Mécanique analytique
著者
書誌事項
Mécanique analytique
（Cambridge library collection, . Mathematical sciences）
Cambridge University Press, 2009
- v. 1 : pbk
- v. 2 : pbk
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注記
Reprint of neuv. éd., rev. et augm. par l'auteur. Originally published: Paris : Courcier, 1811-1815
内容説明・目次
- 巻冊次
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v. 1 : pbk ISBN 9781108001755
内容説明
Joseph-Louis Lagrange (1736-1813), one of the notable French mathematicians of the Revolutionary period, is remembered for his work in the fields of analysis, number theory and mechanics. Like Laplace and Legendre, Lagrange was assisted by d'Alembert, and it was on the recommendation of the latter and the urging of Frederick the Great himself that Lagrange succeeded Euler as the director of mathematics at the Prussian Academy of Sciences in Berlin. The two-volume Mecanique analytique was first published in 1788; the edition presented here is that of 1811-15, revised by the author before his death. In this work, claimed to be the most important on classical mechanics since Newton, Lagrange developed the law of virtual work, from which single principle the whole of solid and fluid mechanics can be derived.
目次
- Part I. La statique
- Part II. La dynamique.
- 巻冊次
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v. 2 : pbk ISBN 9781108001762
内容説明
Joseph-Louis Lagrange (1736-1813), one of the notable French mathematicians of the Revolutionary period, is remembered for his work in the fields of analysis, number theory and mechanics. Like Laplace and Legendre, Lagrange was assisted by d'Alembert, and it was on the recommendation of the latter and the urging of Frederick the Great himself that Lagrange succeeded Euler as the director of mathematics at the Prussian Academy of Sciences in Berlin. The two-volume Mecanique analytique was first published in 1788; the edition presented here is that of 1811-15, revised by the author before his death. In this work, claimed to be the most important on classical mechanics since Newton, Lagrange developed the law of virtual work, from which single principle the whole of solid and fluid mechanics can be derived.
目次
Part II. La dynamique (continued).
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