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Newton’s Example of the Two Globes

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Theory, Evidence, Data: Themes from George E. Smith

Part of the book series: Boston Studies in the Philosophy and History of Science ((BSPS,volume 343))

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Abstract

At the end of the Scholium Newton includes a long paragraph about two globes revolving around their center of gravity and held together by a tensed cord. It has been interpreted as a thought experiment (Sect. 6.2) meant to show how the properties of true circular motion defined as absolute motion can be determined in a three-dimensional empty universe. I start by showing that this reading of Newton’s example as a bona fide thought experiment is riddled with interpretation problems and that it is less straightforward than so far assumed (Sect. 6.3).

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Notes

  1. 1.

    Some of the novel quantities, such as the quantity of matter and the various quantities of centripetal force, are described in the set of definitions at the beginning of the Principia. The space-time Scholium, as it is now called, is a commentary pertaining to the set of definitions. The definitions are of: quantity of matter, quantity of motion, inherent force of matter (vis insita), impressed force, centripetal force and three measures of it (absolute quantity of centripetal force, accelerative quantity and motive quantity). (See Newton 1999, 403–408)

  2. 2.

    “Absolute, true, and mathematical time, in and of itself and of its own nature, without reference to anything external, flows uniformly and by another name is called duration.” (Newton 1999, 408)

  3. 3.

    “Absolute space, of its own nature and without reference to anything external, always remains homogenous and immovable. Relative space is any movable measure or dimension of this absolute space; such a measure or dimension is determined by our senses from the situation of the space with respect to bodies and is popularly used for immovable space.” (Newton 1999, 408–9)

  4. 4.

    “Place is the part of space that a body occupies, and it is, depending on the space, either absolute or relative.”(Newton 1999, 409)

  5. 5.

    “Absolute motion is the change of position from one absolute place to another; relative motion is change of position from one relative place to another.” (Newton 1999, 409)

  6. 6.

    See Maudlin (2012), Nagel (1961), Van Fraassen (1970).

  7. 7.

    See, for instance Maudlin (2012, 15): “Newton produces powerful empirical evidence for the existence of absolute motion (and hence absolute space and time) using considerations of the causes of motion.”

  8. 8.

    Arthur (2018), Barbour (1989, 629–40), Berkeley (1721), DiSalle (2006, 33–4), Earman (1989, Ch 4), Laymon (1978), Mach (1919, 229) Maudlin (2012, 22–5), Westfall (1971, 443–5)

  9. 9.

    Rynasiewicz (2019) understands the distinction between the true and absolute motion of a body on the one hand, and the apparent and relative motions, on the other hand, as one of a metaphysical kind. The former has an elevated ontological status, more reality or existence perhaps, than the latter. See also Huggett (2012) and DiSalle (2002, 2006) on the connection between true and absolute motion. The clearest presentation I found in Brading, Philosophy and the Physics Within, Ch 3 (ms). My own view departs from all of these, but this is not the place to develop it. I take it from the recent literature that, at least in the case of the globes, Newton builds the description such that there is a single quantity of true motion pertaining to each globe, and that the challenge is to capture the factors which change this quantity, and only those.

  10. 10.

    In Sect. 6.3 we shall see that this inference does not hold, given Newton’s own qualifications about relativity of motions. The most direct criticism of it I found in Barbour (1989, 643–4).

  11. 11.

    A side note: we immediately face the question of how to understand the gravity of those two globes in such an empty universe.

  12. 12.

    There is a great similarity between this strategy and current methodology of studying the properties of binary star systems. Most stars are in fact binary systems. (csiro.au)

  13. 13.

    For instance, Mach (1919) faults Newton with the assumptions entering into this thought experiment because it looks like the universe assumed is very different in crucial aspects from the universe we know to observe and inhabit. As he puts it, “the universe is not given twice.”

  14. 14.

    On the contrary, Newton says that the example aims to “actually” (actu) distinguish apparent and true motions. (See Sect. 6.4)

  15. 15.

    The model I have in mind is akin the two-body problem in physics, and not, say, mechanical models for causal interaction of two bodies. Newton, of course, does not use the word “model.” For recent work on this understanding of Newtonian models see Ducheyne (2005) and Ducheyne (2012, esp. chap. 2). Ducheyne focuses on planetary models. I share much with Ducheyne’s arguments, especially the idea that the models in Book 1 are not restricted to mathematics. But I also think that the two features which I introduce here are to be more systematically applied and embedded into Newton’s natural philosophy, going beyond models of planetary motions.

  16. 16.

    This claim will be developed elsewhere. This paper restricts itself to arguing that the presentation of the globes scenario is best understood as an illustration of the result of applying these two features. Specifically, it demotes the understanding of the scenario as a thought experiment. (That is not say that thought experiments in natural science do not use models.) Briefly put, this scenario is closer to reasoning in physics proper than we have seen it so far represented in the literature.

  17. 17.

    ?- shows insertions

  18. 18.

    The adverb deleted and replaced by “actu” cannot quite be made out, and hence this translation is a guess.

  19. 19.

    In the second edition of the Principia Newton inserted at this point the further clause, “and that the bodies were at rest.”

  20. 20.

    These passages are quoted from a longer manuscript by George Smith and Anne Whitman. Appendix 5 consists of variorum translations of selections from the version of Liber Primus Newton submitted to Cambridge Library under the auspices of Lucasian Lectures, Dd. 9.46 (pp. 36–215 of Whiteside 1989). See Whiteside (1989, 45–6), translated by George E. Smith; and the folio numbers (11 and 12) in Dd. 9.46. Smith (in press-b).

  21. 21.

    This question has often showed up during George’s course and it is a recurrent pattern in the history of testing Newtonian gravity. See Smith 2014.

  22. 22.

    The preceding paragraph stressed again the distinction between relative and “actual” quantities. The former are sensible measures of the latter. When we refer to quantities involving time, space, place, motion in the absolute sense, we use a “manner of expression which is out of the ordinary and purely mathematical.”

  23. 23.

    According to the reading on offer here, the bucket experiment follows the same method.

  24. 24.

    Focusing on changes in the motions of bodies as quantities also shows how specifying the bodies the motion to take place in a vacuum is a significant detail. It points out to the lack of resistance for the motions and, therefore, it provides a separate reason for considering the bodies a system unto itself. That is, the isolation of the system is well supported from a dynamical point of view as well.

  25. 25.

    These kinds of assumptions are crucial in idealizations of dynamically interacting systems. As George Smith’s works show, when we clearly spell out assumptions, we make it easier for ourselves to subject these idealizations to systematic revision Smith (2007, 2012, 2014).

  26. 26.

    See Newton’s discussion of the distinction between absolute space and relative space. Newton (1999, pp. 409–10)

  27. 27.

    “Thereupon if?no matter what? equal forces were to be impressed [imprimerentur] at the same time on alternate faces of the globes increasing or lessening the circular motion, the increase or decrease of the motion could be still be learned?would become known? from the added or diminished tension in the cord, and therefrom?finally? on which faces of the globes the forces would have to be [deberent] impressed for the motion to be increased maximally could be found, that is, the posterior faces, or those which follow [sequuntur] in the circular motion.” (See Sect. 6.4)

  28. 28.

    The general hypothetical form is basically an inference: if such-and-such effects are present, then such-and-such claims are true. See Sect. 6.5.

  29. 29.

    Smith (in press-a), ‘Liber secundus.’

  30. 30.

    The bolded emphasis is mine throughout.

  31. 31.

    This is yet another one of the great contributions for which I am grateful to George Smith. On the one hand, there is the dedication to the analysis of the text. On the other hand, there is the generosity in sharing these materials with generations of researchers.

  32. 32.

    Recall that the two globes were taken to revolve around their center of gravity (and not some arbitrary point), a well-defined mathematical point which assumes some understanding of gravity.

  33. 33.

    Newton proposes here a view of analyzing the motion of an isolated system of two bodies acting through a central potential. Our current physics sensibilities recognizes this as a two-body problem and it is one the paradigmatic examples taught in celestial physics. Yet until Newton there was nobody who formulated the motion of two bodies under gravity in this manner.

  34. 34.

    Law 3 is inevitably included in the model.

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Solomon, M. (2023). Newton’s Example of the Two Globes. In: Stan, M., Smeenk, C. (eds) Theory, Evidence, Data: Themes from George E. Smith. Boston Studies in the Philosophy and History of Science, vol 343. Springer, Cham. https://doi.org/10.1007/978-3-031-41041-3_6

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