Source normalization and mass matching
Define all four masses from the same complete core–field system. Equality and the Zφ condition require source–energy matching, not ontology alone. Setting coefficients by observed G is effective normalization.
Based on the final manuscript · Chapters 4 and 5
Define all four masses from the same complete core–field system. Equality and the Zφ condition require source–energy matching, not ontology alone. Setting coefficients by observed G is effective normalization.
Chapter reference: Ch. 5 (5.6.26)–(5.6.29) · ASD-BOOK-ddbade997b45
Source and ID
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Return to premises and derivationAdopted source, conditions and previous versions
Ch. 5 (5.6.26)–(5.6.29)
Registered formula checked individually against the final manuscript; semantic potential phi→varphi; four independent mass definitions and explicit matching identity; source-grounded scope note synchronized
Conditions retained in this adoption
- Define all four masses from the same complete core–field system. Equality and the Zφ condition require source–energy matching, not ontology alone. Setting coefficients by observed G is effective normalization.
Source locators: p2283–2294
Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e
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Previous source, retained as history
SD-51779505a476 · Ch. 5 (5.6.26)–(5.6.29)
Dependencies
algebraStatic stretch far fieldASD-WEB-SD-030