Coulomb law in true space

Using true length as the interaction distance is a constitutive input, not a deduction from metrology alone.

Theory · FOUNDATIONEquation version 1.0.0

Based on the final manuscript · Chapter 3

\mathbf F_T=\frac{q_1q_2}{4\pi\varepsilon_0r_T^2}\hat{\mathbf r},\qquad\mathbf F_0=\frac{q_1q_2}{4\pi\varepsilon_0r^2}\hat{\mathbf r}

Using true length as the interaction distance is a constitutive input, not a deduction from metrology alone.
Chapter reference: Final collected manuscript · Chapter 3, equations (3.3) · ASD-BOOK-ddbade997b45

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Final collected manuscript · Chapter 3, equations (3.3)

Using true length as the interaction distance is a constitutive input, not a deduction from metrology alone.

Conditions retained in this adoption

Special two-body result: uniform exterior background, equal parallel velocities, transverse separation and virtual displacement at fixed velocity.
Free Maxwell representation: long waves, weak perturbations, transverse constraint, constant coefficients and normalization.
Minimal-coupling sources: macroscopic coarse graining, low-speed point sources or a low-frequency near zone; high-speed closed sources require separate construction.

Specific unresolved source issues

Local results do not automatically close high-speed topological sources, full instrument mapping or global directed propagation.

Source locators: p0961 · p0964 · p0966 · p0968 · p0982 · p0984 · p0986 · p1281 · 最终合订稿 · 第三章式 (3.3)

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

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EM-f06476f55cae · 第三章 / Chapter 3 · (3.3), PDF p. 2

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