Charge conservation conditional on identification

The first two follow from the candidate identification; the flux law also needs effective EM source equations.

Theory · CANDIDATE MODELEquation version 1.0.0

Based on the final manuscript · Chapter 4

\partial_t\rho_{\rm em}+\nabla\cdot\mathbf j_{\rm em}=0,\qquad Q_{\rm em}=eN_{\rm em},\qquad\epsilon_0\oint_{\partial V}\mathbf E\cdot d\mathbf S=Q_{\rm em}(V)

The first two follow from the candidate identification; the flux law also needs effective EM source equations.
Chapter reference: Ch. 4 (4.28)–(4.29) · ASD-BOOK-ddbade997b45

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Ch. 4 (4.28)–(4.29)

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The first two follow from the candidate identification; the flux law also needs effective EM source equations.

Source locators: p1391–p1395

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

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MAT-d1034a344d58 · Ch. 4 (4.28)–(4.29)

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