How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
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 and . If the source and charge rows satisfy at every step, then and 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.
The Yee magnetic row is and its electric row is . (Lossless or midpoint-conductive Yee leapfrog update)
The incidence maps satisfy and for the selected periodic or PEC-relative complex. (Incidence curl has zero discrete divergence and gradient curl)
Discrete charge continuity is the displayed update for and total current . (Oriented Maxwell cochains, masses, and the Yee grid)
Proof
Apply to the magnetic row in [F1]. Then by [F2]. Starting from , induction gives at every half step.
Apply to the electric row in [F1]. Since , this gives . By [F3], the right side equals . Thus the physical-charge residual is constant in and is initially zero, so it remains zero.
Depends on
Used by
Nothing in the library uses this result yet.
Dependency tree · two levels
7 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- John B. Schneider, Understanding the Finite-Difference Time-Domain Method (standard reference, not scraped)