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Compatible discrete charge and magnetic divergence propagate

Statement

For the Yee update in Lossless or midpoint-conductive Yee leapfrog update, suppose the initial rows satisfy −GTMee0=ρ0 and Db−1/2=0. If the source and charge rows satisfy ρn+1−ρn−Δt GT(jn+1/2+Sen+1+en2)=0 at every step, then −GTMeen=ρn and Dbn−1/2=0 for every later step. This is exact constraint propagation; it does not assert stability for a time step violating the CFL condition.

Facts & Assumptions

Given: A finite incidence complex, the Yee rows, initial charge and magnetic constraints, and the discrete continuity equation above.

[F1]

The Yee magnetic row is bn+1/2=bn−1/2−Δt Cen and its electric row is Me(en+1−en)/Δt+S(en+1+en)/2=CTMbbn+1/2−jn+1/2. (Lossless or midpoint-conductive Yee leapfrog update)

[F2]

The incidence maps satisfy CG=0 and DC=0 for the selected periodic or PEC-relative complex. (Incidence curl has zero discrete divergence and gradient curl)

[F3]

Discrete charge continuity is the displayed update for ρ and total current j+S(en+1+en)/2. (Oriented Maxwell cochains, masses, and the Yee grid)

Proof

1.1givenF1F2induction

Apply D to the magnetic row in [F1]. Then Dbn+1/2=Dbn−1/2−Δt DCen=Dbn−1/2 by [F2]. Starting from Db−1/2=0, induction gives Dbn−1/2=0 at every half step.

2.1givenF1F2F3algebra∎

Apply −GT to the electric row in [F1]. Since GTCT=(CG)T=0, this gives −GTMeen+1+GTMeen=ΔtGT(jn+1/2+S(en+1+en)/2). By [F3], the right side equals ρn+1−ρn. Thus the physical-charge residual −GTMeen−ρn is constant in n and is initially zero, so it remains zero.

Depends on

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Sources