definition 13.5 Tensor under orthogonal transformations
open in the book ·
parts/02-mathematical-methods/11-manifolds-tensors-curvature.tex:305
· p. 453
- ground object -- no derivation owed
Rests on
-
depends_on
definition 13.4
Orthogonal coordinate transformation
¶
- depends_on definition 13.3 Orthogonal coordinate system ¶
Supports
-
depends_on
definition 19.42
Inertia tensor
¶
-
depends_on
definition 29.13
Inertia tensor, continuum form
¶
-
depends_on
definition 29.19
Inertia ellipsoid
¶
-
depends_on
theorem 29.29
Poinsot's construction
¶
- depends_on remark 29.32 What the linearization is entitled to conclude ¶
- depends_on remark 29.30 Polhode and herpolhode ¶
-
depends_on
theorem 29.29
Poinsot's construction
¶
-
depends_on
example 29.23
The polar moment of the Earth, and what it reveals
¶
- depends_on phenomenon 29.34 Free nutation of the Earth ¶
- depends_on proposition 49.17 Magnetic-dipole spin-down ¶
- depends_on proposition 29.14 Angular momentum and kinetic energy ¶
-
depends_on
proposition 29.15
Positivity
¶
- depends_on definition 29.19 Inertia ellipsoid ¶ ↺
-
depends_on
theorem 29.16
Principal axes
¶
- depends_on definition 29.19 Inertia ellipsoid ¶ ↺
- depends_on definition 29.35 The Lagrange top ¶
- depends_on definition 29.18 Classification of tops ¶
- depends_on phenomenon 29.31 The intermediate-axis instability ¶
- depends_on proposition 29.33 Dissipation drives a free body to its largest moment ¶
- depends_on proposition 29.17 Triangle inequalities ¶
- depends_on theorem 29.25 Euler's equations ¶
-
depends_on
proposition 29.24
MacCullagh's formula
¶
-
depends_on
phenomenon 29.49
Precession of the equinoxes
¶
- depends_on proposition 29.50 The principal nutation ¶
-
depends_on
phenomenon 29.49
Precession of the equinoxes
¶
- depends_on proposition 29.22 Perpendicular-axis theorem ¶
-
depends_on
theorem 29.20
Parallel-axis theorem
¶
- depends_on corollary 29.21 The centre of mass minimizes the moment ¶
- depends_on theorem 29.16 Principal axes ¶ ↺
-
depends_on
definition 29.19
Inertia ellipsoid
¶
- depends_on example 19.45 The uniform solid sphere ¶
- depends_on proposition 19.43 The moment of inertia is a quadratic form in the axis ¶
-
depends_on
definition 29.13
Inertia tensor, continuum form
¶
- depends_on definition 29.13 Inertia tensor, continuum form ¶ ↺
-
depends_on
lemma 30.26
Isotropic Cartesian tensors of rank four
¶
-
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
phenomenon 30.28
Hooke's law
¶
- depends_on notation 30.1 Strain and displacement share a letter ¶
- depends_on proposition 30.7 Strain is a Cartesian tensor of rank two ¶
- depends_on proposition 13.96 The cross product is an axial vector ¶
-
depends_on
proposition 13.6
Levi-Civita identities in three dimensions
¶
- depends_on proposition 13.96 The cross product is an axial vector ¶ ↺
- depends_on proposition 13.95 The elementary cross-product identities ¶
- depends_on proposition 19.43 The moment of inertia is a quadratic form in the axis ¶ ↺
- depends_on remark 13.7 What the classification is used for ¶
-
depends_on
theorem 30.18
Cauchy: the stress tensor exists
¶
-
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
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 31.1
Fluid
¶
-
depends_on
definition 31.21
Ideal fluid
¶
-
depends_on
theorem 31.22
Euler's equations of motion
¶
- depends_on lemma A.712 The force is a far-field integral ¶
- depends_on phenomenon 31.88 Sound travels at the adiabatic speed ¶
- depends_on proposition A.797 The outer limit loses a boundary condition ¶
- depends_on proposition 31.80 Rayleigh's circulation criterion ¶
- depends_on proposition 52.24 The p-mode cavity ¶
- depends_on remark 31.23 Boundary conditions, and what the ideal model omits ¶
- depends_on theorem 31.24 Bernoulli ¶
- depends_on theorem 31.64 Kelvin's circulation theorem ¶
- depends_on theorem 31.37 The Navier–Stokes equations ¶
- depends_on theorem 31.91 Rankine–Hugoniot jump conditions ¶
- depends_on theorem 31.77 Rayleigh's inflexion-point criterion ¶
-
depends_on
theorem 31.22
Euler's equations of motion
¶
-
depends_on
definition 31.2
Knudsen number
¶
- depends_on remark 31.3 When the continuum picture is allowed ¶
-
depends_on
definition 31.32
Newtonian fluid; dynamic and kinematic viscosity
¶
- depends_on remark 31.35 Non-Newtonian fluids are out of scope ¶
- depends_on remark 31.33 Reading the two viscosities ¶
-
depends_on
theorem 31.36
The Newtonian constitutive relation
¶
- depends_on theorem A.718 Stokes' drag law with its coefficient ¶
- depends_on theorem 31.37 The Navier–Stokes equations ¶ ↺
-
depends_on
proposition 31.16
Hydrostatic balance
¶
- depends_on example 31.19 The barometric distribution ¶
- depends_on phenomenon 49.8 The white-dwarf luminosity function has an edge ¶
-
depends_on
phenomenon 31.18
Archimedes' principle
¶
- depends_on example 31.46 Terminal velocity, and Millikan's droplets ¶
-
depends_on
proposition 52.1
Hydrostatic equilibrium of a self-gravitating
sphere
¶
- depends_on phenomenon 52.12 The mass–luminosity relation ¶
- depends_on proposition 49.3 Lane–Emden form of hydrostatic equilibrium; restated from the stellar-structure chapter ¶
- depends_on theorem 52.2 Virial theorem for a self-gravitating sphere ¶
-
depends_on
definition 31.21
Ideal fluid
¶
-
depends_on
proposition 30.19
The stress tensor is symmetric
¶
-
depends_on
definition 30.20
Pressure and deviatoric stress
¶
-
depends_on
definition 30.31
The engineering moduli
¶
- depends_on phenomenon 30.70 Hertzian contact ¶
- depends_on phenomenon 30.60 Coulomb's law of torsion ¶
- depends_on proposition 30.33 Conversion among the moduli ¶ ↺
- depends_on proposition 30.51 Moment and curvature ¶
- 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 30.79
Maxwell viscoelasticity
¶
- depends_on proposition 30.80 A Maxwell material is a solid or a fluid depending on how long you watch ¶
-
depends_on
proposition 30.74
The maximum shear stress, and its indifference to
pressure
¶
- depends_on phenomenon 30.73 Yield and brittle fracture ¶
- depends_on remark A.705 The dangerous stress is below the surface ¶
- depends_on remark 30.75 Two criteria, one uncited ¶
- depends_on remark 30.75 Two criteria, one uncited ¶ ↺
-
depends_on
definition 30.31
The engineering moduli
¶
-
depends_on
definition 30.20
Pressure and deviatoric stress
¶
- depends_on proposition 30.74 The maximum shear stress, and its indifference to pressure ¶ ↺
-
depends_on
remark 30.72
Stress concentration
¶
-
depends_on
proposition 30.76
Griffith's criterion
¶
- depends_on example 30.77 Why glass is weak, and thin glass is not ¶
- depends_on phenomenon 30.73 Yield and brittle fracture ¶ ↺
-
depends_on
proposition 30.76
Griffith's criterion
¶
- depends_on theorem A.695 Boussinesq's point-force solution, quoted ¶ ↺
-
depends_on
theorem 30.21
Cauchy's equation of motion
¶
-
depends_on
definition 30.22
Boundary conditions of elastostatics
¶
- depends_on proposition 30.50 Love waves need a slow surface layer ¶
-
depends_on
proposition 30.48
Rayleigh's secular equation
¶
- depends_on proposition 30.49 The Rayleigh speed of a Poisson solid ¶
-
depends_on
proposition 30.23
Virtual work; the weak form
¶
- depends_on phenomenon 30.70 Hertzian contact ¶ ↺
- depends_on proposition 30.34 Minimum of the potential energy ¶
- depends_on remark 30.69 Saint-Venant's principle, and its exact status ¶
- depends_on proposition 30.23 Virtual work; the weak form ¶ ↺
- depends_on proposition 31.16 Hydrostatic balance ¶ ↺
- depends_on remark 30.69 Saint-Venant's principle, and its exact status ¶ ↺
-
depends_on
theorem 30.40
Navier–Cauchy equations
¶
-
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
proposition 30.41
Energy balance and its flux
¶
- depends_on theorem 30.42 Uniqueness in elastodynamics ¶
- depends_on proposition 30.50 Love waves need a slow surface layer ¶ ↺
- depends_on proposition 30.48 Rayleigh's secular equation ¶ ↺
- depends_on remark 30.46 Why the plane-wave route, and not the potentials ¶ ↺
-
depends_on
phenomenon 30.43
Two bulk wave speeds
¶
- depends_on theorem 31.22 Euler's equations of motion ¶ ↺
-
depends_on
definition 30.22
Boundary conditions of elastostatics
¶
-
depends_on
definition 30.24
The elasticity tensor
¶
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 |
→ | Orthogonal coordinate transformation | declared | parts/02-mathematical-methods/11-manifolds-tensors-curvature.tex:312 |
depends_on |
← | Inertia tensor | declared | parts/03-classical-mechanics/02-newtonian-dynamics.tex:1239 |
depends_on |
← | Inertia tensor, continuum form | declared | parts/03-classical-mechanics/12-rigid-body-rotating-frames.tex:373 |
depends_on |
← | Isotropic Cartesian tensors of rank four | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:813 |
depends_on |
← | Strain and displacement share a letter | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:58 |
depends_on |
← | Strain is a Cartesian tensor of rank two | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:215 |
depends_on |
← | The cross product is an axial vector | declared | parts/02-mathematical-methods/11-manifolds-tensors-curvature.tex:4700 |
depends_on |
← | Levi-Civita identities in three dimensions | declared | parts/02-mathematical-methods/11-manifolds-tensors-curvature.tex:520 |
depends_on |
← | The moment of inertia is a quadratic form in the axis | declared | parts/03-classical-mechanics/02-newtonian-dynamics.tex:1252 |
depends_on |
← | What the classification is used for | declared | parts/02-mathematical-methods/11-manifolds-tensors-curvature.tex:625 |
depends_on |
← | Cauchy: the stress tensor exists | declared | parts/03-classical-mechanics/13-continuum-elasticity.tex:560 |