example 30.77 Why glass is weak, and thin glass is not

open in the book · parts/03-classical-mechanics/13-continuum-elasticity.tex:2730 · p. 1037

example -- no derivation owed by its kind

Rests on

depends_on equation 30.63 eq:elast-griffith ¶
depends_on proposition 30.76 Griffith's criterion ¶
- depends_on equation 30.23 eq:elast-energy-density ¶
- depends_on remark 30.72 Stress concentration ¶
  - depends_on equation 30.21 eq:elast-hooke-isotropic ¶
  - depends_on theorem 30.18 Cauchy: the stress tensor exists ¶
    - depends_on definition 30.17 Traction ¶
      - depends_on definition 7.126 Line and surface integrals ¶
      - depends_on definition 30.2 Representative volume element; continuum field ¶
    - depends_on definition 13.5 Tensor under orthogonal transformations ¶
      - depends_on definition 13.4 Orthogonal coordinate transformation ¶
    - proves proof ch:13-continuum-elasticity@proof-7 ¶
- proves proof ch:13-continuum-elasticity@proof-37 ¶

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type	direction	node	provenance	where
`cites`	→	The phenomena of rupture and flow in solids	derived	parts/03-classical-mechanics/13-continuum-elasticity.tex:2753
`depends_on`	→	eq:elast-griffith	declared	parts/03-classical-mechanics/13-continuum-elasticity.tex:2755
`depends_on`	→	Griffith's criterion	declared	parts/03-classical-mechanics/13-continuum-elasticity.tex:2755