definition 13.5 Tensor under orthogonal transformations

open in the book · parts/02-mathematical-methods/11-manifolds-tensors-curvature.tex:305 · p. 453

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definition 13.5: Tensor under orthogonal transformations13.5definition 13.4: Orthogonal coordinate transformation13.4definition 19.42: Inertia tensor19.42definition 29.13: Inertia tensor, continuum form29.13lemma 30.26: Isotropic Cartesian tensors of rank four30.26notation 30.1: Strain and displacement share a letter30.1proposition 30.7: Strain is a Cartesian tensor of rank two30.7proposition 13.96: The cross product is an axial vector13.96proposition 13.6: Levi-Civita identities in three dimensions13.6proposition 19.43: The moment of inertia is a quadratic form in the axis19.43remark 13.7: What the classification is used for13.7theorem 30.18: Cauchy: the stress tensor exists30.18definition 13.3: Orthogonal coordinate system13.3definition 19.41: Moment of inertia about an axis19.41example 19.45: The uniform solid sphere19.45definition 7.125: Multiple integral7.125definition 29.19: Inertia ellipsoid29.19example 29.23: The polar moment of the Earth, and what it reveals29.23proposition 49.17: Magnetic-dipole spin-down49.17proposition 29.14: Angular momentum and kinetic energy29.14proposition 29.15: Positivity29.15proposition 29.24: MacCullagh's formula29.24proposition 29.22: Perpendicular-axis theorem29.22theorem 29.20: Parallel-axis theorem29.20theorem 29.16: Principal axes29.16theorem 5.133: Isotropic Cartesian tensors of rank at most four5.133phenomenon 30.28: Hooke's law30.28proof : ch:13-continuum-elasticity@prooflink-1proofdefinition 30.6: Linear strain and infinitesimal rotation30.6proof : ch:13-continuum-elasticity@proof-1proofequation 13.13: eq:mfd-condorto13.13proof : ch:11-manifolds-tensors-curvature@proof-19proofequation 5.19: eq:lin-leibniz-det5.19proposition 13.95: The elementary cross-product identities13.95proof : ch:11-manifolds-tensors-curvature@proof-1proofproof : ch:02-newtonian-dynamics@proof-13proofdefinition 30.17: Traction30.17definition 30.24: The elasticity tensor30.24definition 31.1: Fluid31.1proposition 30.19: The stress tensor is symmetric30.19neighborhood truncated

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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