definition 30.6 Linear strain and infinitesimal rotation
open in the book ·
parts/03-classical-mechanics/13-continuum-elasticity.tex:189
· p. 1009
- ground object -- no derivation owed
Rests on
- depends_on definition 13.91 Symmetric and antisymmetric parts ¶
- depends_on equation 30.2 eq:elast-displacement ¶
Supports
-
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 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 remark A.692 The corner force is real, and you can feel it ¶
-
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.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
lemma A.685
The Gaussian-curvature term is a null Lagrangian
¶
-
depends_on
proposition A.684
The plate energy
¶
-
depends_on
lemma A.687
Kinetic energy
¶
-
depends_on
definition 30.24
The elasticity tensor
¶
-
depends_on
definition 30.37
Voigt notation
¶
- depends_on remark 30.39 The rari-constant controversy, decided by measurement ¶
-
depends_on
phenomenon 30.28
Hooke's law
¶
-
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 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 remark 30.36 How the moduli are actually measured ¶
-
depends_on
proposition 30.33
Conversion among the moduli
¶
- depends_on remark 30.78 Anharmonicity: what the quadratic energy also suppresses ¶
-
depends_on
phenomenon 30.32
Poisson contraction
¶
-
depends_on
proposition 30.25
Twenty-one constants
¶
- depends_on definition 30.37 Voigt notation ¶ ↺
-
depends_on
proposition 30.38
The Cauchy relations
¶
- depends_on remark 30.39 The rari-constant controversy, decided by measurement ¶ ↺
-
depends_on
theorem A.675
Three constants for a cubic crystal, two for an
isotropic solid
¶
- depends_on remark A.676 The third cubic constant is measured, and it is not small ¶
- depends_on proposition 30.38 The Cauchy relations ¶ ↺
- depends_on remark 30.78 Anharmonicity: what the quadratic energy also suppresses ¶ ↺
- depends_on theorem A.675 Three constants for a cubic crystal, two for an isotropic solid ¶ ↺
-
depends_on
definition 30.37
Voigt notation
¶
-
depends_on
definition 30.11
Green strain
¶
-
depends_on
proposition 30.12
The Green strain measures length exactly
¶
- depends_on example 30.13 A rigid rotation forges a strain of $-\theta^{2}/2$ ¶
-
depends_on
proposition 30.12
The Green strain measures length exactly
¶
- depends_on example 30.13 A rigid rotation forges a strain of $-\theta^{2}/2$ ¶ ↺
- depends_on example 30.10 Simple shear and pure shear are the same strain ¶
- depends_on lemma A.681 Strains under the Kirchhoff hypothesis ¶ ↺
-
depends_on
proposition 30.14
Saint-Venant compatibility is necessary
¶
- depends_on theorem 30.15 Compatibility is sufficient on a simply connected body ¶
- depends_on proposition 30.8 The trace is the fractional volume change ¶
-
depends_on
proposition 30.9
Principal strains
¶
- depends_on example 30.10 Simple shear and pure shear are the same strain ¶ ↺
- depends_on proposition 30.7 Strain is a Cartesian tensor of rank two ¶
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 |
→ | Symmetric and antisymmetric parts | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:205 |
depends_on |
→ | eq:elast-displacement | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:205 |
depends_on |
← | Kirchhoff kinematics | declared | appendices/A-long-proofs.tex:33097 |
depends_on |
← | The elasticity tensor | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:778 |
depends_on |
← | Green strain | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:331 |
depends_on |
← | A rigid rotation forges a strain of $-\theta^{2}/2$ | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:384 |
depends_on |
← | Simple shear and pure shear are the same strain | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:313 |
depends_on |
← | Strains under the Kirchhoff hypothesis | declared | appendices/A-long-proofs.tex:33112 |
depends_on |
← | Saint-Venant compatibility is necessary | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:402 |
depends_on |
← | The trace is the fractional volume change | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:250 |
depends_on |
← | Principal strains | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:273 |
depends_on |
← | Strain is a Cartesian tensor of rank two | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:215 |