Active and passive gravitational mass

Isolated-source far field and weak slowly varying external field; mP must be obtained from the configuration’s response.

Theory · CANDIDATE MODELEquation version 1.0.0

Based on the final manuscript · Chapters 4 and 5

ASD-WEB-MAT-011

\varphi(r)\sim\frac{Gm_G}{c^2r},\quad\Phi_g^{\rm ext}=-c^2\varphi^{\rm ext},\quad U_{\rm ext}=m_P\Phi_g^{\rm ext},\quad\mathbf F=-m_P\nabla\Phi_g^{\rm ext}

Isolated-source far field and weak slowly varying external field; mP must be obtained from the configuration’s response.
Chapter reference: Ch. 4 (4.36)–(4.38); Ch. 5 (5.6.28) and following text · ASD-BOOK-ddbade997b45

Assumptions and derivation Registry and dependencies Research this equation Discuss this equation

Source and ID

ASD-WEB-MAT-011 is the stable website equation ID. It retains existing links and does not replace the manuscript reference. Use the copy button to obtain LaTeX.

Return to premises and derivation

Adopted source, conditions and previous versions

Ch. 4 (4.36)–(4.38); Ch. 5 (5.6.28) and following text

Registered equation, symbols and scope checked against the final manuscript; original ID and scientific status preserved.

Conditions retained in this adoption

Isolated-source far field and weak slowly varying external field; mP must be obtained from the configuration’s response.

Specific unresolved source issues

MAT-SRC-001

Source locators: p1418–p1426 · p2289–p2293

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

MAT-d1034a344d58 · Ch. 4 (4.36)–(4.38); Ch. 5 (5.6.28) and following text

DEPENDS ON

Dependencies

No preceding equation is recorded in this index. Consult the source topic for definitions, geometry and model scope.

USED BY

Uses of this equation

Discuss this page Browse all equations