definition 30.31 The engineering moduli
open in the book ·
parts/03-classical-mechanics/13-continuum-elasticity.tex:954
· p. 1017
- ground object -- no derivation owed
Rests on
-
depends_on
definition 30.20
Pressure and deviatoric stress
¶
-
depends_on
proposition 30.19
The stress tensor is symmetric
¶
-
depends_on
definition 30.17
Traction
¶
-
depends_on
definition 7.126
Line and surface integrals
¶
- depends_on definition 7.98 Functions of class $C^{1}$ ¶
- depends_on definition 7.125 Multiple integral ¶
-
depends_on
definition 30.2
Representative volume element; continuum field
¶
- depends_on definition 7.97 Partial derivative; gradient ¶
-
depends_on
definition 7.126
Line and surface integrals
¶
-
depends_on
theorem 30.18
Cauchy: the stress tensor exists
¶
- depends_on definition 30.17 Traction ¶ ↺
-
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-8 ¶
-
depends_on
definition 30.17
Traction
¶
-
depends_on
theorem 5.79
Spectral theorem for a self-adjoint operator
¶
-
depends_on
corollary 5.72
Existence of an eigenvalue over $\C$
¶
-
depends_on
theorem 8.19
Fundamental theorem of algebra
¶
- depends_on theorem 8.18 Liouville ¶
- proves proof ch:06-complex-analysis@proof-13 ¶
-
depends_on
theorem 5.71
The eigenvalues are the roots of the characteristic
polynomial
¶
- depends_on definition 5.70 Characteristic polynomial ¶
- depends_on definition 5.69 Eigenvector, eigenvalue, eigenspace ¶
- depends_on proposition 5.49 Injective, surjective, invertible ¶
- proves proof ch:03-linear-algebra-representations@proof-26 ¶
- proves proof ch:03-linear-algebra-representations@proof-27 ¶
-
depends_on
theorem 8.19
Fundamental theorem of algebra
¶
-
depends_on
definition 5.41
Adjoint
¶
-
depends_on
definition 5.18
Inner product
¶
- depends_on definition 4.33 Vector space ¶
-
depends_on
definition 5.37
Linear transformation
¶
- depends_on definition 4.33 Vector space ¶ ↺
-
depends_on
definition 5.18
Inner product
¶
-
depends_on
theorem 5.40
Rank–nullity
¶
-
depends_on
definition 5.15
Basis
¶
- depends_on definition 5.12 Subspace generated by a set of vectors ¶
- depends_on definition 5.14 Linear independence ¶
-
depends_on
definition 5.39
Kernel, image, nullity, rank
¶
- depends_on definition 5.37 Linear transformation ¶ ↺
- depends_on definition 5.7 Vector subspace ¶
- proves proof ch:03-linear-algebra-representations@proof-12 ¶
-
depends_on
lemma 5.38
Exchange and completion
¶
- depends_on definition 5.15 Basis ¶ ↺
- depends_on definition 5.12 Subspace generated by a set of vectors ¶ ↺
- depends_on definition 5.14 Linear independence ¶ ↺
- proves proof ch:03-linear-algebra-representations@proof-11 ¶
- proves proof ch:03-linear-algebra-representations@proof-13 ¶
-
depends_on
definition 5.15
Basis
¶
- proves proof ch:03-linear-algebra-representations@proof-31 ¶
-
depends_on
corollary 5.72
Existence of an eigenvalue over $\C$
¶
-
depends_on
proposition 30.19
The stress tensor is symmetric
¶
- depends_on equation 30.21 eq:elast-hooke-isotropic ¶
Supports
-
depends_on
phenomenon 30.70
Hertzian contact
¶
-
depends_on
definition A.698
The Hertz contact problem
¶
-
depends_on
lemma A.700
The displacement produced by an elliptic pressure
¶
-
depends_on
theorem A.702
Hertz's solution
¶
- depends_on example A.703 The numbers of the chapter, recomputed ¶
- depends_on remark A.704 $E^{*}$ in two roles, and one trap ¶
- depends_on remark A.705 The dangerous stress is below the surface ¶
-
depends_on
theorem A.702
Hertz's solution
¶
-
depends_on
proposition A.701
The two-body compliance rule
¶
- depends_on theorem A.702 Hertz's solution ¶ ↺
- depends_on remark A.699 The third condition is not decoration ¶
- depends_on theorem A.702 Hertz's solution ¶ ↺
-
depends_on
lemma A.700
The displacement produced by an elliptic pressure
¶
- depends_on example A.703 The numbers of the chapter, recomputed ¶ ↺
- depends_on example 30.71 Contact stresses are enormous ¶
-
depends_on
definition A.698
The Hertz contact problem
¶
-
depends_on
phenomenon 30.60
Coulomb's law of torsion
¶
- depends_on example 30.61 A torsion fibre as a force sensor ¶
- depends_on phenomenon 34.3 The stiffness of a twisted wire is geometric ¶
- depends_on remark 30.62 Saint-Venant's theory: non-circular sections warp ¶
- tests experiment Coulomb: the torsion pendulum ¶
-
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 remark A.686 Why the operator comes out as $\nabla^{4}$ ¶
-
depends_on
theorem A.688
The Kirchhoff plate equation
¶
- depends_on remark A.690 Poisson's count, and why it cannot be right ¶
- depends_on theorem A.691 Kirchhoff's edge conditions and the corner force ¶
-
depends_on
lemma A.685
The Gaussian-curvature term is a null Lagrangian
¶
-
depends_on
proposition A.682
The plane-stress law
¶
-
depends_on
definition A.689
Edge resultants
¶
- depends_on remark A.690 Poisson's count, and why it cannot be right ¶ ↺
- depends_on theorem A.691 Kirchhoff's edge conditions and the corner force ¶ ↺
- depends_on proposition A.684 The plate energy ¶ ↺
- depends_on remark A.683 Where the factor $1-\nu^{2}$ comes from ¶
-
depends_on
definition A.689
Edge resultants
¶
-
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 30.51
Moment and curvature
¶
-
depends_on
definition A.680
Kirchhoff kinematics
¶
-
depends_on
lemma A.687
Kinetic energy
¶
- depends_on theorem A.688 The Kirchhoff plate equation ¶ ↺
-
depends_on
lemma A.681
Strains under the Kirchhoff hypothesis
¶
- depends_on proposition A.684 The plate energy ¶ ↺
-
depends_on
lemma A.687
Kinetic energy
¶
- depends_on definition 30.63 Flexural rigidity ¶ ↺
-
depends_on
phenomenon 30.52
Euler buckling
¶
- depends_on example 30.53 A steel rod buckles at a twentieth of its crushing load ¶
- depends_on remark 30.54 Other end conditions, and what buckling is variationally ¶
- depends_on remark 30.55 Beyond the critical load: the elastica ¶
- depends_on remark 30.68 Shells carry load in a different way ¶ ↺
-
depends_on
theorem 30.56
The beam equation
¶
- depends_on example 30.58 A steel ruler ¶
-
depends_on
proposition 30.57
Bending waves are dispersive
¶
- depends_on example 30.58 A steel ruler ¶ ↺
- depends_on remark 30.59 Where Euler–Bernoulli fails ¶
-
depends_on
definition A.680
Kirchhoff kinematics
¶
- depends_on remark A.676 The third cubic constant is measured, and it is not small ¶
-
depends_on
theorem A.695
Boussinesq's point-force solution, quoted
¶
- depends_on definition A.698 The Hertz contact problem ¶ ↺
-
depends_on
lemma A.697
Surface displacement under a distributed pressure
¶
- depends_on lemma A.700 The displacement produced by an elliptic pressure ¶ ↺
- depends_on proposition A.701 The two-body compliance rule ¶ ↺
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 |
|---|---|---|---|---|
cites |
→ | Mémoire sur l'équilibre et le mouvement des corps élastiques | derived | parts/03-classical-mechanics/13-continuum-elasticity.tex:962 |
cites |
→ | A Course of Lectures on Natural Philosophy and the Mechanical Arts | derived | parts/03-classical-mechanics/13-continuum-elasticity.tex:960 |
depends_on |
→ | Pressure and deviatoric stress | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:969 |
depends_on |
→ | eq:elast-hooke-isotropic | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:969 |
depends_on |
← | Hertzian contact | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:2477 |
depends_on |
← | Coulomb's law of torsion | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:2186 |
depends_on |
← | Conversion among the moduli | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:1036 |
depends_on |
← | Moment and curvature | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:1895 |
depends_on |
← | The third cubic constant is measured, and it is not small | declared | appendices/A-long-proofs.tex:32962 |
depends_on |
← | Boussinesq's point-force solution, quoted | declared | appendices/A-long-proofs.tex:33755 |