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terrestrial phenomena mentioned in the earlier section, previous page. Although, late in 1679,
not long after he had embraced the concept, another application was suggested
in a letter from Robert Hooke, who was seeking to renew correspondence. Robert Hooke
mentioned his analysis of planetary motion--in effect, the continuous diversion of a
rectilinear motion by a central attraction. Newton bluntly refused to correspond
but, nevertheless, went on to mention an experiment to demonstrate the rotation
of the Earth: let a body be dropped from a tower; because the tangential velocity
at the top of the tower is greater than that at the base, the body should fall
slightly to the east. He sketched the path of fall as part of a spiral ending at the
centre of the Earth. This was a mistake, as Hooke pointed out; according to
Hooke's theory of planetary motion, the path should be elliptical, so that if the
Earth were split and separated to allow the body to fall, it would rise again to its
original location. Newton did not like being corrected, least of all by Hooke, but Newton
had to accept the basic point; he corrected Hooke's figure, used the
assumption that gravity is constant. Robert Hooke countered by replying that,
although Isaac Newton's figure was correct for constant gravity, his own assumption
was that gravity decreases as the square of the distance. Several years later, this
letter became the basis for Hooke's charge of plagiarism. He was mistaken in the
charge. His knowledge of the inverse square relation rested only on intuitive
grounds; he did not derive it properly from the quantitative statement of
centripetal force and Kepler's third law, which relates the periods of planets to
the radii of their orbits. Moreover, unknown to him, Newton had so derived the
relation more than ten years earlier. Nevertheless, Newton later confessed that
the correspondence with Hooke led him to demonstrate that an elliptical orbit
entails an inverse square attraction to one focus--one of the two crucial
propositions on which the law of all gravitation would ultimately depend. What is
more, Robert Hooke's description of orbiting motion--in which the constant action of an
attracting body continuously pulls an object away from its inertial path--suggested a
cosmic application for Newton's concept of force and an explanation of planetary
paths employing it. In 1679 and 1680, Newton dealt only with orbital dynamics; he
had not yet arrived at the concept of universal gravitation.
Universal gravitation
Almost five years later, in August 1684, Newton was visited by the English
scientific astronomer Edmond Halley, who was also troubled by the problem of orbital
dynamics. Upon learning that Newton had solved the problem, he extracted
Newton's promise to send the demonstration. Three months later he received a
short tract entitled De Motu ("On Motion"). Already Newton was at work improving
and expanding it. In two and a half years, the tract De Motu grew into Philosophiae
Naturalis Principia Mathematica, which is not only Isaac Newton's masterpiece but also
the basis book for the whole of modern science.
Significantly, De Motu did not state the law of universal gravitation. For that
matter, even though it was a treatise on planetary dynamics, it did not contain any
of the three laws of motion. Only when revising De Motu did Isaac Newton
embrace the principle of inertia his first law and arrive at the second law of
motion. The second law, the force law, proved to be an accurate
statement of the action of the forces between bodies which had become the
central members of his system of nature. When quantifying the idea of force, the
second law completed the exact fundamental of mechanics which has been the
model of natural science ever since.
The precise mechanics of the Principia are not to be mistaken with the
mechanical philosophy. The latter is a philosophy of nature which endeavours to
show natural events by means of imagined mechanisms among unobserverable
particles.
Continued
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