remark 13.7 What the classification is used for

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remark 13.7: What the classification is used for13.7definition 13.5: Tensor under orthogonal transformations13.5theorem 5.133: Isotropic Cartesian tensors of rank at most four5.133definition 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 axis19.43theorem 30.18: Cauchy: the stress tensor exists30.18lemma 5.33: Determinant through the Levi–Civita symbol5.33lemma 5.132: Parity constraint5.132proposition 5.130: An orthogonal transformation is an isometry5.130lemma A.742: Isotropic representationA.742lemma A.671: The three products are independentA.671remark A.677: The lower ranks, and why an isotropic solid is not piezoelectricA.677remark 30.27: Two results this chapter borrows from Part II30.27proof : ch:03-linear-algebra-representations@proof-58proof

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