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Notes
- 1.
The matrix \(({\mathcal D}_{\;\,\beta }^{\alpha })\) in the representation \( {\varvec{D}}_{\mathcal S} ={\mathcal D}_{\;\,\beta }^{\alpha }{\varvec{\tau }}_{\alpha }\otimes {\varvec{\tau }}^{\beta }\) is needed to obtain the eigenvalues and eigenvectors of \( {\varvec{D}}_{\mathcal S}\), and it has been derived in Sect. 3.2, formula (3.53).
- 2.
\( \displaystyle \delta _{\beta \gamma }=\varvec{f}_{\beta }\cdot \varvec{f}_{\gamma }= (C^{\alpha }_{\;\;\beta }{\varvec{\tau }}_{\alpha }) \cdot (C^{\lambda }_{\;\;\gamma }{\varvec{\tau }}_{\lambda })= C^{\alpha }_{\;\;\beta }C^{\lambda }_{\;\;\gamma } M^{-1}_{0\alpha \lambda } \displaystyle \Longleftrightarrow \; \mathbf {I}=\mathbf {C}^T\mathbf {M}_0^{-1}\mathbf {C}\)
\(\Longleftrightarrow \; \mathbf {C}^{-T}\mathbf {C}^{-1}=\mathbf {M}_0^{-1} \;\Longleftrightarrow \;\mathbf {C}\mathbf {C}^{T}=\mathbf {M}_0{.} \)
- 3.
A symmetric second order tensor \(\varvec{\sigma }\) on a three-dimensional Euclidean real vector space \(\mathcal V\) has the spectral decomposition
$$\varvec{\sigma }=\lambda _1\varvec{f}_1\otimes \varvec{f}_1+\lambda _2\varvec{f}_2\otimes \varvec{f}_2 +\lambda _3\varvec{f}_3\otimes \varvec{f}_3\,,$$where \(\lambda _1,\lambda _2,\lambda _3\) are the (real) eigenvalues of \(\varvec{\sigma }\), and \(\{\varvec{f}_1,\varvec{f}_2,\varvec{f}_3\}\) is an orthonormal basis of eigenvectors for \(\mathcal V\).
- 4.
To avoid this step one could have worked on the form (A.3) of the depth-averaged linear momentum balance equation, written for the case \({\mathcal H }=O(\epsilon ^{\gamma ^{\prime }})\).
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Luca, I., Tai, YC., Kuo, CY. (2016). Closure Relations for the Depth-Averaged Modelling Equations. In: Shallow Geophysical Mass Flows down Arbitrary Topography. Advances in Geophysical and Environmental Mechanics and Mathematics. Springer, Cham. https://doi.org/10.1007/978-3-319-02627-5_5
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