Page:Encyclopædia Britannica, Ninth Edition, v. 14.djvu/222

 210 LAGRANGE perhaps unduly what he could not approve, and was emphatically, in his own phrase, &quot; philosophe sans crier.&quot; The delicacy of his health demanded precautions ex aggerated, under the influence of nervous anxiety, into minute watchfulness. He observed a scrupulous regimen, living mainly on fruit and vegetables, and his temperance doubtless helped to keep his faculties unimpaired to the last. By self-imposed rules of study, he regulated his vast capability of work as strictly as if it had been a machine entrusted to his care. It was one of his maxims that the mind gains full command over its powers only by exercise and discipline. He had learned from Frederick the Great always to do the same things at the same hours, assigning the most difficult to the morning. Each day he set himself a task for the next, and from the first aimed at mastering certain points of his subject, with a view to inventing improvements. He always read with a pen in his hand, developing the methods of his author as he proceeded ; and his own works were so profoundly meditated that they were usually written without erasures. Amongst the brilliant group of mathematicians whose magnani mous rivalry contributed to accomplish the task of generalization and deduction reserved for the 18th century Lagrange occupies an eminent place. It is, however, by no means easy to distinguish and apportion the respective merits of the competitors. This is especially the case between Lagrange and Euler on the one side, and between Lagrauge and Laplace on the other. The calculus of varia tions lay undeveloped in Euler s mode of treating isoperimetrical problems. The fruitful method, again, of the variation of elements was introduced by Euler, but adopted and perfected by Lagrange, who first recognized its supreme importance to the analytical investigation of the planetary movements. Finally, of the grand series of researches by which the stability of the solar system was ascertained the glory must be almost equally divided between Lagrange and Laplace. In analytical invention, and mastery over the calculus, the Turin mathematician was admittedly unrivalled. Laplace owned that he had despaired of effecting the integration of he differential equations relative to secular inequalities until Lagrange showed him the way. On the other hand, Laplace unquestionably surpassed his rival in practical sagacity, and the intuition of physical truth. Lagrange saw in the problems of nature so many occasions for analytical triumphs ; Laplace regarded analytical triumphs as the means of solving the problems of nature. One mind seemed, as it were, the complement of the other ; and both united in honourable rivalry formed an instrument of unexampled perfection for the investigation of the celestial machinery. What may be called Lagrange s first period of research into planetary perturbations extended from 1774 to 1784 (see ASTRONOMY, vol. ii. p. 761). The remarkable group of treatises communicated, 1781-84, to the Berlin Academy was designed, but did not prove, to be his final contribution to the theory of the planets. After an interval of twenty-four years the subject, having been reopened by Poisson in a paper read June 20, 1808, was once more attacked by Lagrange with all his pristine vigour and fertility of invention. Resuming the inquiry into the invariability of mean motions, Poisson carried the approximation, with Lagrange s formulae, as far as the squares of the disturbing forces, hitherto neglected, with the same result as to the stability of the system. He had not, however, attempted to include in his calculations the orbital variations of the disturbing bodies ; but Lagrange, by the happy artifice of transferring the origin of coordinates from the centre of the sun to the centre of gravity of the sun and planets, obtained a simplification of the formulae, by which the same analysis was rendered equally applicable to each of the planets severally. It deserves to be recorded as one of the numerous coin cidences of discovery that Laplace, on being made acquainted by Lagrange with his new method, produced analogous expressions, to which his independent researches had led him. The final achieve ment of Lagrange in this direction was the extension of the method of the variation of arbitrary constants, successfully used by him in the investigation of periodical as well as of secular inequalities, to any system whatever of mutually interacting bodies. 1 &quot;Not without astonishment,&quot; even to himself, regard being had to the great generality of the differential equations, he reached a result so wide as to include, as a particular case, the solution of the planetary problem recently obtained by him. He proposed to apply the same principles to the calculation of the disturbances produced in the rotation of the planets by external action on their equatorial pro tuberances, but was anticipated by Poisson, who gave formula; for the variation of the elements of rotation strictly corresponding with those found by Lagrange for the variation of the elements of revolu- 1 OSuvres, vi. p. 771. tion. The revision of the Mecanique Analytique was undertaken mainly for the purpose of embodying in it these new methods and final results, but was interrupted, when two-thirds completed, by the death of its author. In the advancement of almost every branch of pure mathematics Lagrange took a conspicuous part. The calculus of variations is indissolubly associated with his name. In the theory of numbers he furnished solutions of many of Fermat s theorems, and added some of his own. In algebra he discovered the method of approxi mating to the real roots of an equation by means of continued frac tions, and imagined a general process of solving algebraical equations of every degree. The method indeed fails for equations of an order above the fourth, because it then involves the solution of an equa tion of higher dimensions than the proposed. It possesses, however, the great and characteristic merit of generalizing the solutions of his predecessors, exhibiting them all as modifications of one prin ciple. To Lagrange, perhaps more than to any other, the theory of differential equations is indebted for its position as a science, rather than a collection of ingenious artifices for the solution of particular problems. To the calculus of finite differences he contributed the beautiful formula of interpolation which bears his name ; although substantially the same result seemed to have been previously obtained by Euler. But it was in the application to mechanical questions of the instrument which he thus helped to form that his singular merit lay. It was his just boast to have transformed mechanics (defined by him as a &quot;geometry of four dimensions&quot;) into a branch of analysis, and to have exhibited the so-called mechanical &quot;principles&quot; as simple results of the calculus. The method of &quot;generalized coordinates,&quot; as it is now called, 2 by which he attained this result, is the most brilliant achievement of the analytical method. Instead of following the motion of each indi vidual part of a material system, he showed that, if we determine its configuration by a sufficient number of variables, whose number is that of the degrees of freedom to move (there being as many equations as the system has degrees of freedom), the kinetic and potential energies of the system can be expressed in terms of these, and the differential equations of motion thence deduced by simple differentiation. Besides this most important contribution to the general fabric of dynamical science, we owe to Lagrange several minor theorems of great elegance among which may be mentioned his theorem that the kinetic energy imparted by given impulses to a material system under given constraints is a maximum. To this entire branch of knowledge, in short, he successfully imparted that character of generality and completeness towards which his labours invariably tended. His share in the gigantic task of verifying the Newtonian theory would alone suffice to immortalize his name. His co-operation was indeed more indispensable than at first sight appears. Much as was done by him, what was done through him was still more import ant. Some of his brilliant rival s most conspicuous discoveries were implicitly contained in his writings, and wanted but one step for completion. But that one step, from the abstract to the concrete, was precisely that which the character of Lagrange s mind indis posed him to make. As notable instances may be mentioned Laplace s discoveries relating to the velocity of sound and the secular acceleration of the moon, both of which were led close up to by Lagrange s analytical demonstrations. In the Berlin Memoirs for 1778 and 1783 Lagrange gave the first direct and theoreti cally perfect method of determining cometary orbits. It has not indeed proved practically available ; but his system of calcu lating cometary perturbations by means of &quot;mechanical quadra tures &quot; has formed the starting-point of all subsequent researches on the subject. His determination 3 of maximum and minimum values for the slowly varying planetary eccentricities was the earliest attempt to deal with the problem. Without a more accurate knowledge of the masses of the planets than was then possessed a satisfactory solution was indeed impossible ; but the upper limits assigned by him agreed closely with those obtained later by Leverrier. 4 As a mathematical writer Lagrange has per haps never been surpassed. His treatises are not only storehouses of ingenious methods, but models of symmetrical form. The clear ness, elegance, and originality of his mode of presentation give lucidity to what is obscure, novelty to what is familiar, and sim plicity to what is abstruse. His genius was one of generalization and abstraction ; and the aspirations of the time towards unity and perfection received, by his serene labours, an embodiment denied to them in the troubled world of politics. Lagrange s numerous scattered memoirs hare been collected and published in seven handsome 4to volumes, under the title (Euvres de Lagrange, ptibliees sous les sains de M. J. A. Serret, Paris, 1867-77. The first, second, and third sections of this important publication comprise respectively the papers communicated by him to the Academies of Sciences of Turin, Berlin, and Paris ; the fourth includes his miscellaneous contributions to other scientific collections, together with his additions to Euler s Algebra, and his Lemons Elementaires at the Ecole Normale in 1795. Delambre s notice of his life, extracted from the Mem. de 2 We use the modern terms by which the functions introduced by Lagrange are now denoted. 3 (Euvres, v. p. 211 sq. 4 Grant, History of Physical Astronomy, p. 117.