Abstract
To measure data and solutions spatially, we recall a number of useful definitions and results on Lebesgue and standard Sobolev spaces. Then, we introduce more specialized Sobolev spaces, which are better suited to measuring solutions to electromagnetics problems, in particular, the divergence and the curl of fields. This also allows one to measure their trace at interfaces between two media, or on the boundary. Last, we construct ad hoc function spaces, adapted to the study of time- and space-dependent electromagnetic fields.
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Notes
- 1.
Given any subset S of \(\mathbb {R}^n\), 1 S denotes the indicator function of S .
- 2.
The space \({\mathcal {D}}(\varOmega )\) can also be denoted by \(C^\infty _c(\varOmega )\), where the index c stands for compact support.
- 3.
Classically, for \(k\in \mathbb {N}\), β ∈ ]0, 1], \({\mathcal O}\subset \mathbb {R}^n\), \(C^{k,\beta }({\mathcal O})\) is the Hölder space defined by
$$\displaystyle \begin{aligned} C^{k,\beta}({\mathcal O}):=\{f\in C^{k}({\mathcal O})\ :\ \sum_{\alpha\in\mathbb{N}^n,\ |\alpha|=k}\sup_{{\boldsymbol{x}}\ne\boldsymbol{y}}\frac{|\partial_\alpha f({\boldsymbol{x}})-\partial_\alpha f(\boldsymbol{y})|}{|{\boldsymbol{x}}-\boldsymbol{y}|{}^\beta}<\infty\},\end{aligned}$$where \(C^k({\mathcal O}):=\{f\in C^0({\mathcal O})\ :\ \partial _\alpha f\in C^0({\mathcal O}),\ \forall \alpha \in \mathbb {N}^n,\ |\alpha |\le k\}\).
Lipschitz-continuity coincides with C 0, 1 continuity.
- 4.
Given any subset S of \(\mathbb {R}^n\), int(S) denotes the interior of S.
- 5.
Evidently, a direct construction is also possible!
- 6.
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Assous, F., Ciarlet, P., Labrunie, S. (2018). Basic Applied Functional Analysis. In: Mathematical Foundations of Computational Electromagnetism. Applied Mathematical Sciences, vol 198. Springer, Cham. https://doi.org/10.1007/978-3-319-70842-3_2
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