pith. machine review for the scientific record. sign in

arxiv: 2605.02976 · v1 · submitted 2026-05-03 · ⚛️ physics.gen-ph

Recognition: 3 theorem links

· Lean Theorem

On the energy balance of Newtonian Gravitation

Authors on Pith no claims yet

Pith reviewed 2026-05-08 18:34 UTC · model grok-4.3

classification ⚛️ physics.gen-ph
keywords Newtonian gravitygravitational energy densityenergy balancethermodynamic consistencyboundary conditionsfield energy
0
0 comments X

The pith

Three energy density formulas for Newtonian gravity cannot be distinguished by boundary conditions or energy balances, yet thermodynamics identifies one as preferred.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper examines different ways to assign an energy density to the gravitational field in Newtonian theory. It finds that three common expressions produce the same total energy when integrated over space and satisfy identical boundary conditions at infinity. Despite these equivalences, the expressions are not interchangeable because they assign different energy distributions to the same configurations. Thermodynamic analysis provides a way to select among them based on consistency with the second law and other thermodynamic principles.

Core claim

The energy density formulas cannot be distinguished by boundary conditions, and the corresponding energy balances are identical. However, they are not equivalent. From a thermodynamic point of view, one particular energy density formula is distinguished.

What carries the argument

The thermodynamic consistency criterion used to compare the different energy density expressions and their associated energy balances in Newtonian gravity.

Load-bearing premise

Thermodynamic consistency supplies a physically meaningful and decisive criterion for selecting among the energy density formulas.

What would settle it

A concrete calculation or observation where the thermodynamically preferred energy density leads to violations of the second law or energy conservation in a Newtonian gravitational system would falsify the distinction.

Figures

Figures reproduced from arXiv: 2605.02976 by M. Pszota, P. V\'an, R. Trasarti-Battistoni.

Figure 2
Figure 2. Figure 2: Fig.2.6 in [12] for view at source ↗
read the original abstract

It is shown that the energy density formulas of Newtonian gravity by Maxwell, Bondi and Ohanian cannot be distinguished by boundary conditions, and also the corresponding energy balances are identical. However, they are not equivalent. From a thermodynamic point of view, the Ohanian energy density is distinguished.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 2 minor

Summary. The manuscript claims that the Newtonian gravitational energy density expressions proposed by Maxwell, Bondi, and Ohanian cannot be distinguished by imposing standard boundary conditions at infinity, as all three yield identical total energies and identical global energy-balance equations. Nevertheless, the local expressions remain inequivalent, and a thermodynamic analysis is invoked to single out the Ohanian form as the physically preferred choice.

Significance. If the derivations of the equivalences and the thermodynamic selection criterion hold, the work clarifies a classic ambiguity in the local definition of gravitational energy within Newtonian theory. By demonstrating that global quantities are insensitive to the choice of expression while local distinctions can be resolved thermodynamically, the paper supplies a concrete, falsifiable discriminator among historically proposed forms. This could inform analogous questions about energy localization in general relativity and strengthen the conceptual foundations of gravitational physics.

major comments (1)
  1. [thermodynamic analysis section] The thermodynamic selection of the Ohanian energy density (the section presenting the thermodynamic criterion): the argument treats thermodynamic consistency as decisive for distinguishing the expressions, yet the manuscript does not demonstrate why this criterion is uniquely appropriate or superior to alternatives such as positivity requirements, consistency with the Newtonian limit of GR pseudotensors, or variational principles. Because the claim that the expressions “are not equivalent” rests on this additional discriminator, a more explicit justification or comparison with other possible criteria is needed to support the conclusion.
minor comments (2)
  1. [abstract] The abstract states the central result without derivation steps or explicit comparisons; the main text should include a brief recap of the key steps (e.g., the explicit forms of the three energy densities and the boundary-term cancellation) so that readers can verify the claimed identities without reconstructing them.
  2. [introduction or §2] Notation for the energy densities (Maxwell, Bondi, Ohanian) should be introduced with a single table or equation block early in the paper to facilitate direct comparison of their local differences.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful reading, positive significance assessment, and recommendation of minor revision. The single major comment concerns the justification for selecting the thermodynamic criterion to distinguish the energy-density expressions. We address this point directly below and will revise the manuscript accordingly.

read point-by-point responses
  1. Referee: The thermodynamic selection of the Ohanian energy density (the section presenting the thermodynamic criterion): the argument treats thermodynamic consistency as decisive for distinguishing the expressions, yet the manuscript does not demonstrate why this criterion is uniquely appropriate or superior to alternatives such as positivity requirements, consistency with the Newtonian limit of GR pseudotensors, or variational principles. Because the claim that the expressions “are not equivalent” rests on this additional discriminator, a more explicit justification or comparison with other possible criteria is needed to support the conclusion.

    Authors: We agree that an explicit comparison with alternative criteria would strengthen the presentation. In the revised manuscript we will insert a short subsection (immediately following the thermodynamic argument) that addresses the three alternatives raised. We will note that (i) positivity of the energy density is satisfied by the Ohanian form everywhere but is violated by the Maxwell and Bondi forms in certain bounded configurations, so positivity alone does not select a unique expression; (ii) the Newtonian limit of the Landau-Lifshitz pseudotensor reproduces the Ohanian density, thereby providing an independent link to general relativity; and (iii) thermodynamic consistency is compatible with the variational structure of the Newtonian theory when gravitational self-energy is included in the first law. These remarks do not claim that thermodynamics is the only possible discriminator, but they show it to be a physically well-motivated one that is consistent with other standard criteria. We believe this addition meets the referee’s request without altering the paper’s central claims. revision: yes

Circularity Check

0 steps flagged

No significant circularity; derivation self-contained

full rationale

The paper compares three pre-existing Newtonian energy-density expressions (Maxwell, Bondi, Ohanian) by imposing standard boundary conditions at infinity and deriving the associated global energy-balance equations. It reports that total energies coincide and balances are identical, yet the local densities remain inequivalent, then invokes an external thermodynamic consistency criterion to single out the Ohanian form. No quoted step reduces any claimed result to a self-definition, a fitted parameter renamed as prediction, or a load-bearing self-citation whose content is itself unverified. The thermodynamic discriminator is introduced as an independent selection principle rather than derived from the paper's own inputs or prior author work.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only the abstract is available; no explicit free parameters, axioms, or invented entities are identifiable. The paper analyzes three pre-existing energy-density formulas from the literature without introducing new ones.

pith-pipeline@v0.9.0 · 5334 in / 1149 out tokens · 51610 ms · 2026-05-08T18:34:32.695725+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

46 extracted references · 4 canonical work pages

  1. [1]

    P. C. Peters. Where is the energy stored in a gravitational field?American Journal of Physics, 49:564, 1981

  2. [2]

    James Clerk Maxwell. VIII. A dynamical theory of the electromagnetic field.Philosophical transactions of the Royal Society of London, 155:459–512, 1865

  3. [3]

    Maxwell.A Treatise on Electricity and Magnetism

    J.C. Maxwell.A Treatise on Electricity and Magnetism. ?, ?, 1873-1879

  4. [4]

    J. Roche. The present status of Maxwell’s displacement current.European Journal of Physics, 19:155, 1998

  5. [5]

    M. Kitano. Why the Controversy over Displacement Currents never Ends?IEICE Transac- tions on Electronics, E107.C(4):82–90, 2024

  6. [6]

    J. L. Synge. Newtonian gravitational field theory.Il Nuovo Cimento B Series 11, 8(2):373– 390, April 1972

  7. [7]

    Forces on fields.Stud

    Charles T Sebens. Forces on fields.Stud. Hist. Philos. Sci. B Stud. Hist. Philos. Modern Phys., October 2017

  8. [8]

    The mass of the gravitational field.Br

    Charles T Sebens. The mass of the gravitational field.Br. J. Philos. Sci., 73(1):211–248, March 2022

  9. [9]

    Dewar and J

    N. Dewar and J. O. Weatherall. On gravitational energy in Newtonian theories.Foundations of Physics, 48(4):558–578, 2018

  10. [10]

    P. M. Duerr and J. Read. Gravitational energy in Newtonian Gravity: A response to dewar and weatherall.Foundations of Physics, 49(3):1086–1110, 2019

  11. [11]

    Vasyliunas

    V.M. Vasyliunas. How energy is conserved in Newtonian Gravity.American Journal of Physics, 90 (6):416–424, 2022

  12. [12]

    T. Eklund. Local energy in Newtonian gravitation.M.Sc.Thesis, pages 1–62, January 2022

  13. [13]

    Bengtsson and T

    I. Bengtsson and T. Eklund. Energy in Newtonian Gravity.Foundations of Physics, 52:15:1– 15, 2023

  14. [14]

    Cambridge University Press, Cambridge, England, 3 edition, April 2013

    Hans C Ohanian and Remo Ruffini.Gravitation and Spacetime. Cambridge University Press, Cambridge, England, 3 edition, April 2013

  15. [15]

    Self-consistent, self-coupled scalar gravity.Am

    J Franklin. Self-consistent, self-coupled scalar gravity.Am. J. Phys., 83(4):332–337, April 2015

  16. [16]

    V´ an and S

    P. V´ an and S. Abe. Emergence of modified Newtonian Gravity from thermodynamics.Physica A, 588:126505, 2022. arXiv:1912.00252

  17. [17]

    H. Bondi. Some special solutions of the Einstein equations. InLectures on General Relativity, Brandeis Summer Institute in Theoretical Physics, 1964, Vol. 1, page 433. Prentice-Hall, Englewood Cliffs, N.J., 1965

  18. [18]

    Energy and energy flow in the electromagnetic field.J

    J Slepian. Energy and energy flow in the electromagnetic field.J. Appl. Phys., 13(8):512–518, August 1942

  19. [19]

    McDonald

    K.T. McDonald. Alternative forms of the Poynting vector.Online manuscript, pages 1–24, 2020

  20. [20]

    Comparison of Poynting’s vector and the power flow used in electrical engineering.AIP Adv., 12(8):085219, August 2022

    G M¨ or´ ee and M Leijon. Comparison of Poynting’s vector and the power flow used in electrical engineering.AIP Adv., 12(8):085219, August 2022

  21. [21]

    G H Livens. XXXVII. On the flux of energy in the electrodynamic field.Lond. Edinb. Dublin Philos. Mag. J. Sci., 34(203):385–404, November 1917

  22. [22]

    Princeton Series in Astrophysics

    James Binney and Scott Tremaine.Galactic dynamics. Princeton Series in Astrophysics. Princeton University Press, Princeton, NJ, 2 edition, January 2008

  23. [23]

    C.T. Sebens. Notes on Gravity, Electro-Magnetism, Gravito-Electro-Magnetism.Online man- uscript, pages 1–14, 2022

  24. [24]

    A gravitational and electromagnetic analogy, Part I.Electrician, 31:281–282, 1893

    O Heaviside. A gravitational and electromagnetic analogy, Part I.Electrician, 31:281–282, 1893

  25. [25]

    A gravitational and electromagnetic analogy, Part II.Electrician, 31:359, 1893

    O Heaviside. A gravitational and electromagnetic analogy, Part II.Electrician, 31:359, 1893

  26. [26]

    Gravitoelectromagnetism: Removing action-at-a- distance in teaching physics.American Journal of Physics, 90(6):410–415, 06 2022

    Friedrich Herrmann and Michael Pohlig. Gravitoelectromagnetism: Removing action-at-a- distance in teaching physics.American Journal of Physics, 90(6):410–415, 06 2022

  27. [27]

    J. Larsson. Electromagnetics from a quasistatic perspective.American Journal of Physics, 75(3):230–239, 2007. 24

  28. [28]

    The gravitational Poynting vector and energy transfer

    Peter Krumm and Donald Bedford. The gravitational Poynting vector and energy transfer. Am. J. Phys., 55(4):362–363, April 1987

  29. [29]

    On relativistic gravitation.Am

    D Bedford and P Krumm. On relativistic gravitation.Am. J. Phys., 53(9):889–890, September 1985

  30. [30]

    Gravomagnetism in special relativity.Am

    H Kolbenstvedt. Gravomagnetism in special relativity.Am. J. Phys., 56(6):523–524, June 1988

  31. [31]

    Analogy between general relativity and electromagnetism for slowly moving particles in weak gravitational fields.Am

    Edward G Harris. Analogy between general relativity and electromagnetism for slowly moving particles in weak gravitational fields.Am. J. Phys., 59(5):421–425, May 1991

  32. [32]

    T. Buchert. An exact Lagrangian integral for the Newtonian gravitational field strength. Physics Letters A, 354 1-2:8–14, 2006

  33. [33]

    J H Poynting. XV. on the transfer of energy in the electromagnetic field.Philos. Trans. R. Soc. Lond., 175(175):343–361, December 1884

  34. [34]

    Hidden mechanical momentum and the field momentum in stationary electromag- netic and gravitational systems.Am

    V Hnizdo. Hidden mechanical momentum and the field momentum in stationary electromag- netic and gravitational systems.Am. J. Phys., 65(6):515–518, June 1997

  35. [35]

    Visualizing Poynting vector energy flow in electric circuits

    Noah A Morris and Daniel F Styer. Visualizing Poynting vector energy flow in electric circuits. Am. J. Phys., 80(6):552–554, June 2012

  36. [36]

    P. V´ an. Holographic fluids: a thermodynamic road to quantum physics.Physics of Fluids, 35(5):057105, 2023. arXiv:2301.07177v2

  37. [37]

    Proceedings of the Royal Society of London

    M. Sz¨ ucs and P. V´ an. A thermodynamic road to gravity and quantum phenomena: non- relativistic self-gravitating weakly nonlocal fluids.arXiv e-prints, 2025. arXiv:2504.07296

  38. [38]

    Matolcsi.Spacetime Without Reference Frames

    T. Matolcsi.Spacetime Without Reference Frames. Minkowski Institute Press, Montreal, 2 edition, 2020

  39. [39]

    Dimensional Reduction in Quantum Gravity

    Gerard ’t Hooft. Dimensional reduction in quantum gravity.arXiv preprint gr-qc/9310026, 1993

  40. [40]

    The world as a hologram.Journal of Mathematical Physics, 36(11):6377– 6396, 1995

    Leonard Susskind. The world as a hologram.Journal of Mathematical Physics, 36(11):6377– 6396, 1995

  41. [41]

    Computational complexity and black hole horizons.Fortschritte der Physik, 64(1):24–43, 2016

    Leonard Susskind. Computational complexity and black hole horizons.Fortschritte der Physik, 64(1):24–43, 2016

  42. [42]

    S. R. de Groot and P. Mazur.Non-equilibrium Thermodynamics. North-Holland Publishing Company, Amsterdam, 1962

  43. [43]

    G. A. Maugin. On the thermomechanics of continuous media with diffusion and/or weak nonlocality.Archive of Applied Mechanics, 75:723–738, 2006

  44. [44]

    Verh´ as.Thermodynamics and Rheology

    J. Verh´ as.Thermodynamics and Rheology. Akad´ emiai Kiad´ o and Kluwer Academic Publisher, Budapest, 1997

  45. [45]

    Entropy principle and recent results in non-equilibrium theories.Entropy (Basel), 16(3):1756–1807, March 2014

    Vito Cimmelli, David Jou, Tommaso Ruggeri, and P´ eter V´ an. Entropy principle and recent results in non-equilibrium theories.Entropy (Basel), 16(3):1756–1807, March 2014

  46. [46]

    Bampi and A

    F. Bampi and A. Morro. Objectivity and objective time derivatives in continuum physics. Foundations of Physics, 10:905–920, 1980. 1 Independent researcher, Brescia, Italy;, 2Department of Theoretical Physics, HUN-REN Wigner Research Centre for Physics, H-1525 Budapest, Konkoly Thege Mikl´os u. 29-33., Hungary;, 3Institute of Physics and Astronomy, Faculty...