Gravity · Experimental Relations and Tests
Distinguish reproduced results, physical reinterpretations and proposed discriminating tests.
Results are conditional on the stated scale, path and coupling inputs; mathematical reproduction and microscopic closure are distinct.
Read the formal review items01Reading the Matrix
Compare the same observable, parameter calibration, endpoints and approximation order. REPRODUCED, REINTERPRETED and POTENTIALLY DISCRIMINATING are relationship categories; evidence status is separate. Identical formulas are not independent experimental verification.
02Gravity Tests Matrix
| Observable | ASD | GR | Same numerically? | Distinguishing? |
|---|---|---|---|---|
| Static redshift | , weak field | Same static ratio | Yes, matching calibration | NO |
| Weak deflection | Same at this order | Yes | NO at weak field | |
| Shapiro | times endpoint logarithm | Same at this order | Yes, fixed endpoints | NO at this order |
| Periapsis advance | Same at this order | Yes, first-order central field | NO; higher order need not differ | |
| Static photon sphere / shadow | / | Same static scales | Yes, adopted exterior | NO for these scales |
| Boundary, rotation, nondegenerate terms | Dynamical closure pending | Matching observing model needed | TBD | Potential; no difference yet |
03REPRODUCED
Weak-field light deflection
Chapter 2 §IV.5, (2.43)–(2.50); JPL / IAU; Will (2014)Ready to recalculate the stated limited model; not a completed distinct prediction.
ASD-PRED-006- Observed result
- Deflection is an established observable; the chapter calculates about 1.75 arcseconds for solar grazing.
- ASD calculation / interpretation
- Integration of the full optical gradient gives 4G₀M/(c²b).
- Established-theory result
- The same result for matching distant endpoints and weak-field order.
- Numerically different?
- NO — same order.
- Interpretation different?
- YES — spatial stretching and phase-path selection.
- Does this distinguish ASD?
- NO — weak field.
- Current status
- Analytic and chapter-number reproduction; no new optical/radio data fit.
- Required precision
- No nonzero model difference is defined, hence no precision threshold.
Shapiro / Cassini link
Chapter 2 §IV.6, (2.51)–(2.58); NASA/JPL Cassini (2003)Ready to recalculate the stated limited model; not a completed distinct prediction.
ASD-PRED-006- Observed result
- Near-Sun Cassini radio links recorded frequency and round-trip light-time changes.
- ASD calculation / interpretation
- The one-way logarithm has coefficient 2G₀M/c³; a static round trip is approximately twice this.
- Established-theory result
- The same first-order delay after matching endpoints and order.
- Numerically different?
- NO — same in this static approximation.
- Interpretation different?
- YES — spatial accumulation of full reference optical length.
- Does this distinguish ASD?
- NO — at this order.
- Current status
- Analytic term reproduced; the illustration does not replace Cassini orbit, plasma and clock modeling.
- Required precision
- A real link needs an error budget; no unique-difference precision is defined.
Mercury central-field periapsis advance
Chapter 2 §IV.1–3, (2.25)–(2.42); JPL; Will (2014)Ready to recalculate the stated limited model; not a completed distinct prediction.
- Observed result
- Mercury orbital tests include a relativistic central-field advance; full observations include other perturbations.
- ASD calculation / interpretation
- Eq. (2.42) gives about 0.1035 arcseconds/orbit or 43.0 arcseconds/Julian century with chapter parameters.
- Established-theory result
- The same value for matching central field, parameters and first order.
- Numerically different?
- NO — same model and order.
- Interpretation different?
- YES — spatial-length and inertia-action construction.
- Does this distinguish ASD?
- NO — the current static spherical action is mathematically equivalent.
- Current status
- Central-field calculation reproduced; no independent ephemeris fit.
- Required precision
- First establish a difference not absorbed into mass, distance or orbital parameters.
Static photon sphere and critical shadow scale
Chapter 2 §V.1–3, (2.59)–(2.71)Source, coupling, readout or statistical mapping remains open; instrument precision cannot replace it.
- Observed result
- No fitted shadow image or emission-ring dataset is published in this module.
- ASD calculation / interpretation
- The adopted exterior gives r_ph = 3ℓ_g and b_c = 3√3ℓ_g; capture additionally requires absorption.
- Established-theory result
- Schwarzschild static optics gives identical critical scales.
- Numerically different?
- NO — for the adopted static exterior optical path.
- Interpretation different?
- YES — continuum termination is a separately stated ontological hypothesis.
- Does this distinguish ASD?
- NO — for these scales themselves; other boundary responses remain undetermined.
- Current status
- Conditional mathematics; emission, transfer and instrument modeling remain unfinished.
- Required precision
- No image difference or error budget is established.
Reproduction here includes matching chapter expressions to established results. Each card states whether data were refitted. The static strong-field optics card remains UNTESTED as evidence.
04REINTERPRETED
Static atomic-clock height shift
Chapter 2 §I, (2.2a); Bothwell et al. (2022)Ready to recalculate the stated limited model; not a completed distinct prediction.
ASD-PRED-005- Observed result
- Bothwell et al. report a gravitational frequency gradient across a millimetre-scale strontium sample.
- ASD calculation / interpretation
- Ω and the standard-process response give Δf/f = ΔΨ/c².
- Established-theory result
- The same static weak-field clock ratio.
- Numerically different?
- NO — same at this order.
- Interpretation different?
- YES — spatial/wavelength response versus proper-time construction.
- Does this distinguish ASD?
- NO — the shared ratio does not select an ontology.
- Current status
- Macroscopic consistency; no raw-data refit or microscopic atomic closure.
- Required precision
- No independent difference is specified, so no discriminating precision is assigned.
The Bothwell paper supplies the observation; Chapter 2 supplies the ASD interpretation. These sources have distinct roles.
05POTENTIALLY DISCRIMINATING
Nondegenerate higher-order, boundary or rotation observables
Chapter 2 §IV conclusion, §V.4–8; OP-GRV-001–004First acquire traceable observational inputs; a nondegenerate theoretical difference also requires review.
ASD-PRED-004- Observed result
- No independent difference or validating dataset has been published in this module.
- ASD calculation / interpretation
- Determine new responses from master equations or boundary/rotation dynamics, then calculate shared apparatus readouts.
- Established-theory result
- Compute a baseline using identical mass, distance, source structure, endpoints and order.
- Numerically different?
- TBD — neither second order nor strong field guarantees a difference.
- Interpretation different?
- Possible; identify the additional constitution and process response.
- Does this distinguish ASD?
- POTENTIALLY / PROPOSED TEST — existence of a discriminator is not established.
- Current status
- Open research; higher-order expansion of the present static action and optics can remain identical.
- Required precision
- TBD — after a difference model and parameter-degeneracy analysis.
Second order, strong field and rotation are not substitutes for a nonzero difference calculation. Current static spherical actions and optical paths are equivalent; parameter and coordinate degeneracies must be excluded first. See the open research tasks.
06Data and Sources
No new raw-data fit, residuals, confidence interval or underived prediction is published here. S301 stays an independent case study (Chinese), awaiting complete data before reproducible fitting.
Parameters use JPL and IAU B3. Link observations are described by the Cassini project; established-test context is in Will (2014). These are external references, not independent ASD validation reports.
Anisotropic Space Dynamics
Chapter 2 · Static Spatial Anisotropy
Chapter 2 / 第二章 §§I, IV–V, pp. 1–5, 11–25
- Module version
- 1.0.0
- Source snapshot
- FND-3dde8d8e081d
- Content review date
- 2026-09-14
Source files and checksums
The snapshot hash identifies the source manifest; each source file has its own checksum below.
- PREF-125df9543371 · 序章.pdf
8 PDF pages125df9543371f89656a2c29d552e1166e5edcc9ff5f6ec1ef1e438c7688d6ec5 - CH1-46d43c8c39bf · 第一章(2).pdf
23 PDF pages46d43c8c39bfd47f06ad699a6780e1142adc14bdd3520e2d5603d37a696cd9e9 - CH2-f9598318d123 · 第二章-ASD理论-修订书稿 (2).pdf
27 PDF pagesf9598318d123c1f85a7d720af9cecbed8392e0b399910e3f9bfb675d49494709
Prepared from the final Chinese manuscripts identified above. A public reading link for the full manuscript has not yet been released.
Position within the framework
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Revision history
Chapter 2 · Static Spatial Anisotropy · Chapter 2 / 第二章 §§I, IV–V, pp. 1–5, 11–25
This is the English translation of the Chinese canonical module, based on the same final-manuscript source snapshot. The Chinese final manuscript remains authoritative. Website equation IDs are stable citation identifiers; original manuscript numbers are listed separately.
Knowledge scopeASD: Gravity · Experimental Relations and Tests. ASD-GRV-GRAVITY-EN. Version 1.0.0; 2026-09-14. https://asd-physics.org/en/tests/gravity. Chapter 2 / 第二章 §§I, IV–V, pp. 1–5, 11–25. Source FND-3dde8d8e081d.
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