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ASDBoundary energy balance and area entropy
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Boundary energy balance and area entropy

Nonrotating uncharged quasistatic sequence at fixed G₀; counting model of approximately independent area cells and accessible states. The microscopic a_*, g_* and correlation corrections remain to be determined.

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Based on the final manuscript · Chapter 2

ASD-WEB-GRV-050
c2dMdt=Pin−Pout,Ah=16πG02M2c4,Nh=Aha∗,W=g∗Nh,Sbdy=kBln⁡W=kBσhAh,σh=ln⁡g∗a∗.\begin{aligned}c^2\frac{dM}{dt}&=P_{\rm in}-P_{\rm out},\qquad A_h=\frac{16\pi G_0^2M^2}{c^4},\\N_h&=\frac{A_h}{a_*},\quad W=g_*^{N_h},\\S_{\rm bdy}&=k_B\ln W=k_B\sigma_hA_h,\qquad\sigma_h=\frac{\ln g_*}{a_*}.\end{aligned}

Nonrotating uncharged quasistatic sequence at fixed G₀; counting model of approximately independent area cells and accessible states. The microscopic a_*, g_* and correlation corrections remain to be determined.
Chapter reference: Final collected manuscript · Chapter 2 §V.7 (2.84)—(2.87) · ASD-BOOK-ddbade997b45

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Final collected manuscript · Chapter 2 §V.7 (2.84)—(2.87)

Nonrotating uncharged quasistatic sequence at fixed G₀; counting model of approximately independent area cells and accessible states. The microscopic a_*, g_* and correlation corrections remain to be determined.

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: p0784 · p0786 · p0794 · p0796 · p0802 · p0807 · p0820 · p0822 · p0831 · p0840 · p0849 · p0856 · p0876 · p0878 · p0886 · p0891 · p0899 · p0937 · 最终合订稿 · 第二章 §五.7 (2.84)—(2.87)

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

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inputStatic exterior limiting radiusASD-WEB-GRV-037
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