Abstract

AbstractElectromagnetic phenomena are mathematically described by solutions of boundary value problems. For exploiting symmetries of these boundary value problems in a way that is offered by techniques of dimensional reduction, it needs to be justified that the derivative in symmetry direction is constant or even vanishing. A generalized notion of symmetry can be defined with different directions at every point in space, as long as it is possible to exhibit unidirectional symmetry in some coordinate representation. This can be achieved, for example, when the symmetry direction is given by the direct construction out of a unidirectional symmetry via a coordinate transformation which poses a demand on the boundary value problem. Coordinate independent formulations of boundary value problems do exist but turning that theory into practice demands a pedantic process of backtranslation to the computational notions. This becomes even more challenging when multiple chained transformations are necessary for propagating a symmetry. We try to fill this gap and present the more general, isolated problems of that translation. Within this contribution, the partial derivative and the corresponding chain rule for multivariate calculus are investigated with respect to their encodability in computational terms. We target the layer above univariate calculus, but below tensor calculus.

Highlights

  • There is a variety of different formulas for the transformation of vector components of fields and fluxes in classical electromagnetism

  • Electromagnetic phenomena are mathematically described by solutions of boundary value problems

  • For exploiting symmetries of these boundary value problems in a way that is offered by techniques of dimensional reduction, it needs to be justified that the derivative in symmetry direction is constant or even vanishing

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Summary

| INTRODUCTION

There is a variety of different formulas for the transformation of vector components of fields and fluxes in classical electromagnetism. We have used a programming language that is developed precisely for the purpose of establishing a translatability of propositions into equivalent type equations This choice seems to offer the best chance of being able to express all algebraic rules of a construction of finite element shape functions completely. The representations of the considered objects, the electric and magnetic fields, the geometry, for example, when given by parametrized coordinates, and coordinate transformations are expressed as multivariate functions, taking multiple arguments to multiple results[15]. In this way, the definition (23) does not bind any free variables of its argument-terms. Having equivalence proven for one obvious encoding it can be easier for a new encoding to show it isomorphic, transferring the proofs

| CONCLUSION
Methods
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