2001
DOI: 10.2528/pier00080108
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Topological Approach to Computational Electromagnetism

Abstract: Software systems designed to solve Maxwell's equations need abstractions that accurately explain what different kinds of electromagnetic problems really do have in common. Computational electromagnetics calls for higher level abstractions than what is typically needed in ordinary engineering problems. In this paper Maxwell's equations are described by exploiting basic concepts of set theory. Although our approach unavoidably increases the level of abstraction, it also simplifies the overall view making it easi… Show more

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Cited by 21 publications
(21 citation statements)
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References 10 publications
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“…The chain space C p ðK; EÞ can be decomposed similarly where › is the key operator (Tarhasaari and Kettunen, 2001) which related cuts on a dual complex to finding appropriate generators for primal cohomology groups (Kettunen et al, 1998). Let us next check whether there exists isomorphisms between subspaces of primal cochains and dual chains.…”
Section: A Decompositions On (Co)chain Spacesmentioning
confidence: 99%
“…The chain space C p ðK; EÞ can be decomposed similarly where › is the key operator (Tarhasaari and Kettunen, 2001) which related cuts on a dual complex to finding appropriate generators for primal cohomology groups (Kettunen et al, 1998). Let us next check whether there exists isomorphisms between subspaces of primal cochains and dual chains.…”
Section: A Decompositions On (Co)chain Spacesmentioning
confidence: 99%
“…1). They are related to the homology group (10) This is a conceptually tricky, but practically straightforward, notion. The elements of a homology group are equivalence classes of chains, but in practical computations we just take one chain-a representative-from such a class and operate to it.…”
Section: Classification Of Chainsmentioning
confidence: 99%
“…Assume we have the basis matrices and , according to Problem 3. We decompose basis as follows: This algorithm [10] cumulates a basis of to matrix . The vectors of are linearly independent of the vectors in 3 The null space of matrix A 2 from the QR-decomposition of A costs 2m (n 0 m=3) flops with Householder QR or 3m (n 0 m=3) flops with Givens QR [9].…”
Section: B Chain By Chain Computationmentioning
confidence: 99%
“…where a p and b p+1 are called cochains [25,28]. Cochains therefore constitute the discrete representation of the electromagnetic fields.…”
Section: The General Finite Formulationmentioning
confidence: 99%