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<v Speaker 1>Chapter eighteen, Part two of A Short Account of the

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<v Speaker 1>History of Mathematics. This is a LibriVox recording. All LibriVox

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<v Speaker 1>recordings are in a public domain. For more information or

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<v Speaker 1>to volunteer, please visit LibriVox dot org. This is a

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<v Speaker 1>reading by Paul King p J K dot scrips dot

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<v Speaker 1>m I T dot E d U forward slash p

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<v Speaker 1>K J. A Short Account of the History of mathematics

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<v Speaker 1>by W. W. Rouse Baul. Chapter eighteen Leibniz and the

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<v Speaker 1>Mathematicians of the first half of the eighteenth century, Part two.

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<v Speaker 1>Lambert Johann Heinrich Lambert was born at Mulhausen on August

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<v Speaker 1>twenty eighth, seventeen twenty eight and died at Berlin on

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<v Speaker 1>September twenty fifth, seventeen seventy seven. He was the son

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<v Speaker 1>of a small tailor and had to rely on his

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<v Speaker 1>own efforts for his education. From a clerk in some

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<v Speaker 1>iron works, he got a place in a newspaper office,

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<v Speaker 1>and subsequently, on the recommendation of the editor, he was

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<v Speaker 1>appointed tutor in a private family, which secured him the

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<v Speaker 1>use of a good library and sufficient leisure to use it.

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<v Speaker 1>In seventeen fifty nine he settled in Augsburg, and in

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<v Speaker 1>seventeen thirty three removed to Berlin, where he was given

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<v Speaker 1>a small pension and finally made editor of the Prussian

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<v Speaker 1>Astronomical Almanac. Lambel's most important work were one on optics,

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<v Speaker 1>issued in seventeen fifty nine, which suggested to arago the

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<v Speaker 1>lines of investigation. He subsequently pursued a treatise on perspective,

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<v Speaker 1>published in seventeen fifty nine, to which in seventeen sixty

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<v Speaker 1>eight an appendix given practical applications was added, and a

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<v Speaker 1>treatise on comets printed in seventeen sixty one, containing the

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<v Speaker 1>well known expression for the area of a focal sector

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<v Speaker 1>of a conic in terms of the cord and the

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<v Speaker 1>bounding race. Besides these, he communicated numerous papers to the

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<v Speaker 1>Berlin Academy. Of the most important are his memoir in

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<v Speaker 1>seventeen sixty eight on transcendental magnitudes, in which he proved

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<v Speaker 1>that pi is incommensurable. The proof is given in Legendre's geometry,

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<v Speaker 1>and is there extended to pi squared. His paper on trigonometry,

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<v Speaker 1>read in seventeen sixty eight, in which he developed Demoffra's

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<v Speaker 1>theorems on the trigonometry of complex variables, and introduced the

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<v Speaker 1>hyperbolic sign and co sign, denoted by the symbols sign

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<v Speaker 1>h x cohx. His essay entitled the Analytical Observations, published

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<v Speaker 1>in seventeen seventy one, which is the earliest attempt to

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<v Speaker 1>form the functional equations by expressing the given properties in

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<v Speaker 1>the language of the differential calculus and then integrating. Lastly,

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<v Speaker 1>his paper on viz Viva published in seventeen eighty three,

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<v Speaker 1>in which for the first time he expressed Newton's second

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<v Speaker 1>law of motion in the notation of the differential calculus.

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<v Speaker 1>Of the other mathematicians above mentioned, I hear add a

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<v Speaker 1>few words. Etienne Bezous born in Nemours on March thirty first,

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<v Speaker 1>seventeen thirty and died on September twenty seventh, seventeen eighty three.

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<v Speaker 1>Besides numerous minor works, wrote to Therrie Generreal de sequeigion Algebraque,

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<v Speaker 1>published at Paris in seventeen seventy nine, which in particular

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<v Speaker 1>contained much new and valuable matter on the theory of

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<v Speaker 1>elimination and symmetrical functions of the roots of an equation.

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<v Speaker 1>He used his determinants in a paper in the Histoire

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<v Speaker 1>de leca Demi Royale seventeen sixty four, but did not

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<v Speaker 1>treat of the general theory. Jean Trembrey born at Geneva

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<v Speaker 1>in seventeen forty nine and died at September eighteenth, eighteen eleven,

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<v Speaker 1>contributed to the development of differential equations, finite differences, and

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<v Speaker 1>the calculus of probabilities. Louis Francois d'artoine Abregaste born a

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<v Speaker 1>dal Sas on October fourth, seventeen fifty nine and died

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<v Speaker 1>at Strasbourg, where he was professor, on April eighth, eighteen

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<v Speaker 1>o three, wrote on series and the derivatives. Known by

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<v Speaker 1>his name, he was the first writer to separate the

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<v Speaker 1>symbols of operation from those of quantity. I do not

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<v Speaker 1>wish to crowd my pages with an account of those

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<v Speaker 1>who have not distinctly advanced the subject, but I have

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<v Speaker 1>mentioned the above writers because their names are still well known.

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<v Speaker 1>We may, however, say that the discoveries of Euler and

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<v Speaker 1>Lagrange in the subjects which they treated, were so complete

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<v Speaker 1>and far reaching that what their less gifted contemporary he's

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<v Speaker 1>added is not of sufficient importance to require mention in

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<v Speaker 1>a book of this nature. Lagrange. Joseph Louis Lagrange, the

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<v Speaker 1>greatest mathematician of the eighteenth century, was born at Turin

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<v Speaker 1>on January twenty fifth, seventeen thirty six, and died at

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<v Speaker 1>Paris on April tenth, eighteen thirteen. His father, who had

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<v Speaker 1>the charge of the Sardinian Military Chest, was of good

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<v Speaker 1>social position and wealthy, but before his son grew up,

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<v Speaker 1>he had lost most of his property in speculations, and

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<v Speaker 1>young Lagrange had to rely for his position on his

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<v Speaker 1>own abilities. He was educated at the College of Tyrann,

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<v Speaker 1>but was not until he was seventeen that he chewed

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<v Speaker 1>any taste for mathematics, his interest in the subject being

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<v Speaker 1>first excited by a memoir by Halley across which he

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<v Speaker 1>came by accident, alone and unaided. He threw himself into

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<v Speaker 1>mathematical studies, and at the end of a year's incessant toil,

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<v Speaker 1>he was already an accomplished mathematician, and was made a

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<v Speaker 1>lecturer in the artillery school. The first of these labors

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<v Speaker 1>was his letter, written when he was still only nineteen

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<v Speaker 1>to Euler, in which he solved the isoparametrical problem, which

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<v Speaker 1>for more than half a century had been the subject

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<v Speaker 1>of discussion to effect a solution in which he sought

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<v Speaker 1>to determine the form of a function so that a

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<v Speaker 1>formula in which it entered should satisfy a certain condition.

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<v Speaker 1>He enunciated the principles of the calculus of variations. Euler

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<v Speaker 1>recognized the generality of the method adopted and its superiority

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<v Speaker 1>to that used by himself, and with rare courtesy he

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<v Speaker 1>withheld a paper that he had previously written, which covered

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<v Speaker 1>some of the same ground, in order that the young

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<v Speaker 1>Italian might have time to complete his work and claim

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<v Speaker 1>the undisputed invention of the new calculus. The name of

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<v Speaker 1>this branch of analysis was suggested by Euler. This memoir

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<v Speaker 1>at once placed Lagrange in the front rank of mathematicians.

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<v Speaker 1>Then living. In seventeen fifty eight, Lagrange established, with the

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<v Speaker 1>aid of his pupils, a society which was subsequently incorporated

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<v Speaker 1>as the Turan Academy, and in the five volumes of

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<v Speaker 1>its transactions, usually known as the Miscellanea Tourernensia, most of

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<v Speaker 1>his early writings are to be found. Many of these

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<v Speaker 1>are elaborate works. The first volume contains a memoir of

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<v Speaker 1>the theory of the propagation of sound and in this

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<v Speaker 1>he indicates a mistake made by Newton, obtains a general

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<v Speaker 1>differential equation for the motion, and integrates it for motion

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<v Speaker 1>in a straight line. This volume also contains the complete

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<v Speaker 1>solution of the problem of a string vibrating transversely. In

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<v Speaker 1>this paper, he points out a lack of generality in

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<v Speaker 1>the solutions previously given by Taylor, de Lambert and Euler,

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<v Speaker 1>and arrives at the con inclusion that form of a

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<v Speaker 1>curve at any time T is given by the equation

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<v Speaker 1>y equals a sign mx sign nt. The article concludes

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<v Speaker 1>with a masterly discussion of echoes, beats, and compound sounds.

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<v Speaker 1>Other articles in this volume are on recurring series probabilities

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<v Speaker 1>and the calculus of variations. The second volume containing a

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<v Speaker 1>long paper embodying the results of several memoirs in the

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<v Speaker 1>first volume on the theory and notation of the calculus

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<v Speaker 1>of variations, and he illustrates its use by deducing the

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<v Speaker 1>principle of least action and also by solutions of various

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<v Speaker 1>problems in dynamics. The third volume includes a solution of

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<v Speaker 1>several dynamical problems by means of the calculus of variations.

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<v Speaker 1>Some papers on the integral calculus, a solution of Fermat's

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<v Speaker 1>problem mentioned above, and on the general differential equations of

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<v Speaker 1>motion for three bodies moved under their mutual attractions. In

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<v Speaker 1>seventeen sixty one, Lagrange stood without arrival as the foremost

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<v Speaker 1>mathematician living, But the unceasing labour of the preceding nine

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<v Speaker 1>years had seriously affected his health, and the doctors refused

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<v Speaker 1>to be responsible for his reason or life unless he

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<v Speaker 1>would take rest and exercise. Although his health was temporarily restored,

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<v Speaker 1>his nervous system never quite recovered its tone, and henceforth

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<v Speaker 1>he constantly suffered from attacks of profound melancholy. The next

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<v Speaker 1>work he produced was in seventeen sixty four on the

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<v Speaker 1>libration of the Moon and an explanation as to why

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<v Speaker 1>the same face was always turned to the Earth, a

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<v Speaker 1>problem which he treated by aid of virtual work. His

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<v Speaker 1>solution is especially interesting as containing the germ of the

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<v Speaker 1>idea of generalized equations of motion equations, which he first

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<v Speaker 1>formally proved in seventeen eighty. He now started to go

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<v Speaker 1>on a visit to London, but on the way fell

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<v Speaker 1>ill at Paris. There he was received with the most

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<v Speaker 1>marked honour, and it was with regret that he left

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<v Speaker 1>the brilliant society of that city to return to his

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<v Speaker 1>provincial life at Tehran. His further stay in Piedmont was,

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<v Speaker 1>however short. In seventeen sixty six, Euler left Berlin, and

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<v Speaker 1>Frederick the Great immediately wrote expressing the wish of the

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<v Speaker 1>greatest king in Europe to have the greatest mathematician in

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<v Speaker 1>Europe resident in his court. Lagrange accepted the offer and

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<v Speaker 1>spent the next twenty years at Prussia, where he produced

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<v Speaker 1>not only the long series of memoirs published at the

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<v Speaker 1>Berlin and Tyran Transactions, but his monumental work Mechanique Anarritique.

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<v Speaker 1>His residence at Berlin commenced with an unfortunate mistake, finding

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<v Speaker 1>most of his colleagues married and assured by their wives

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<v Speaker 1>that it was the only way to be happy. He married,

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<v Speaker 1>his wife soon died, but the union was not a

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<v Speaker 1>happy one. Lagrange was a favorite of the King, who

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<v Speaker 1>used frequently to discourse to him on the advantage of

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<v Speaker 1>perfect regularity of life. The lesson went home, and thenceforth

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<v Speaker 1>Lagrange studied his mind and body as though they were machines,

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<v Speaker 1>and found by experiment the exact amount of work which

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<v Speaker 1>he was able to do without breaking down. Every night

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<v Speaker 1>he set himself a definite task for the next day,

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<v Speaker 1>and on completing any branch of a subject, he wrote

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<v Speaker 1>a short analysis to see what points in the demonstrations

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<v Speaker 1>or in the subject matter were capable of improvement. He

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<v Speaker 1>always thought out the subject of his papers before he

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<v Speaker 1>began to compose them, and usually wrote them straight off

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<v Speaker 1>without a single erasure or correction. His mental activity during

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<v Speaker 1>these twenty years was amazing. Not only did he produce

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<v Speaker 1>his splendid mechanique and rietique, but he contributed between one

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<v Speaker 1>and two hundred papers to the academies of Berlin, Tyrann

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<v Speaker 1>and Paris. Some of these are complete treatises, and all,

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<v Speaker 1>without exception, are of Hahaigh order of excellence, except for

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<v Speaker 1>a short time when he was ill, and produced on

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<v Speaker 1>an average about one memoir a month. Of these, I

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<v Speaker 1>note the following as among the most important. First, his

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<v Speaker 1>contributions to the fourth and fifth volumes seventeen sixty six

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<v Speaker 1>to seventeen seventy three of the Miscellanea Taurernensia, of which

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<v Speaker 1>the most important was the one in seventeen seventy one,

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<v Speaker 1>in which he discussed how numerous astronomical observations should be

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<v Speaker 1>combined so as to give the most probable result, and

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<v Speaker 1>later his contributions to the first two volumes seventeen eighty

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<v Speaker 1>four to seventeen eighty five of the Transactions of the

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<v Speaker 1>Turin Academy, to the first of which he contributed a

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<v Speaker 1>paper on the pressure exerted by fluids in motion, and

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<v Speaker 1>to the second an article on integration by infinite series

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<v Speaker 1>and the kind of problems for which it is suitable.

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<v Speaker 1>Most of the memoirs sent to Paris were on astronomical questions,

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<v Speaker 1>and among these I ought particularly to mention his memoir

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<v Speaker 1>on the Jovian System in seventeen sixty six, his essay

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<v Speaker 1>on the problem of the three bodies in seventeen seventy two,

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<v Speaker 1>his work on the secular equation of the Moon in

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<v Speaker 1>seventeen seventy three, and his treatise on cometary perturbations in

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<v Speaker 1>seventeen seventy eight. These were all written on subjects proposed

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<v Speaker 1>by the French Academy, and in each case the prize

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<v Speaker 1>was awarded to him. The greater number of his papers

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<v Speaker 1>during the same time were, however, contributed to the Berlin Academy.

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<v Speaker 1>Several of them deal with questions on algebra. In particular.

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<v Speaker 1>I may mention one his discussion of the solution of

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<v Speaker 1>indeterminate equations on integers in seventeen seventy with special notice

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<v Speaker 1>of indeterminate quadratics in seventeen sixty nine, two, His tract

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<v Speaker 1>on the Theory of Elimination seventeen seventy three, His Memoirs

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<v Speaker 1>on the General Process for solving in algebraical equations of

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<v Speaker 1>any degree seventeen seventy and seventeen seventy one. This method

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<v Speaker 1>fails for equations of an order above the fourth, because

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<v Speaker 1>then it involves a solution of an equation of higher

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<v Speaker 1>dimensions than the one proposed, but it gives all the

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<v Speaker 1>solutions of his predecessors as modifications of a single principle.

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<v Speaker 1>He found, however, the complete solution of the binomial equations

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00:14:45.039 --> 00:14:49.000
<v Speaker 1>of any degree and fourth. Lastly, in seventeen seventy three

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<v Speaker 1>he treated of determinants of the second and third order.

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<v Speaker 1>Several of his early papers also deal with questions connected

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<v Speaker 1>with the neglected but singularly fascinating suchbject of the theory

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00:15:00.879 --> 00:15:04.639
<v Speaker 1>of numbers. Among these are one his proof of the

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00:15:04.639 --> 00:15:08.519
<v Speaker 1>theorem that every integer which is not a square can

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<v Speaker 1>be expressed as a sum of either two, three, or

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<v Speaker 1>four integral squares seventeen seventy His proof of Wilson's theorem

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<v Speaker 1>the off n b prime, then n minus one factorial

222
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<v Speaker 1>plus one is always a multiple of nds seventeen seventy one. Three,

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<v Speaker 1>His memoirs of seventeen seventy three, seventeen seventy five, and

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<v Speaker 1>seventeen seventy seven, which give the demonstrations of several results

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00:15:35.960 --> 00:15:41.120
<v Speaker 1>enunciated by format and not previously proved. Four And lastly,

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<v Speaker 1>his method for determining the factors of numbers of the

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<v Speaker 1>form x squared plus a y squared. There are also

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<v Speaker 1>numerous articles on various points of analytical geometry. In two

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<v Speaker 1>of them, in seventeen ninety two and seventeen ninety three,

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<v Speaker 1>he reduced the equations of the quadrix or conochoids to

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<v Speaker 1>their canonical forms. During the years from seventeen seventy two

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<v Speaker 1>to seventeen eighty five he contributed a long series of

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<v Speaker 1>memoirs which created the science of deferential equations at any rate,

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<v Speaker 1>as far as partial differential equations are concerned, I do

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<v Speaker 1>not think that any previous writer had done anything beyond

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<v Speaker 1>considering equations of some particular form. A large part of

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00:16:26.200 --> 00:16:29.399
<v Speaker 1>these results were collected in the second edition of Euler's

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<v Speaker 1>Integral Calculus, which was published in seventeen ninety four. His

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<v Speaker 1>papers on mechanics require no separate mention here, as the

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00:16:38.360 --> 00:16:43.639
<v Speaker 1>results arrived at are embodied in the mechanique analytique, which

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00:16:43.679 --> 00:16:48.679
<v Speaker 1>is described below. Lastly, there are numerous memoirs on problems

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00:16:48.679 --> 00:16:53.000
<v Speaker 1>in astronomy. Of these, the most important are the following one,

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<v Speaker 1>The Attraction of ellipsoids seventeen seventy three. This is founded

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<v Speaker 1>on mclaurin's work two on the secular equation of the

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00:17:02.000 --> 00:17:07.240
<v Speaker 1>Moon seventeen seventy three. Also noticeable for the earliest introduction

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<v Speaker 1>of the idea of the potential. The potential of a

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<v Speaker 1>body at any point is the sum of the mass

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<v Speaker 1>of every element of the body when divided by its

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00:17:17.000 --> 00:17:21.480
<v Speaker 1>distance from the point. Lagrant should that if the potential

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00:17:21.519 --> 00:17:24.559
<v Speaker 1>of a body at an external point were known, the

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00:17:24.640 --> 00:17:28.960
<v Speaker 1>attraction in any direction could be at once found. The

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00:17:28.960 --> 00:17:32.119
<v Speaker 1>theory of the potential was elaborated in a paper sent

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<v Speaker 1>to Berlin in seventeen seventy seven three on the motion

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<v Speaker 1>of the nodes of a planet's orbit seventeen seventy four.

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<v Speaker 1>Four on the Stability of Planetary orbits seventeen seventy six, five.

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<v Speaker 1>Two memoirs in which the method of determining the orbit

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00:17:51.839 --> 00:17:55.160
<v Speaker 1>of a comet from three observations is completely worked out

258
00:17:55.279 --> 00:17:59.640
<v Speaker 1>seventeen seventy eight and seventeen eighty three. This is not

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00:17:59.640 --> 00:18:03.440
<v Speaker 1>indeed proved practically available, but his system of calculating the

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00:18:03.480 --> 00:18:07.759
<v Speaker 1>perturbations by means of mechanical quadratures has formed the basis

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<v Speaker 1>of most subsequent researches on the subject. Six His Determination

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<v Speaker 1>of the secular and periodic variations of the elements of

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<v Speaker 1>the planets seventeen eighty one to seventeen eighty four. The

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<v Speaker 1>upper limits assigned for these agree closely with those obtained

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<v Speaker 1>later by Leverrier, and he proceeded as far as the

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<v Speaker 1>knowledge then possessed of the masses of the planets permitted seven.

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<v Speaker 1>Three Memoirs on the method of interpolation seventeen eighty three,

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<v Speaker 1>seventeen ninety two, and seventeen ninety three. The part of

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<v Speaker 1>finite differences dealing Therewith is now in the same stage

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<v Speaker 1>as that in which Lagrange left it. Over and above

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<v Speaker 1>these various papers, he composed his great treatise Mechanique Analytique.

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<v Speaker 1>In this he lays down the law of virtual work,

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<v Speaker 1>and from that one fundamental principle, by the age of

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00:19:00.240 --> 00:19:03.839
<v Speaker 1>the calculus of variations, he deduces the whole of mechanics,

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00:19:03.960 --> 00:19:07.960
<v Speaker 1>both of solids and fluids. The object of the book

276
00:19:08.039 --> 00:19:10.880
<v Speaker 1>is to shew that the subject is implicitly included in

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00:19:10.960 --> 00:19:14.400
<v Speaker 1>a single principle, and to give the general formulae from

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00:19:14.640 --> 00:19:18.720
<v Speaker 1>which any particular result can be obtained. The method of

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00:19:18.799 --> 00:19:22.519
<v Speaker 1>generalized coordinates by which he obtained this result is perhaps

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00:19:22.519 --> 00:19:26.519
<v Speaker 1>the most brilliant result of his analysis. Instead of following

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00:19:26.559 --> 00:19:29.759
<v Speaker 1>the motion of each individual part of a material system,

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00:19:31.039 --> 00:19:34.440
<v Speaker 1>as de Lambert and Euler had done, he shewed that

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00:19:34.480 --> 00:19:37.759
<v Speaker 1>if we determine its configuration by a sufficient number of

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00:19:37.839 --> 00:19:40.200
<v Speaker 1>variables whose number is the same as that of the

285
00:19:40.240 --> 00:19:43.759
<v Speaker 1>degrees of freedom possessed by the system, then the connecticut

286
00:19:43.839 --> 00:19:46.720
<v Speaker 1>potential energies of the system can be expressed in terms

287
00:19:46.759 --> 00:19:50.640
<v Speaker 1>of these, and the differential equations of motions then deduced

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00:19:50.680 --> 00:19:55.200
<v Speaker 1>by simple differentiation, for example, in dynamics of a rigid system.

289
00:19:55.279 --> 00:19:58.519
<v Speaker 1>He replaces the consideration of the particular problem by the

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00:19:58.559 --> 00:20:01.319
<v Speaker 1>general equation, which is no now usually written in the

291
00:20:01.359 --> 00:20:05.480
<v Speaker 1>form of D by dt times the partial derivative of

292
00:20:05.839 --> 00:20:09.480
<v Speaker 1>capital T with respect to theta minus, the partial derivative

293
00:20:09.519 --> 00:20:12.880
<v Speaker 1>of capital T with respect to theta plus the partial

294
00:20:12.920 --> 00:20:19.160
<v Speaker 1>derivative of V with respect to theta equals zero, amongst

295
00:20:19.599 --> 00:20:23.359
<v Speaker 1>other minor theorems. Here given, I may mention the proposition

296
00:20:23.440 --> 00:20:27.119
<v Speaker 1>that the kinetic energy imparted by given impulses to a

297
00:20:27.160 --> 00:20:32.240
<v Speaker 1>material system under given constraints is a maximum, and the

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00:20:32.240 --> 00:20:36.640
<v Speaker 1>principle of least action. All the analysis is so elegant

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00:20:36.680 --> 00:20:40.440
<v Speaker 1>that Sir William Rowan Hamilton said the work could be

300
00:20:40.559 --> 00:20:45.279
<v Speaker 1>only described as a scientific poem. It may be interesting

301
00:20:45.359 --> 00:20:48.359
<v Speaker 1>to note that Legrange remarked that the mechanics was really

302
00:20:48.440 --> 00:20:51.880
<v Speaker 1>a branch of pure mathematics, analogous to a geometry of

303
00:20:51.920 --> 00:20:56.839
<v Speaker 1>four dimensions, namely the time and the three coordinates of

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00:20:56.880 --> 00:20:59.799
<v Speaker 1>the point in space. And it is said that he

305
00:21:00.000 --> 00:21:03.559
<v Speaker 1>he prided himself that from the beginning to the end

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00:21:03.599 --> 00:21:07.160
<v Speaker 1>of the work there was not a single diagram. At first,

307
00:21:07.160 --> 00:21:09.359
<v Speaker 1>no printer could be found who had published the book.

308
00:21:09.480 --> 00:21:13.240
<v Speaker 1>Be Legendre at last persuaded a Paris firm to undertake it,

309
00:21:13.759 --> 00:21:17.599
<v Speaker 1>and it was issued under his supervision in seventeen eighty eight.

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<v Speaker 1>In seventeen eighty seven, Frederick died, and Lagrange, who had

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<v Speaker 1>found the climate of Berlin trying, gladly accepted the offer

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00:21:26.880 --> 00:21:30.680
<v Speaker 1>of Louis the sixteenth to migrate to Paris. He received

313
00:21:30.880 --> 00:21:34.720
<v Speaker 1>similar invitations from Spain and Naples. In France, he was

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00:21:34.799 --> 00:21:38.559
<v Speaker 1>received with every mark of distinction, and special apartments in

315
00:21:38.680 --> 00:21:42.799
<v Speaker 1>the Louverre were prepared for his reception. For the first

316
00:21:42.880 --> 00:21:46.079
<v Speaker 1>two years of his residence here he was seized with

317
00:21:46.200 --> 00:21:50.079
<v Speaker 1>an attack of melancholy, and even the printed copy of

318
00:21:50.160 --> 00:21:53.000
<v Speaker 1>his mechanique on which he had worked for a quarter

319
00:21:53.000 --> 00:21:56.039
<v Speaker 1>of a century, lay for more than two years unopened

320
00:21:56.079 --> 00:22:00.240
<v Speaker 1>on his desk. Curiosity as to the results so the

321
00:22:00.279 --> 00:22:03.839
<v Speaker 1>French Revolution first stirred him out of his lethargy, a

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00:22:04.119 --> 00:22:08.200
<v Speaker 1>curiosity which soon turned to alarm as the revolution developed.

323
00:22:08.920 --> 00:22:12.640
<v Speaker 1>It was about the same time, seventeen ninety two, that

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<v Speaker 1>the unaccountable sadness of his life and timidity moved the

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<v Speaker 1>compassion of a young girl, who insisted on marrying him

326
00:22:21.519 --> 00:22:25.200
<v Speaker 1>and proved a devoted wife to whom he became warmly attached.

327
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<v Speaker 1>Although the decree of October seventeen ninety three, which ordered

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00:22:29.880 --> 00:22:34.359
<v Speaker 1>all foreigners to leave France, specially exempted him by name.

329
00:22:35.680 --> 00:22:38.759
<v Speaker 1>He was preparing to escape when he was offered the

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<v Speaker 1>presidency of the Commission for the Reform of Weights and Measures.

331
00:22:43.400 --> 00:22:46.599
<v Speaker 1>The choice of the units finally selected was largely due

332
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<v Speaker 1>to him, and it was mainly owing to his influence

333
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<v Speaker 1>that the decimal subdivision was accepted by the Commission of

334
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<v Speaker 1>seventeen ninety nine. The general idea of the decimal system

335
00:22:59.319 --> 00:23:03.039
<v Speaker 1>was taken from a work by Thomas Williams entitled Method

336
00:23:03.119 --> 00:23:08.000
<v Speaker 1>for Fixing a Universal Standard for Weights and Measures, published

337
00:23:08.000 --> 00:23:11.960
<v Speaker 1>in London in seventeen eighty eight. This almost unknown writer

338
00:23:12.160 --> 00:23:17.680
<v Speaker 1>has hardly received the credit due to his suggestion. Though

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<v Speaker 1>Lagrange had determined to escape from France while there was

340
00:23:21.880 --> 00:23:25.559
<v Speaker 1>yet time, he was never in any danger, and the

341
00:23:25.559 --> 00:23:30.400
<v Speaker 1>different revolutionary governments and at a later time Napoleon loaded

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00:23:30.480 --> 00:23:34.319
<v Speaker 1>him with honors and distinctions. A striking testimony to the

343
00:23:34.359 --> 00:23:37.319
<v Speaker 1>respect in which he was held was shewn in seventeen

344
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<v Speaker 1>ninety six when the French Commissary in Italy ordered to

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<v Speaker 1>attend in full state on Lagrange's father and tender the

346
00:23:44.680 --> 00:23:48.119
<v Speaker 1>congratulations of the Republic on the achievements of his son,

347
00:23:48.680 --> 00:23:52.200
<v Speaker 1>who had done honor to all mankind by his genius,

348
00:23:52.240 --> 00:23:54.880
<v Speaker 1>and whom it was a special glory of Piedmont to

349
00:23:54.960 --> 00:23:59.240
<v Speaker 1>have produced. In seventeen ninety five, Lagrange was appointed to

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00:23:59.279 --> 00:24:03.759
<v Speaker 1>a mathematic chair at the newly established Echol Noomal which

351
00:24:03.920 --> 00:24:08.319
<v Speaker 1>only enjoyed a brief existence of four months. His lectures

352
00:24:08.359 --> 00:24:12.880
<v Speaker 1>here were quite elementary and contain nothing of any special importance.

353
00:24:13.160 --> 00:24:16.720
<v Speaker 1>But they were published because the professors had to pledge

354
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<v Speaker 1>themselves to the representatives of the people and to each other,

355
00:24:21.119 --> 00:24:24.680
<v Speaker 1>neither to read nor to repeat from memory, and the

356
00:24:24.759 --> 00:24:28.759
<v Speaker 1>discourses were ordered to be taken down in shorthand in

357
00:24:28.960 --> 00:24:32.319
<v Speaker 1>order to enable the deputies to see how the professors

358
00:24:32.319 --> 00:24:37.680
<v Speaker 1>acquitted themselves. On the establishment of the Ecole Polytechnique in

359
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<v Speaker 1>seventeen ninety seven, Lagrange was made a professor, and his

360
00:24:42.359 --> 00:24:45.440
<v Speaker 1>lectures there are described by mathematicians who had the good

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00:24:45.519 --> 00:24:48.799
<v Speaker 1>fortune to be able to attend them, as almost perfect,

362
00:24:48.960 --> 00:24:52.519
<v Speaker 1>both in form and matter. Beginning with the merest elements,

363
00:24:52.559 --> 00:24:55.759
<v Speaker 1>he led his hearers on until almost unknown to themselves,

364
00:24:55.839 --> 00:24:59.640
<v Speaker 1>they were themselves extending the bounds of the subject. Above all,

365
00:24:59.680 --> 00:25:02.799
<v Speaker 1>he pressed on his pupils the advantage of always using

366
00:25:02.880 --> 00:25:07.599
<v Speaker 1>general methods expressed in a symmetrical notation. His lectures on

367
00:25:07.640 --> 00:25:11.200
<v Speaker 1>the differential calculus form the basis of his Theire de

368
00:25:11.440 --> 00:25:16.440
<v Speaker 1>Functio Analytique, which was published in seventeen ninety seven. This

369
00:25:16.599 --> 00:25:19.039
<v Speaker 1>work is the extension of an idea contained in a

370
00:25:19.079 --> 00:25:22.559
<v Speaker 1>paper he had sent to the Berlin Memoirs in seventeen

371
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<v Speaker 1>seventy two, and its object is to substitute for the

372
00:25:26.079 --> 00:25:29.480
<v Speaker 1>differential calculus as a group of theorems based on the

373
00:25:29.519 --> 00:25:34.119
<v Speaker 1>development of algebraic functions in series. A somewhat similar method

374
00:25:34.200 --> 00:25:38.119
<v Speaker 1>had been previously used by John Landon in his Residual Analysis,

375
00:25:38.160 --> 00:25:42.559
<v Speaker 1>published in London in seventeen fifty eight. Lagrange believed that

376
00:25:42.640 --> 00:25:46.200
<v Speaker 1>he could thus get rid of those difficulties connected with

377
00:25:46.240 --> 00:25:49.920
<v Speaker 1>the use of infinitely large or infinitely small quantities which

378
00:25:49.960 --> 00:25:54.279
<v Speaker 1>philosophers professed to see in the usual treatment of the

379
00:25:54.279 --> 00:25:59.200
<v Speaker 1>differential calculus. The book is divided into three parts. Of these,

380
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<v Speaker 1>the first treats of the general theory of functions and

381
00:26:03.279 --> 00:26:06.920
<v Speaker 1>gives an algebraic proof of Taylor's theorem, the validity of

382
00:26:06.960 --> 00:26:10.119
<v Speaker 1>which is, however, to open the question. The second deals

383
00:26:10.119 --> 00:26:14.880
<v Speaker 1>with applications to geometry, and the third with applications to mechanics.

384
00:26:15.319 --> 00:26:18.559
<v Speaker 1>Another treatise on the same lines was his lessence Le

385
00:26:18.680 --> 00:26:23.359
<v Speaker 1>Calcure de function, issued in eighteen o four. These works

386
00:26:23.400 --> 00:26:26.359
<v Speaker 1>may be considered as the starting point for the researches

387
00:26:26.400 --> 00:26:30.799
<v Speaker 1>of Koshi and Jacoby. At a later period, Lagrange reverted

388
00:26:30.839 --> 00:26:34.440
<v Speaker 1>to the use of infinitesimals in preference to the founding

389
00:26:34.519 --> 00:26:38.119
<v Speaker 1>the differential calculus on a study of algebraic forms, and

390
00:26:38.240 --> 00:26:40.960
<v Speaker 1>in the preface to the second edition of the Mechanique,

391
00:26:41.240 --> 00:26:44.759
<v Speaker 1>which was issued in eighteen eleven, he justifies their use

392
00:26:44.799 --> 00:26:48.079
<v Speaker 1>and concludes by saying that when we have grasped the

393
00:26:48.160 --> 00:26:52.359
<v Speaker 1>spirit of the infinitesimal method, and have verified the exactness

394
00:26:52.359 --> 00:26:55.759
<v Speaker 1>of its results, either by the geometrical method of prime

395
00:26:55.799 --> 00:27:01.039
<v Speaker 1>and ultimate ratios or by the analytical method of derived functions,

396
00:27:01.480 --> 00:27:05.759
<v Speaker 1>we may employ infinitely small quantities as a sure and

397
00:27:05.920 --> 00:27:11.400
<v Speaker 1>valuable means of shortening and simplifying our proofs. His resolution

398
00:27:11.480 --> 00:27:15.680
<v Speaker 1>des equasion nu meric, published in seventeen ninety eight, was

399
00:27:15.759 --> 00:27:19.720
<v Speaker 1>also the fruit of his lectures at the Polytechnic. In

400
00:27:19.759 --> 00:27:23.400
<v Speaker 1>this he gives the method of approximating to the real

401
00:27:23.480 --> 00:27:27.279
<v Speaker 1>roots of an equation by means of continued fractions and

402
00:27:27.519 --> 00:27:31.039
<v Speaker 1>enunciates several other theorems. In a note at the end,

403
00:27:31.119 --> 00:27:34.839
<v Speaker 1>he shews how Fermat's theorem that a to the power

404
00:27:34.839 --> 00:27:38.559
<v Speaker 1>of p minus one minus one is defined as zero

405
00:27:38.680 --> 00:27:42.319
<v Speaker 1>mod p, where p is prime and a is prime

406
00:27:42.400 --> 00:27:46.079
<v Speaker 1>to p, combined with a certain suggestion due to Gauss,

407
00:27:46.519 --> 00:27:50.039
<v Speaker 1>may be applied to give the complete algebraical solution of

408
00:27:50.079 --> 00:27:55.319
<v Speaker 1>any binomial equation. He also here explains how the equation

409
00:27:55.480 --> 00:27:57.960
<v Speaker 1>whose roots are the squares of the differences of the

410
00:27:58.039 --> 00:28:01.119
<v Speaker 1>roots of the original equation, may be used so as

411
00:28:01.160 --> 00:28:04.240
<v Speaker 1>to give considerable information so as to the position and

412
00:28:04.400 --> 00:28:09.319
<v Speaker 1>nature of those roots. The theory of the planetary motions

413
00:28:09.359 --> 00:28:11.880
<v Speaker 1>had formed the subject of some of the most remarkable

414
00:28:11.920 --> 00:28:15.720
<v Speaker 1>of Lagrange's Berlin papers. In eighteen oh six a subject

415
00:28:15.799 --> 00:28:19.440
<v Speaker 1>was reopened by Poissan, who, in a paper read before

416
00:28:19.480 --> 00:28:23.000
<v Speaker 1>the French Academy, she shewed that Lagrange's formula led to

417
00:28:23.680 --> 00:28:27.440
<v Speaker 1>certain limits for the stability of the orbits. La Grange,

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<v Speaker 1>who was present, now discussed the whole subject afresh, and,

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<v Speaker 1>in a memoir communicated to the Academy in eighteen oh eight,

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<v Speaker 1>explained how, by the variation of arbitrary constance, the periodical

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<v Speaker 1>and secular inequalities of any system of mutually interacting bodies

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<v Speaker 1>could be determined. In eighteen ten, Lagrange commenced the thorough

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<v Speaker 1>revision of the Mechanique an letique, but he was able

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<v Speaker 1>to complete only about two thirds of it before his death.

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<v Speaker 1>In appearance, he was of medium height and slightly formed,

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<v Speaker 1>with pale blue eyes colorless complexion. In character, he was

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<v Speaker 1>nervous and timid. He detested controversy, and to avoid it

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<v Speaker 1>willingly allowed others to take the credit for what he

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<v Speaker 1>had himself done. Lagrange was, above all a student of

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<v Speaker 1>pure mathematics. He sought and obtained far reaching abstract results,

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<v Speaker 1>and was content to leave the applications to others. Indeed,

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<v Speaker 1>no considerable part of the discoveries of his great contemporary

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<v Speaker 1>Laplace consists of the applications of the Lagrangian formulae to

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<v Speaker 1>the facts of nature. For example, Laplace's conclusions on the

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<v Speaker 1>velocity of sound and the secular acceleration of the moon

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<v Speaker 1>are implicitly involved in Lagrange's results. The only difficulty in

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<v Speaker 1>understanding Lagrange is that of the subject matter and of

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<v Speaker 1>the extreme generality of his processes. But his analysis is

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<v Speaker 1>as lucid and luminous as it is symmetrical and ingenious.

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<v Speaker 1>A recent writer, speaking of verg Lagrange, says truly that

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<v Speaker 1>he took a prominent part in the advancement of almost

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<v Speaker 1>every branch of pure mathematics. Like Theophantus and Fermat, he

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<v Speaker 1>proposed a special genius for the theory of numbers, and in

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<v Speaker 1>this subject he gave solutions of most of the problems

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<v Speaker 1>which had been proposed by Fermat and added some theorems

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<v Speaker 1>of his own. He created the calculus of variations. To him, too,

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<v Speaker 1>the theory of differential equations is indebted for its position

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<v Speaker 1>as a science, rather than as a collection of ingenious

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<v Speaker 1>artifices for the solution of particular problems. To the calculus

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<v Speaker 1>of finite differences, he contributed the formula of interpolation, which

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<v Speaker 1>bears his name. But above all he impressed a mechanics which,

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<v Speaker 1>it will be remembered. He considered a part of pure

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<v Speaker 1>mathematics that generality and completeness towards which his labours invariably tended.

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<v Speaker 1>Section thirty one recording by Paul King, Oakville, Ontario, p

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<v Speaker 1>J K dot scripts dot M I T dot E

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<v Speaker 1>d U forward slash p K J
