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Newton’s ‘Phenomena’

Kirsten Walsh writes…

On this blog, I have often argued that Newton’s Principia should be characterised as a work of experimental philosophy (for example, here, here and here).  To support this argument, I have tended to emphasise similarities between Newton’s work in optics and mechanics.  Recently, however, I have noted that some aspects of Newton’s methodology varied according to context.  For example, in the Opticks, Newton employed ‘experiments’, but in the Principia, he employed ‘phenomena’.  Given that experimental philosophy emphasises observation- and experiment-based knowledge, it is important for my project that I understand Newton’s use of phenomena, and its relationship to observation.  In this post, I’ll discuss the phenomena in Principia, and in my next, I’ll discuss the relationship between phenomena and experiments in more detail.

Firstly, let’s consider the origin of the phenomena of Principia.  In the first edition of Principia (1687), book 3 contained nine hypotheses.  But in the second edition (1713), Newton re-structured book 3 so that it contained only two hypotheses.  Five of the old hypotheses were re-labelled ‘phenomena’, and he added one more (phenomenon 2), to bring the total to six:

Phenomenon 1: The circumjovial planets, by radii drawn to the centre of Jupiter, describe areas proportional to the times, and their periodic times – the fixed stars being at rest – are as the 3/2 powers of their distances from that centre.

Phenomenon 2: The circumsaturnian planets, by radii drawn to the centre of Saturn, describe areas proportional to the times, and their periodic times – the fixed stars being at rest – are as the 3/2 powers of their distances from that centre.

Phenomenon 3: The orbits of the five primary planets – Mercury, Venus, Mars, Jupiter, and Saturn – encircle the sun.

Phenomenon 4: The periodic times of the five primary planets and of either the sun about the earth or the earth about the sun – the fixed stars being at rest – are as the 3/2 powers of their mean distances from the sun.

Phenomenon 5: The primary planets, by radii drawn to the earth, describe areas in no way proportional to the times but, by radii drawn to the sun, traverse areas proportional to the times.

Phenomenon 6: The moon, by a radius drawn to the centre of the earth, describes areas proportional to the times.

There are several things to notice about these phenomena.  Firstly, they are distinct from data, in that they describe general patterns of motion, rather than measurements of the positions of planetary bodies at particular times.  So, while the phenomena are detected and supported by astronomical observations, they are not observed or perceived directly.

Secondly, they are distinct from noumena (or the nature or essence of things), in that they are facts inferred from the observable, measurable properties of the world.  They describe the motions, sizes and locations of bodies, but not the substance or causes of these properties of bodies.

Thirdly, they describe relative motions of bodies.  That is, in each case, the orbit is described around a fixed point.  For example, phenomenon 1 describes the motions of the satellites of Jupiter around Jupiter, which is taken as a stationary body for the purposes of this proposition.  In phenomena 4 and 5, the motion of Jupiter is described around the sun, which is taken as stationary.

Fourthly, these phenomena do not prioritise the observer.  Rather, each motion is described from the ideal standpoint of the centre of the relevant system: the satellites of Jupiter and Saturn are described from the standpoints of Jupiter and Saturn respectively, the primary planets are described from the standpoint of the sun, and the moon is described from the standpoint of the Earth.  And because Newton doesn’t prioritise the observer, effects such the phases and retrograde motions of the planets are not phenomena but only evidence of phenomena.

The re-labelling of these propositions as ‘phenomena’ is somewhat puzzling.  The term ‘phenomenon’ has a variety of uses, such as:*

  1. A particular (kind of) fact, occurrence, or change, which is perceived or observed, the cause or explanation of which is in question;
  2. An immediate object of sensation or perception (often as distinguished from a real thing or substance); or
  3. An exceptional or unaccountable thing, fact or occurrence.

But, as we’ve seen, Newton’s ‘phenomena’ don’t properly fit any of these definitions.  Can any reader shed light on what Newton really meant by the term?

 

* Definitions (a) and (c) feature in both C18th and C21st dictionaries, but in the C21st, definition (b) has become more prominent, particularly in philosophy.

 

UPDATE: I have written a follow-up post.

 

 

4 thoughts on “Newton’s ‘Phenomena’

  1. Does understanding the expression as ‘data to be accounted for’ work? Loosely relevant: Fodor’s “The Dogma that Didn’t Bark” and Owen’s “Tithenai ta phainomena.”

  2. Hi Mike,

    Thanks for pointing me towards those two papers.

    In response to your question: I’ve been thinking of Newton’s phenomena as distinct from the data (or evidence) that supports them. Of course, in Newton’s case, this distinction is muddied by the fact that even the data (listed in tables under each phenomenon) are already generalised and isolated to some degree – they are average distances, and calculated periods of orbit; not pure ‘data’. Also, Newton’s tables have an extra piece of supporting evidence that surely can’t be considered ‘data’ in the sense of observation: he states the average distance calculated from the period and the Harmonic Rule. This illustrates the ‘fit’ between the expected distance and the observed distance. Nevertheless, these tables are supposed to support the phenomena, and, in turn, the phenomena support the propositions. There doesn’t appear to be any direct interaction between the data and the propositions, which suggests that data and phenomena are methodologically distinct.

    Does that sound right?

    Cheers,
    Kirsten

  3. Perhaps ‘data’ isn’t the best word. I suppose that he’s thinking of phenomena as things known which are to be explained and which can support more general propositions. Something doesn’t have to be directly observed to be a phenomenon in his sense (which is your point, of course).

    Best,
    Mike

  4. A continuity in Newton’s method would be consistent with his approaches elsewhere. Your point about relative motions is pertinent. He is not looking at absolute motion. I think that Newton is in harmony with the greek sense of phenomena as referring to a fact or event in the changing and perceptible forms, as distinct from the permanent essences of things. Your point about the observer is also pertinent, because the motions of these bodies about a central fixed referand is being looked at from the viewpoint of Jupiter, Moon etc. as observers. These events are phenomena for them. The change in terminology is interesting, as you say, since it seems to mark a solidifying of Newton’s commitment to a universally applicable self-consciousness whereby each and every body becomes aware of itself as a self through its sense of presence of an other whereby the limits of self are first experienced and ultimately established.
    Does that make sense?