theorem 5.116 Sylvester's law of inertia
open in the book ·
parts/02-mathematical-methods/03-linear-algebra-representations.tex:4989
· p. 154
Rests on
-
depends_on
definition 5.110
Bilinear map
¶
-
depends_on
definition 5.37
Linear transformation
¶
-
depends_on
definition 4.33
Vector space
¶
-
depends_on
definition 4.8
Commutativity; abelian structure
¶
- depends_on definition 4.4 Internal binary operation; magma ¶
- depends_on definition 4.32 Field ¶
- depends_on definition 4.31 Module ¶
-
depends_on
definition 4.8
Commutativity; abelian structure
¶
-
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 ¶
Supports
-
depends_on
definition 5.117
Signature
¶
-
depends_on
proposition 5.94
Principal axes of a real quadratic form
¶
- depends_on proposition 5.95 The focal polar equation of a conic ¶
-
depends_on
proposition 5.94
Principal axes of a real quadratic form
¶
-
depends_on
definition 10.6
Type of a second-order operator
¶
-
depends_on
definition 10.79
Parabolic boundary
¶
-
depends_on
theorem 10.80
Parabolic maximum principle
¶
- depends_on corollary 10.81 Uniqueness for the heat equation ¶
- depends_on proposition A.163 The viscous problem produces the entropy inequality ¶
-
depends_on
theorem 10.80
Parabolic maximum principle
¶
- depends_on example 10.9 ex:pde-three-types ¶
- depends_on proposition 10.25 The backward heat problem is ill posed ¶
- depends_on theorem A.83 Local canonical form for an elliptic operator with Hölder coefficients ¶
-
depends_on
theorem 10.8
The type is a coordinate invariant
¶
-
depends_on
lemma A.90
Affine normalization
¶
- depends_on lemma A.91 Smallness after rescaling ¶
-
depends_on
proposition 10.13
Canonical form in two variables
¶
- depends_on theorem A.83 Local canonical form for an elliptic operator with Hölder coefficients ¶ ↺
-
depends_on
theorem 10.55
d'Alembert's formula
¶
- depends_on corollary 10.56 Domain of dependence and influence ¶
- depends_on theorem 10.59 Kirchhoff's formula ¶
-
depends_on
proposition 10.11
What a characteristic surface is
¶
-
depends_on
corollary 10.12
Characteristics of the three canonical operators
¶
- depends_on corollary 10.60 Huygens' principle in three space dimensions ¶
-
depends_on
definition A.102
Normal Cauchy problem of order $k$
¶
- depends_on definition A.103 First-order quasilinear system with zero data ¶
- depends_on lemma A.105 Formal reduction of a normal problem ¶
- depends_on theorem 10.22 Cauchy–Kovalevskaya ¶
-
depends_on
corollary 10.12
Characteristics of the three canonical operators
¶
-
depends_on
lemma A.90
Affine normalization
¶
-
depends_on
definition 10.79
Parabolic boundary
¶
-
depends_on
proposition 30.30
Stability bounds
¶
-
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 proposition A.682 The plane-stress law ¶
- depends_on proposition 30.66 Chladni scaling ¶
- 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 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 ¶
-
depends_on
phenomenon 30.43
Two bulk wave speeds
¶
- depends_on proposition 5.94 Principal axes of a real quadratic form ¶ ↺
- depends_on remark 7.107 What the Hessian is for ¶
-
depends_on
theorem 5.86
Simultaneous diagonalization of a definite pencil
¶
- depends_on corollary 5.89 Rayleigh–Ritz ¶
-
depends_on
proposition 5.88
Rayleigh quotient of a definite pencil
¶
-
depends_on
corollary 5.91
The operator norm of a real array
¶
- depends_on proposition 5.92 The eigenvalues do not control the norm ¶
- depends_on corollary 5.89 Rayleigh–Ritz ¶ ↺
-
depends_on
corollary 5.91
The operator norm of a real array
¶
-
depends_on
theorem 28.33
Normal modes
¶
- depends_on example 28.39 The linear triatomic molecule ¶
- depends_on proposition 28.40 Modes and dispersion of the loaded string ¶
- depends_on remark 28.34 Part II owes the simultaneous diagonalization of two quadratic forms ¶
- depends_on theorem 10.8 The type is a coordinate invariant ¶ ↺
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 |
→ | Bilinear map | declared | parts/02-mathematical-methods/03-linear-algebra-representations.tex:4998 |
depends_on |
→ | Symmetric and antisymmetric forms | declared | parts/02-mathematical-methods/03-linear-algebra-representations.tex:4998 |
depends_on |
→ | eq:lin-bilinear-congruence | declared | parts/02-mathematical-methods/03-linear-algebra-representations.tex:4998 |
depends_on |
← | Signature | declared | parts/02-mathematical-methods/03-linear-algebra-representations.tex:5056 |
depends_on |
← | Type of a second-order operator | declared | parts/02-mathematical-methods/08-pdes.tex:160 |
depends_on |
← | Stability bounds | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:928 |
depends_on |
← | Principal axes of a real quadratic form | declared | parts/02-mathematical-methods/03-linear-algebra-representations.tex:4107 |
depends_on |
← | What the Hessian is for | declared | parts/02-mathematical-methods/05-real-analysis.tex:3255 |
depends_on |
← | Simultaneous diagonalization of a definite pencil | declared | parts/02-mathematical-methods/03-linear-algebra-representations.tex:3781 |
depends_on |
← | Normal modes | declared | parts/03-classical-mechanics/11-oscillations-waves.tex:1127 |
depends_on |
← | The type is a coordinate invariant | declared | parts/02-mathematical-methods/08-pdes.tex:190 |
proves |
← | ch:03-linear-algebra-representations@proof-53 | declared | parts/02-mathematical-methods/03-linear-algebra-representations.tex:5001 |