Orbital action in a static background

In addition to the free action, adopt universal static energy conversion L dt = L₀(v*) Φ dt.

Theory · EFFECTIVE MODELEquation version 1.0.0

Based on the final manuscript · Chapter 2

\mathcal L=\Phi\mathcal L_0(v_*)=-m_0c^2\sqrt{X-\frac{\dot r^2}{c^2X}-\frac{r^2\dot\varphi^2}{c^2}}

In addition to the free action, adopt universal static energy conversion L dt = L₀(v*) Φ dt.
Chapter reference: Final collected manuscript · Chapter 2 §IV.2 (2.27) · ASD-BOOK-ddbade997b45

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Final collected manuscript · Chapter 2 §IV.2 (2.27)

In addition to the free action, adopt universal static energy conversion L dt = L₀(v*) Φ dt.

Conditions retained in this adoption

Fixed G₀; isolated, static, spherically symmetric, uncharged exterior.
Areal radius, actual spatial length and reference optical path are defined separately.
Weak-field perturbation, slow-rotation far field and boundary statistics each have separate conditions.

Specific unresolved source issues

Microscopic source matching, dynamical strong fields and full boundary-state dynamics remain open.

Source locators: p0682 · p0694 · p0698 · p0701 · p0703 · p0705 · p0715 · p0717 · p0719 · p0730 · p0732 · p0779 · 最终合订稿 · 第二章 §四.2 (2.27)

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

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FND-3dde8d8e081d · 第二章 / Chapter 2 · (2.27), p. 12

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