proposition 30.30 Stability bounds
open in the book ·
parts/03-classical-mechanics/13-continuum-elasticity.tex:921
· p. 1017
Rests on
- depends_on equation 30.23 eq:elast-energy-density ¶
-
depends_on
theorem 5.116
Sylvester's law of inertia
¶
-
depends_on
definition 5.110
Bilinear map
¶
-
depends_on
definition 5.37
Linear transformation
¶
- depends_on definition 4.33 Vector space ¶
-
depends_on
definition 5.37
Linear transformation
¶
-
depends_on
definition 5.111
Symmetric and antisymmetric forms
¶
- depends_on definition 5.110 Bilinear map ¶ ↺
- depends_on equation 5.137 eq:lin-bilinear-matrix ¶
- depends_on equation 5.139 eq:lin-bilinear-congruence ¶
- proves proof ch:03-linear-algebra-representations@proof-53 ¶
-
depends_on
definition 5.110
Bilinear map
¶
- proves proof ch:13-continuum-elasticity@proof-13 ¶
Supports
-
depends_on
phenomenon 30.43
Two bulk wave speeds
¶
- depends_on phenomenon 30.47 The three seismic phases ¶
- depends_on remark 30.46 Why the plane-wave route, and not the potentials ¶
-
depends_on
phenomenon 30.32
Poisson contraction
¶
-
depends_on
proposition 30.33
Conversion among the moduli
¶
-
depends_on
definition 30.63
Flexural rigidity
¶
-
depends_on
proposition A.684
The plate energy
¶
- depends_on lemma A.685 The Gaussian-curvature term is a null Lagrangian ¶
- depends_on theorem A.688 The Kirchhoff plate equation ¶
-
depends_on
proposition A.682
The plane-stress law
¶
- depends_on definition A.689 Edge resultants ¶
- depends_on proposition A.684 The plate energy ¶ ↺
- depends_on remark A.683 Where the factor $1-\nu^{2}$ comes from ¶
-
depends_on
proposition 30.66
Chladni scaling
¶
- depends_on phenomenon 30.65 Chladni figures ¶
- depends_on remark A.704 $E^{*}$ in two roles, and one trap ¶
- depends_on remark A.686 Why the operator comes out as $\nabla^{4}$ ¶
- depends_on remark A.683 Where the factor $1-\nu^{2}$ comes from ¶ ↺
- depends_on remark 30.68 Shells carry load in a different way ¶
-
depends_on
theorem 30.64
The Kirchhoff plate equation
¶
- depends_on phenomenon 30.65 Chladni figures ¶ ↺
- depends_on proposition 30.66 Chladni scaling ¶ ↺
- depends_on remark 30.67 Germain, Kirchhoff, and the edge conditions ¶
-
depends_on
proposition A.684
The plate energy
¶
- depends_on example 30.35 From single crystals to the isotropic aggregate ¶
- depends_on proposition A.682 The plane-stress law ¶ ↺
-
depends_on
proposition 30.44
The speed ratio is fixed by Poisson's ratio
¶
- depends_on example 30.45 Elastic waves in steel, and the distance to a source ¶
- depends_on remark 30.36 How the moduli are actually measured ¶
-
depends_on
definition 30.63
Flexural rigidity
¶
-
depends_on
proposition 30.33
Conversion among the moduli
¶
-
depends_on
proposition 30.34
Minimum of the potential energy
¶
- depends_on example 30.35 From single crystals to the isotropic aggregate ¶ ↺
- depends_on theorem 30.42 Uniqueness in elastodynamics ¶
Neighborhood
Every logical edge within two steps of this node.
- declared and complete
- partly declared
- a check failed
- not graded
- declared in the source
- inferred from structure
Edges
| type | direction | node | provenance | where |
|---|---|---|---|---|
depends_on |
→ | eq:elast-energy-density | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:928 |
depends_on |
→ | Sylvester's law of inertia | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:928 |
depends_on |
← | Two bulk wave speeds | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:1461 |
depends_on |
← | Poisson contraction | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:986 |
depends_on |
← | Minimum of the potential energy | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:1073 |
depends_on |
← | Uniqueness in elastodynamics | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:1416 |
proves |
← | ch:13-continuum-elasticity@proof-13 | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:931 |