EQUATION REGISTRY

Symmetric gain of inverse axial scales

This is an identity for two axial factors; a full inertial angular distribution requires an additional constitutive input.

Theory · DERIVEDEquation version 1.0.0

Based on the final manuscript · Chapter 2

ASD-WEB-DYN-005
K+=γ(1−β),K−=γ(1+β),K+K−=1,K+−1+K−−12=γK_+=\gamma(1-\beta),\quad K_-=\gamma(1+\beta),\quad K_+K_-=1,\quad\frac{K_+^{-1}+K_-^{-1}}2=\gamma

This is an identity for two axial factors; a full inertial angular distribution requires an additional constitutive input.
Chapter reference: Final collected manuscript · Chapter 2 §III.2 (2.10a) · ASD-BOOK-ddbade997b45

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Adopted source, conditions and previous versions

Final collected manuscript · Chapter 2 §III.2 (2.10a)

This is an identity for two axial factors; a full inertial angular distribution requires an additional constitutive input.

Conditions retained in this adoption

  • Uniform background, fixed internal state, 0≤v<c and no net radiation.
  • The LVE directional law and inertial angular weight are separate inputs.
  • m₀=C_m m_def; adopt C_m=1 and universal mass normalization.

Specific unresolved source issues

  • The microscopic core profile, inertial weight and four mass responses still require one common structural solution.

Source locators: p0610 · p0613 · p0615 · p0620 · p0624 · p0628 · p0630 · p0936 · 最终合订稿 · 第二章 §三.2 (2.10a)

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

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Previous source, retained as history

FND-3dde8d8e081d · 第二章 §三,(2.10a), PDF p. 7

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