ANISOTROPIC SPACE DYNAMICS · OPEN RESEARCH

Strong-field closure

Derive strong-field X, radial scale and standard-process coupling from a longitudinal–transverse action, source boundary conditions and stable solutions; identify microscopically fixed coefficients.

Based on the final manuscript · Chapter 2

TheoryTheory · OPENReviewMathematical review · OPEN REVIEWEvidenceEvidence · UNTESTEDCanonicalNoStatus, review and sources
OP-GRV-001 · P2

NEEDS THEORY · Needs theory

AstrophysicsPDE
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01Task

An open research task extracted from the final Chapter 2 manuscript, not a new canonical derivation.

02Current state

Both radial-length integrals are analytic in the adopted exterior model, and photon-sphere and capture scales have been obtained. Boundary-cell counting gives area entropy, while the fixed-parameter sequence gives temperature and a first law. Unclosed tasks are termination-boundary formation, microstate capacity, correlation corrections and joint boundary–exterior evolution; these gaps do not erase the existing analytic results.

ASD-WEB-GRV-002
Ω=(1−2G0Mc2r)−1/2,Φ=Ω−1\Omega=\left(1-\frac{2G_0M}{c^2r}\right)^{-1/2},\quad\Phi=\Omega^{-1}

Constitutive input
r is areal radius with r > 2G₀M/c². The full strong-field function is a constitutive input, not uniquely fixed by weak redshift.
Chapter reference: Final collected manuscript · Chapter 2 §I.2 (2.3)—(2.4) · ASD-BOOK-ddbade997b45

ASD-WEB-GRV-003
X=Φ2=1−2G0Mc2r,Ψ=c22(X−1)=−G0MrX=\Phi^2=1-\frac{2G_0M}{c^2r},\quad\Psi=\frac{c^2}{2}(X-1)=-\frac{G_0M}{r}

Definition
Conditional on the stated inputs and domain. Manuscript numbering is separate from the website ID.
Chapter reference: Final collected manuscript · Chapter 2 §II.2 (2.6) · ASD-BOOK-ddbade997b45

ASD-WEB-GRV-005
∇2Ψ=4πG0ρg,∇2X=8πG0c2ρg,M=c28πG0∮∇X⋅dS\nabla^2\Psi=4\pi G_0\rho_g,\quad\nabla^2X=\frac{8\pi G_0}{c^2}\rho_g,\quad M=\frac{c^2}{8\pi G_0}\oint\nabla X\cdot d\mathbf S

Constitutive input
Weak static source equations in reference coordinates, not a closed dynamical strong-field master equation.
Chapter reference: Final collected manuscript · Chapter 2 §II.2 (2.7a)—(2.7b) · ASD-BOOK-ddbade997b45

ASD-WEB-GRV-038
ℓs(rh,r)=r(r−rh)+rhln⁡r+r−rhrh,ℓopt(r1,r2)=(r2−r1)+rhln⁡r2−rhr1−rh.\begin{aligned}\ell_s(r_h,r)&=\sqrt{r(r-r_h)}+r_h\ln\frac{\sqrt r+\sqrt{r-r_h}}{\sqrt{r_h}},\\\ell_{\mathrm{opt}}(r_1,r_2)&=(r_2-r_1)+r_h\ln\frac{r_2-r_h}{r_1-r_h}.\end{aligned}

Mathematical result
Exact analytic integrals for the adopted X=1−r_h/r, with r>r_h and r₂≥r₁>r_h. Actual length remains finite while the reference optical path diverges logarithmically as its inner endpoint approaches the boundary.
Chapter reference: Final collected manuscript · Chapter 2 §V.1 (2.60)—(2.62) · ASD-BOOK-ddbade997b45

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}

Mathematical result
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

ASD-WEB-GRV-051
Tbdy=c632πkBσhG02M,dEbdy=Tbdy dSbdy,σh=c34G0ℏ ⟹ Tbdy=ℏc38πG0kBM,Cbdy=−Mc2Tbdy,dEbdy=Tbdy dS+ωbdy dJ+Vbdy dQ.\begin{aligned}T_{\rm bdy}&=\frac{c^6}{32\pi k_B\sigma_hG_0^2M},\qquad dE_{\rm bdy}=T_{\rm bdy}\,dS_{\rm bdy},\\\sigma_h=\frac{c^3}{4G_0\hbar}&\ \Longrightarrow\ T_{\rm bdy}=\frac{\hbar c^3}{8\pi G_0k_BM},\qquad C_{\rm bdy}=-\frac{Mc^2}{T_{\rm bdy}},\\dE_{\rm bdy}&=T_{\rm bdy}\,dS+\omega_{\rm bdy}\,dJ+\mathcal V_{\rm bdy}\,dQ.\end{aligned}

Mathematical result
Fixed G₀, c and σ_h with E=Mc²; the temperature coefficient adopts the Bekenstein–Hawking reference normalization. The last line assumes differentiable E(S,J,Q), not an already solved rotating strong-field microstate.
Chapter reference: Final collected manuscript · Chapter 2 §V.8 (2.88)—(2.94) · ASD-BOOK-ddbade997b45

03Required work

Derive strong-field X, radial scale and standard-process coupling from a longitudinal–transverse action, source boundary conditions and stable solutions; identify microscopically fixed coefficients.

04Deliverable and boundary

A reviewable action, field equations, exterior solution, weak-field matching and stability analysis, with adopted inputs distinguished from outputs.

Weak-field redshift does not uniquely select a full strong-field function; X=0 of an adopted function does not prove boundary formation.

05Sources and collaboration

Final collected manuscript · Chapter 2 §五.1—8 (2.59)—(2.94)及小结第四项

Gravity · Tests

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STATUS & REVIEW
Theory StatusTheory · OPEN
Mathematical ReviewMathematical review · OPEN REVIEW
Overall Evidence StatusEvidence · UNTESTEDOpen research task; no new confirmed observational result.
Canonical ASDNo · Website guideResearch task from Chapter 2
Mathematical Review Note

Results are conditional on the stated scale, path and coupling inputs; mathematical reproduction and microscopic closure are distinct.

Read the formal review items
Adopted source, conditions and previous versions

§V.1—8 (2.59)—(2.94) and summary item 4

Update open-problem progress with established results; retain problem IDs and unresolved tasks.

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

  • Strong-field, microscopic and full apparatus closure remain task-specific research.

Source locators: p0784 · p0786 · p0794 · p0796 · p0820 · p0822 · p0876 · p0878 · p0886 · p0891 · p0899 · p0937

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

Download source identity manifest

The manifest identifies the source; it is not the complete manuscript. Adopting this source does not upgrade evidence or grant a new licence.

Previous source, retained as history

FND-3dde8d8e081d · Chapter 2 / 第二章 · §I–II, §IV conclusion, §V.1; pp. 3–6, 17–18

PREF-125df9543371 · 序章.pdf
125df9543371f89656a2c29d552e1166e5edcc9ff5f6ec1ef1e438c7688d6ec5

CH1-46d43c8c39bf · 第一章(2).pdf
46d43c8c39bfd47f06ad699a6780e1142adc14bdd3520e2d5603d37a696cd9e9

CH2-f9598318d123 · 第二章-ASD理论-修订书稿 (2).pdf
f9598318d123c1f85a7d720af9cecbed8392e0b399910e3f9bfb675d49494709

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RESEARCH LEDGER

Revision history

SOURCE & SCOPE

Chapter 2 · §V.1—8 (2.59)—(2.94) and summary item 4

This research task is based on the cited final Chinese manuscript. It is not a new canonical result. Both languages use the same source snapshot; original equation numbers and website IDs remain distinct.

Knowledge scope
CITATION & SOURCE FILE

ASD: Strong-field closure. OP-GRV-001-EN. Version 1.0.0; 2026-10-24. https://asd-physics.org/en/open-problems/gravity/strong-field-closure. §V.1—8 (2.59)—(2.94) and summary item 4. Source ASD-BOOK-ddbade997b45.

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