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Titlebook: A Course in Elasticity; B. M. Fraeijs Veubeke Book 1979 Springer-Verlag New York Inc. 1979 Calculation.Elastizität.Finite.Invariant.algebr

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发表于 2025-3-21 16:39:31 | 显示全部楼层 |阅读模式
期刊全称A Course in Elasticity
影响因子2023B. M. Fraeijs Veubeke
视频videohttp://file.papertrans.cn/141/140467/140467.mp4
学科分类Applied Mathematical Sciences
图书封面Titlebook: A Course in Elasticity;  B. M. Fraeijs Veubeke Book 1979 Springer-Verlag New York Inc. 1979 Calculation.Elastizität.Finite.Invariant.algebr
影响因子This book is based on lecture notes of the late Professor de Veubeke. The subject is presented at a level suitable for graduate students in engineering, physics, or mathematics. Some exposure to linear algebra, complex analysis, variational calculus, or basic continuum mechanics would be helpful. The first third of the book contains the fundamentals of the theory of elasticity. Kinematics of continuous media, the notions of stress and equilibrium, conservation of energy, ‘and the elastic constitutive law are each treated first in a nonlinear context, then specialized to the linear case. The remainder of the book is given to three classic applications of the theory, each supplemented by original re­ sults based on the use of complex variables. Each one of the three topics - Saint-Venant‘s theory of prismatic beams, plane deformations, and the bending of plates - is first pre­ sented and analyzed in general, then rounded out with numerous specific and sometimes novel examples. The following notational conventions are generally in force, except where noted to the contrary: lower case boldface letters denote vectors or triples of Cartesian co­ ordinates, upper case boldface letters den
Pindex Book 1979
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Back Matternd Antwort "ver­ absolutiert" sieht. Dies erinnert mich allzusehr an mündliche Prüfungen alter deutscher Ordinarienherrlichkeit, wie sie in unzähligen Witzen und Anekdoten karikiert und überliefert ist. Dieses Arbeitsbuch erfüllt seinen Sinn nur, wenn es dazu beiträgt, daß der Studierende eine gewis
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https://doi.org/10.1007/978-94-007-7537-4tic body. (Non-repeated Latin subscripts will be assumed to range over the values 1, 2, 3.) Let y. denote the coordinates of the same point in a deformed or final configuration. The displacement vector has components u. = y. - x..
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African Literary NGOs (LINGOs),sentation . in terms of its components u.. The orthogonal projections of the vector on the axes,. are identical with its components. As long as we use only Cartesian frames we do not need the distinction between contravariant components, usually defined by (4.2), and covariant components, usually de
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