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Semidiscrete edge-face Maxwell energy conservation

Statement

Assume Countable Choice only as inherited from the real H(div⁡)/Piola finite-element space interfaces in Edge-face Maxwell finite element semidiscretization. For the lossless source-free semidiscretization Mee˙−CTMbb=0,b˙+Ce=0, the weighted energy Hh(t)=12∥e(t)∥Me2+12∥b(t)∥Mb2 is constant in time. The local matrix calculation uses no further choice principle.

Facts & Assumptions

Given: The finite-dimensional semidiscrete fields, symmetric positive definite matrices, and the source-free equations above.

[A1]

The Countable Choice Axiom is the principle that every countable family of nonempty sets has a choice function; it is included only because the imported FE-space and Piola definitions declare it. (The Axiom of Countable Choice (ACω))

[F1]

Me,Mb are symmetric positive definite and the semidiscrete equations are Mee˙=CTMbb and Mbb˙=−MbCe. (Edge-face Maxwell finite element semidiscretization)

Proof

1.1A1F1algebra

On a singleton time interval the energy is constant immediately; assume henceforth that the time interval is nondegenerate. In the declared Countable Choice branch [A1], the FE bases and matrices in [F1] are fixed finite objects; the calculation below makes no selection. Differentiating the electric part gives ddt12eTMee=eTMee˙=eTCTMbb.

2.1F1step 1.1algebra∎

Differentiating the magnetic part gives ddt12bTMbb=bTMbb˙=−bTMbCe=−eTCTMbb, because the scalar transpose equals itself. The two derivatives cancel, so Hh′(t)=0 throughout the interval of existence.

Depends on

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Sources