ISAAC NEWTON

Isaac Newton (1642-1727)Isaac Newton was born December 25th, 1642, at Woolsthorpe, near Grantham in Lincolnshire, where his family had held a small landed property for generations. As a boy, at the Grantham Grammar School, he was slow in book-learning, and much absorbed in mechanical contrivances. At 17 he entered Trinity College, Cambridge. Here he devoted himself eagerly to mathematical study, meditating principally on the Geometry of Descartes, published in 1637, and on the Arithmetica Infinitorum of Wallis, published 1655. In 1667 he was elected Fellow of his college, and two years afterward he succeeded Barrow as Professor of Mathematics. From this chair his lectures on Optics were given. In 1672 he was elected a Fellow of the Royal Society. In 1686 his great treatise on Natural Philosophy, the Principia, was completed, and the next year published. In 1687 he was one of the delegates chosen to defend his University against the encroachments of James II; and in 1689 he represented it in Parliament. In 1695 he was made Warden, and in 1699 Master, of the Mint. In 1703 he became President of the Royal Society, and was re-elected every year till his death, which took place on the 28th of February 1727. He was buried in Westminster Abbey.

The splendour of Newton's discoveries has led many writers to isolate his work from what had been done before him, and was being done in his own time by others. But the History of Science is a fundamental part of the History of Humanity, and the life of no man, however great, should be treated thus. And further, to Newton, as to others, the canon must be applied that publication is the proper test of priority.

Kepler's three laws, that the planets moving round the sun described equal areas in equal times, that their orbits were elliptical, the sun being in one of the foci, and that the squares of their times of revolution were as the cubes of their mean distances, were discovered a generation before Newton's birth. But they remained unreduced to any law of force. Kepler had indeed shown that the force must proceed from the sun, and had put forward the mistaken conjecture that it varied inversely as the distance. Kepler was strongly convinced of the identity between terrestrial weight and planetary attraction, and made an estimate, on this erroneous basis, of the mutual fall of the earth and moon, supposing no other force intervened. Ismael Boulliaud, in his Astronomia Philolaica, published 1645, suggested that gravitation acted not inversely as the distance, but inversely as the square of the distance. But these views rested on vague analogies between gravitation and the radiation of light fromm a focus; and till they could be mathematically tested they received, and deserved, but slight attention.

The law of falling bodies had been accurately given by Galileo. But no attempt had been made to connect it with the laws of planetary motion. In 1665, Newton, being then at Woolsthorpe, thought of investigating the space through whichh the moon in a given time was deflected from the tangent to her path--in other words, fell towards the earth. He found that in one minute the moon fell thirteen feet. Taking the best estimate available to him of the earth's magnitude, from which the moon's parallax, and thence her distance, were to be estimated, he found that, on the supposition that gravitation acted inversely as the square of the distance, the fall of the moon in one minute should not be thirteen, but fifteen feet. He thereforee quietly put the hypothesis aside; a striking example of scientific forbearance. Seven years afterwards, Picard's more exact measurement of the earth's magnitude reached him from Paris. Newton at once resumed his calculations, causing them, for greater certainty, to be completed by a disinterested observer. The correcter statement of facts was found to tally with his hypothesis of gravitation.

It is often supposed that the problem of explaining the planetary motions was now solved. In reality, the difficult part of the work--that which tests Newton's intellectual greatness--had still to be done. The problem before him was to show how Kepler's Third Law, that the squares of the periods of the planets varied as the cubes of their mean distances from the sun, followed mathematically from the supposition of an attractive force, acting inversely as the square of the distance, situate in the focus of an ellipse. Further, this force had to be regarded not as acting upon a particle, but on a planet; i.e. a system of particles. No vague hypothesis could be useful here: no application of such mathematics as were then known could suffice.

In 1673 appeared the great work of Huyghens on the Pendulum and on Centrifugal Force. This contributed in two ways to the solution. Huyghens' laws of centrifugal force gave the measure of the force which retained the planets in their orbits, supposing the orbits circular. And further, in his discussion of the Pendulum, Huyghens had attacked the problem of a system of particles rigidly connected, and each animated with its own tendencies to motion. Newton acknowledged his debt to Huyghens; but in passing from circular to elliptic motion, and above all for his demonstration that the attractive force exercised by the molecules of a sphere might be regarded as condensed in its center, ordinary geometry, even after its algebraic expansion by Descartes and his mathematical successors, was insufficient.

Foremost among these successors stood Newton. And it was at this time--that is to say about 1666--that he constructed the Transcendental Calculus, by the aid of which his great treatise was written; though, for reasons which seem to us now quite inadequate, he presented his demonstrations in the language of ordinary geometry. On the claims for priority to the invention of this calculus a bitter controversy arose between the friends of Leibniz and of Newton. It is admitted now that Newton made his discovery prior to and independently of Leibniz. But no description of Newton's Fluxions was published until 1693. The letters of Leibniz show that he had invented his Differential and Integral Calculus in 1675; and a full account of it was published in the Acta Eruditorum at Leipsic, 1684. It must be further admitted that the differentials and integrals of Leibniz proved more fertile in the subsequent development of mathematics than the fluxions and fluents of Newton.

But it fell to the lot of Newton to combine the discovery of the calculus with what was by far the most important of his applications. And hence it is that the Principia, notwithstanding the archaic form into which he thought fit to transpose his discoveries, will by many be looked upon as the greatest, by all as one of the two or three great masterpieces, of scientific intellect. In unity of purpose, though not in native power, it surpasses the work of Archimedes; in the importance of its application, though not in philosophic breadth, the Mécanique of Lagrange.

Newton's mathematical and experimental researches on light and colour, which began with his installation as Professor of Mathematics, were first communicated to the Royal Society in 1672, and were finally published in a complete form in 1704. The experimental part of his work, to which the analysis of white light into component colours of different refrangibility--a subject opened by Descartes--is but the prelude, remains of indestructible value.

And finally, it must not be forgotten that to Newton we owe the establishment of the Third Law of Motion, the equality of action and reaction: a law stated by him in that large and comprehensive way which enables us to include among the reactions the conversion of sensible into insensible motion; so that it illumines and corrects much modern speculation upon work and energy.

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This biography is reprinted from The New Calendar of Great Men. Ed. Frederic Harrison. London: Macmillan and Co., 1920.

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