Magnetic Vector Potentials and Helicity in Periodic Domains

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Magnetic Vector Potentials and Helicity in Periodic Domains Simon Candelaresi

Transcript of Magnetic Vector Potentials and Helicity in Periodic Domains

Page 1: Magnetic Vector Potentials and Helicity in Periodic Domains

Magnetic Vector Potentialsand Helicity in Periodic Domains

Simon Candelaresi

Page 2: Magnetic Vector Potentials and Helicity in Periodic Domains

Perfectly Conducting Boundaries

gauge transformation:

boundary conditions:

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Periodic Boundaries

gauge transformation:

boundary conditions:

periodic

with periodic:

in general:

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Magnetic helicity is a gauge-dependent quantity, because can be redefined by adding a gradient to it (gauge transformation). However, for perfectly conducting boundaries or periodic systems without a net magnetic flux, the magnetic helicity is gauge invariant.

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Wikipedia

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Periodic Domains with Mean Flux

(Berger 1996)

Mean magnetic field in z-direction

inversion of magnetic helicity

But: Problem starts with magnetic vector potential.

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Differential p-forms

P-form: covariant p-tensor that is antisymmetric:

P-tensor: multilinear map:

Differential 1-form:

Construct every differential p-form from 1-forms with the wedge product:

anti-symmetrized tensor product

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Differentiation of forms

Linearity:

Double differentiation:

Associated vectors in (Euclidean metric):

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PotentialsA p-1 form is a potential for a given p-form if .

need: (exact form)

Poincaré Lemma: On any contractible manifold, if then there exists an such that .

Contractible manifold: Non-contractible manifold:

Integral along closed loops:

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Fundamental Periods, Betti Numbers

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Fundamental periods: Closed hypersurfaces (e.g. loops) which cannot be continuously transformed into each other.

Betti number: number of such loops.

For a potential to exist the Betti number must vanish or integrals along the fundamental periods must vanish.

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Periodic Domains

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exists

1 periodic side:

exists

2 periodic sides:

Mean magnetic field along periodic directions:

Mean magnetic field along non-periodic direction: does not exist

(Berger 1996)

exists

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Periodic Domains

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3 periodic sides:

Mean magnetic field through all sides must vanish.

3 fundamental periods

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Non-Periodic Domains

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known: find:Problem:

Solution:

Coulomb gauge:

!assumed periodicity!

Remedy: Volterra's formula

Need star-shaped domain.

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Conclusions

● Magnetic helicity gauge dependent in periodic domains.

● Vector potential does not always exist in periodic domains.

● Volterra's formula for non-periodic domains.

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