# Philosophiae Naturalis Principia Mathematica

For an in-depth account, see the writing of Principia Mathematica.
File:NewtonsPrincipia.jpg
Newton's own copy of his Principia, with hand written corrections for the second edition.

The Philosophiae Naturalis Principia Mathematica (Latin: "mathematical principles of natural philosophy", often Principia or Principia Mathematica for short) is a three-volume work by Isaac Newton published on July 5, 1687. It contains the statement of Newton's laws of motion forming the foundation of classical mechanics as well as his law of universal gravitation. He derives Kepler's laws for the motion of the planets (which were first obtained empirically).

In formulating his physical theories, Newton had developed a field of mathematics known as calculus. However, the language of calculus was largely left out of the Principia. Instead, Newton recast the majority of his proofs as geometric arguments.

It is in the Principia that Newton expressed his famous Hypotheses non fingo ("I feign no hypotheses", that is, "I do not assert that any hypotheses are true"). Here is the translated passage containing this famous remark:

I have not as yet been able to discover the reason for these properties of gravity from phenomena, and I do not feign hypotheses. For whatever is not deduced from the phenomena must be called a hypothesis; and hypotheses, whether metaphysical or physical, or based on occult qualities, or mechanical, have no place in experimental philosophy. In this philosophy particular propositions are inferred from the phenomena, and afterwards rendered general by induction.

## The historical context

### The beginnings of the scientific revolution

Nicholas Copernicus had firmly moved the earth away from the center of the universe with the heliocentric theory that he presented evidence for in his book De revolutionibus orbium celestium (On the revolutions of the heavenly spheres) published in 1543. The structure was completed when Johannes Kepler wrote the book Astronomia nova (A new astronomy) in 1609, setting out the evidence that planets move in elliptical orbits with the sun at one focus, and that planets do not move with constant speed along this orbit but their speed varies so that the line joining the centers of the sun and a planet sweeps out equal parts of the ellipse in equal times. To these two laws he added a third a decade later, in his otherwise forgettable book Harmonices Mundi (Harmonies of the world). This law sets out a proportionality between the third power of the average distance of a planet from the sun and the square of the length of its year.

The foundations of modern dynamics was set out in Galileo's book Dialogo sopra i due massimi sistemi del mondo (Dialogue on the two main world systems) where the notion of inertia was implicit and used. In addition, Galileo's experiments with inclined planes had yielded precise mathematical relations between elapsed time and acceleration, velocity or distance for uniform and uniformly accelerated motion of bodies.

Descartes' book of 1644 Principia philosophiae (Principles of philosophy) stated that bodies can act on each other only through contact: a principle that induced people, among them he himself, to conjecture a universal medium as the carrier of interactions such as light and gravity— the aether. Another mistake was his treatment of circular motion, but this was more fruitful in that it led others to identify circular motion as a problem raised by the principle of inertia. Christiaan Huygens solved this problem in the 1650s and published it much later.

### Newton's context

Newton had studied these books, or, in some cases, secondary sources based on them, and taken notes entitled Quaestiones quadem philosophicae (Questions about philosophy) during his days as an undergraduate. During this period (1664–1666) he created the basis of calculus, and performed the first experiments in the optics of colour. In addition he took two crucial steps in dynamics: first, in the course of an analysis of the impact between two bodies, he deduced correctly that the center of mass remains in uniform motion, second, he made his first, but mistaken, analysis of circular motion assuming that there must exist a (repulsive) centrifugal force. At this time, the central notion of inertia still remained outside his understanding. He summarized this work in a note which he called "The lawes of Motion" (preserved in the Cambridge University Library as the Additional MS 3958).

Over the following years, he published his experiments on light and the resulting theory of colours, to overwhelmingly favourable response, and a few inevitable scientific disputes with Robert Hooke and others, which forced him to sharpen his ideas to the point where he composed sections of his later book Opticks already by the 1670s. He wrote up bits and pieces of the calculus in various papers and letters, including two to Leibnitz. He became a fellow of the Royal Society and the second Lucasian Professor of Mathematics (succeeding Isaac Barrow) at Trinity College, Cambridge.

He had already, in the plague year of 1665, had the famous revelation under an apple tree in Woolesthorpe which led him to the conclusion that the strength of gravity falls off in inverse square of the distance, by substituting Kepler's third law into his derivation of the centrifugal force, muddled as it was through his misunderstanding of the nature of circular motion (in The lawes of motion).

Hooke, in 1674, wrote Newton a letter (later published in 1679 in his book Lectiones Cutlerianes) through which Newton first understood of the role of inertia in the problem of circular motion— that the tendency of a body is to fly off in a straight line, and that an attractive force must keep it moving in a circle. In reply Newton drew (and described) a fancied trajectory of a body, initially with only tangential velocity, falling towards a centre of attraction in a spiral. Hooke noted this error and corrected it, saying that with an inverse square force law the correct path would be an ellipse, and made the exchange public by reading both Newton's letter and his correction to the Royal Society in 1676. Newton tried a rearguard action by giving the orbits in various other kinds of central potentials in another letter to Hooke, thus showing his mastery over the method. In 1677, in a conversation with Christopher Wren, Newton realized that Wren had also arrived at the inverse square law by exactly the same method as him.

It is not known when he performed his experiment with a rotating bucket with water, and even if he actually performed it at all. But such reflections on the effects of circular motion brought him to his concept of "absolute space" which served as basis for his definitions of motion.

Newton had still not completed all the steps in the construction of the Principia by 1681, when a comet was observed to turn around the sun. The astronomer royal, John Flamsteed, recognized the motion as such, whereas most scientists believed that there were two comets, one which disappeared behind the sun, and another which appeared later from the same direction. The correspondence between Flamsteed and Newton showed that the latter had not grasped the point of the universality of the law of gravity that till then only few knew.

This was the state of affairs when Edmund Halley visited Newton in Cambridge in August 1684, having rediscovered the inverse square law by substituting Kepler's law into Huygens' formula for the centrifugal force. In January of that year Halley, Wren and Hooke had a conversation where Hooke claimed to not only derive the inverse square law, but also all the laws of planetary motion. Wren was unconvinced, and Halley, having failed in the derivation himself, resolved to ask Newton. Newton said that he had already made the derivations but could not find the papers. Matching accounts of this meeting come from Halley and Abraham DeMoivre to whom Newton confided.

In November 1684, Halley received a treatise of nine pages called De motu corporum in gyrum (On the motion of bodies in an orbit). It derived the three laws of Kepler assuming an inverse square law of force, and generalized the answer to conic sections. It extended the methodology of dynamics by adding the solution of a problem on the motion of a body through a resisting medium. After another visit to Newton, Halley reported these results to the Royal Society on 1684-12-10 (Julian calendar). Newton also communicated these results to Flamsteed, but insisted on revising the manuscript. These crucial revisions, especially concerning the notion of inertia, eventually turned into the Principia.

## Publication

The text was presented to the Royal Society in 1686, and on 30 June Samuel Pepys, as President, was authorised to licence it for publication. Unfortunately the Society had just spent their book budget on a history of fish, so the initial cost of publication was borne by Edmund Halley. [1]

## The contents of the book

In the preface of the Principia, Newton wrote6

... rational mechanics will be the science of motion resulting from any forces whatsoever, and of the forces required to produce any motion ... and therefore I offer this work as the mathematical principles of philosophy, for the whole burden of philosophy seems to consist in this — from the phenomena of motions to investigate the forces of nature, and then from these forces to demonstrate the other phenomena ...

It was perhaps the force of the Principia, which explained so many different things about the natural world with such economy, that caused this method to become synonymous with physics, even as it is practised almost three and a half centuries after his beginning. Today the two aspects that Newton outlined would be called analysis and synthesis.

The Principia consists of three books

1. De motu corporum (On the motion of bodies) is a mathematical exposition of calculus followed by statements of basic dynamical definitions and the primary deductions based on these. It also contains propositions and proofs that have little to do with dynamics but demonstrate the kinds of problems which can be solved using calculus.
2. The second book was broken off from the first, since it would have otherwise become too long. It contains sundry applications such as motion through a resistive medium, a derivation of the shape of least resistance, a derivation of the speed of sound and accounts of experimental tests of the result.
3. De mundi systemate (On the system of the world) is an essay on universal gravitation that builds upon the propositions of the previous books and applies them to the motions observed in the solar system — the regularities and the irregularities of the orbit of the moon, the derivations of Kepler's laws, applications to the motion of Jupiter's moons, to comets and tides (much of the data came from John Flamsteed). It also considers the harmonic oscillator in three dimensions, and motion in arbitrary force laws.

The sequence of definitions used in setting up dynamics in the Principia is exactly the same as in all textbooks today. Newton first set out the definition of mass6

The quantity of matter is that which arises conjointly from its density and magnitude. A body twice as dense in double the space is quadruple in quantity. This quantity I designate by the name of body or of mass.

This was then used to define the "quantity of motion" (today called momentum), and the principle of inertia in which mass replaces the previous Cartesian notion of intrinsic force. This then set the stage for the introduction of forces through the change in momentum of a body. Curiously, for today's readers, the exposition looks dimensionally incorrect, since Newton does not introduce the dimension of time in rates of changes of quantities.

He defined space and time "not as they are well known to all". Instead, he defined "true" time and space as "absolute" and explained:

Only I must observe, that the vulgar conceive those quantities under no other notions but from the relation they bear to perceptible objects. And it will be convenient to distinguish them into absolute and relative, true and apparent, mathematical and common. [...] instead of absolute places and motions, we use relative ones; and that without any inconvenience in common affairs; but in philosophical discussions, we ought to step back from our senses, and consider things themselves, distinct from what are only perceptible measures of them.

It is interesting that several dynamical quantities which were used in the book (such as angular momentum) were not given names. The dynamics of the first two books was so self-evidently consistent that it was immediately accepted; for example, Locke asked Huygens whether he could trust the mathematical proofs, and was assured about their correctness.

However, the concept of an attractive force acting at a distance received a cooler response. In his notes, Newton wrote that the inverse square law arose naturally due to the structure of matter. However, he retracted this sentence in the published version, where he stated that the motion of planets is consistent with an inverse square law, but refused to speculate on the origin of the law. Huygens and Leibniz noted that the law was incompatible with the notion of the ether. From a Cartesian point of view, therefore, this was a faulty theory. Newton's defence has been adopted since by many famous physicists — he pointed out that the mathematical form of the theory had to be correct since it explained the data, and he refused to speculate further on the basic nature of gravity. The sheer mass of phenomena which could be organized by the theory was so impressive that younger "philosophers" soon adopted the methods and language of the Principia.

## The mathematical language

The reason for Newton's extension of Euclidean geometry as the mathematical language of choice in Principia is puzzling in two respects. The first is the puzzle that today's physicists, trained in modern analytical methods, descended from Descartes, face in reconstructing the arguments. This mathematical language reportedly baffled Richard Feynman to the extent that he tried to work out alternative Euclidean proofs to his own satisfaction. S. Chandrasekhar, in one of his last major efforts, translated the Principia into modern mathematical language so that physicists of today can read and appreciate the book that founded modern physics.

The second puzzle is historical. Why did Newton revert to Euclidean methods when seventeenth century mathematics increasingly used Descartes' analytical geometry for its transactions. Newton himself had written earlier tracts using this language. Even his earlier communications on the calculus of differentials referred to a new language of fluxions that he had invented. In fact, his early notebooks suggest strongly that he learnt Cartesian geometry long before he came to Euclid. Some commentators have suggested that Newton used the mathematical language of Euclid in order to make a rhetorical point about how his methods followed easily from the Greek tradition. However, this piece of rhetoric was unnecessary for his contemporaries, who knew very well the general nature of Newton's mathematical discoveries. A second point that has been made is that Newton had to reject Descartes' views on inertia in order to understand and generalize Galileo's new ideas. He simultaneously rejected Descartes' new language of geometry: since he recognized that it was equivalent to Euclid's, and it lay within Newton's powers to recast the calculus in these terms.

## Location of copies

File:Principia Page 1726.jpg
A page from the Principia

Many national rare book collections contain original copies of Newton's Principia Mathematica. Notable examples are

• The Wren Library in Trinity College Cambridge has Newton's own copy of the first edition, with hand written notes for the second edition.
• The Whipple Museum of the History of Science in Cambridge has a first edition copy which used to belong to Robert Hooke.
• Fisher Library in the University of Sydney has a first edition copy, annotated by a mathematician of uncertain identity and corresponding notes from Newton himself.
• The Pepys Library in Magdalene College Cambridge, has Samuel Pepys' copy of the third edition.
• The Martin Bodmer Library keeps a copy of the original edition that was owned by Leibniz. In it, we can see hand-written notes by Leibniz, in particular concerning the controversy of who invented calculus (although he published it later, Newton claimed that he invented it earlier). As an interesting side-note, the copy shows clear signs that Leibniz was an avid smoker.

A facsimile edition was published in 1972 by Alexandre Koyré and I. Bernard Cohen, Cambridge University Press, 1972, ISBN 0674664752.

Two more editions were published during Newton's lifetime:

### Second Edition

Richard Bentley, master of Trinity College, influenced Roger Cotes, Plumian professor of astronomy at Trinity, to undertake the editorship of the second edition. Newton did not intend to start any re-write of the Principia until 17091. Under the weight of Cotes' efforts, but impeded by priority disputes between Newton and Leibniz2, and by troubles at the Mint3, Cotes was able to announce publication to Newton 30 June 17134. Bentley sent Newton only six presentation copies; Cotes was unpaid; Newton omitted any acknowledgement to Cotes.

Among those who gave Newton corrections for the Second Edition were:

However, Newton omitted acknowledgements to some because of the priority disputes. John Flamsteed, the Astronomer Royal, suffered this especially.

### Third Edition

The third edition was published 25 March 1726, under the stewardship of Henry Pemberton, M.D., a man of the greatest skill in these matters ...; Pemberton later said that this recognition was worth more to him than the two hundred guinea award from Newton.5

## Notes

• Note 1: p.699, Richard S. Westfall. Never at Rest: A Biography of Isaac Newton. Cambridge U. Press. 1980 ISBN 0-521-27435
• Note 2: Westfall, pp.712–716
• Note 3: Westfall, pp.751–760
• Note 4: Westfall, p.750
• Note 5: Westfall, p.802
• Note 6: J. W. Herivel, The background to Newton's "Principia", Oxford University Press, 1965.
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