13-continuum-elasticity.tex:719
depends_on Hydrostatic balance declared parts/03-classical-mechanics/14-fluid-dynamics.tex:416
depends_on Saint-Venant's principle, and its exact status declared parts/03-classical-mechanics/13-continuum-elasticity.tex:2458
depends_on Navier–Cauchy equations declared parts/03-classical-mechanics/13-continuum-elasticity.tex:1351
depends_on Euler's equations of motion declared parts/03-classical-mechanics/14-fluid-dynamics.tex:596
proves ch:13-continuum-elasticity@proof-9 declared parts/03-classical-mechanics/13-continuum-elasticity.tex:671