標(biāo)題: Titlebook: An Introduction to Modern Variational Techniques in Mechanics and Engineering; B. D. Vujanovic,T. M. Atanackovic Textbook 2004 Springer Sc [打印本頁(yè)] 作者: Asphyxia 時(shí)間: 2025-3-21 19:12
書(shū)目名稱An Introduction to Modern Variational Techniques in Mechanics and Engineering影響因子(影響力)
書(shū)目名稱An Introduction to Modern Variational Techniques in Mechanics and Engineering影響因子(影響力)學(xué)科排名
書(shū)目名稱An Introduction to Modern Variational Techniques in Mechanics and Engineering網(wǎng)絡(luò)公開(kāi)度
書(shū)目名稱An Introduction to Modern Variational Techniques in Mechanics and Engineering網(wǎng)絡(luò)公開(kāi)度學(xué)科排名
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書(shū)目名稱An Introduction to Modern Variational Techniques in Mechanics and Engineering讀者反饋
書(shū)目名稱An Introduction to Modern Variational Techniques in Mechanics and Engineering讀者反饋學(xué)科排名
作者: 使腐爛 時(shí)間: 2025-3-22 00:17 作者: OMIT 時(shí)間: 2025-3-22 04:05
Transformation Properties of the Lagrange— D’Alembert Variational Principle: Conservation Laws of Noof conservat ive and purely nonconservative dynamical systems. The basic idea of this approach is to consider the transformation properties of the Lagrange-D’Alembert principle with respect to the infinite simaltransform at ion of the generalized coordinates and time. It is of interest to note that 作者: 骯臟 時(shí)間: 2025-3-22 07:23 作者: Conscientious 時(shí)間: 2025-3-22 09:02
The Hamiltonian Variational Principle and Its Applicationse is based upon the . characteristics of motion; that is, the relations between its scalar and vector characteristics are considered simultaneously in one particular inst ant of time. The problem of describing the global characteristics of motion has been reduced to the integration of differential e作者: 軌道 時(shí)間: 2025-3-22 14:23
Variable End Points, Natural Boundary Conditions, Bolza Problems We shall cons ider in particular the cases in which the initi al or terminal configur at ions (or both) ar e not sp ecified . Also, it may happen that t he time interval in which the evolut iona ry process is t aking place is not given . For these cases the Hamiltonian principle usually produces ch作者: yohimbine 時(shí)間: 2025-3-22 20:35 作者: Spinal-Fusion 時(shí)間: 2025-3-22 23:51
B. D. Vujanovic,T. M. AtanackovicMany examples and novel applications throughout.Competitive literature - Meirovich, Goldstein - is outdated and does not include the synthesis of topics presented here.Will serve a broad audience in a作者: pulse-pressure 時(shí)間: 2025-3-23 02:12 作者: 鬼魂 時(shí)間: 2025-3-23 08:50
Einleitung und Problemstellung,t form that is not connected to any privileged coordinate system. To accomplish this goal we turn first to the Lagrange-D’Alembert differential variational principle, whose applications are very wide and encompass holonomic and nonholonomic dynamical systems and also conservative and purely nonconse作者: Excitotoxin 時(shí)間: 2025-3-23 10:56
https://doi.org/10.1007/978-3-322-83450-8ilton canonical differential equations . UPi oq, where .(. , ...,.,.l, ...,.) is th e Hamiltonian function. In writing (2.1.1) we assumed that the nonconservative (nonpotential) generalized forces are equal to zero : 作者: misshapen 時(shí)間: 2025-3-23 15:29
Die Vernetzung sozialer Einheitenof conservat ive and purely nonconservative dynamical systems. The basic idea of this approach is to consider the transformation properties of the Lagrange-D’Alembert principle with respect to the infinite simaltransform at ion of the generalized coordinates and time. It is of interest to note that 作者: 逃避責(zé)任 時(shí)間: 2025-3-23 19:00
https://doi.org/10.1007/978-3-476-03451-9method for solving the canonical differential equat ions of mot ion. In addition, a variety of approximate methods can be built up , based upo n this method , for solving nonlinear problems for which an exact, complete solu tion of the Hamilton-J acobi nonlinear partial differential equa t ion is no作者: 逃避責(zé)任 時(shí)間: 2025-3-23 23:17
https://doi.org/10.1007/978-3-476-03451-9e is based upon the . characteristics of motion; that is, the relations between its scalar and vector characteristics are considered simultaneously in one particular inst ant of time. The problem of describing the global characteristics of motion has been reduced to the integration of differential e作者: Aqueous-Humor 時(shí)間: 2025-3-24 05:21
https://doi.org/10.1007/978-3-476-03451-9 We shall cons ider in particular the cases in which the initi al or terminal configur at ions (or both) ar e not sp ecified . Also, it may happen that t he time interval in which the evolut iona ry process is t aking place is not given . For these cases the Hamiltonian principle usually produces ch作者: 總 時(shí)間: 2025-3-24 07:09
https://doi.org/10.1007/978-3-663-16065-6r of degrees of freedom of a dynamical system. In this chapter we will consider several import ant situations in which the generalized coordinates are . but are restricted by given auxiliary conditions. Namely, it is not uncommon in th e analysis of applied variational problems to be faced with the 作者: 不足的東西 時(shí)間: 2025-3-24 11:17
https://doi.org/10.1007/978-0-8176-8162-3Optimal control; Transformation; calculus; dynamical systems; ksa; mechanics; optimization; stability作者: 范例 時(shí)間: 2025-3-24 16:03 作者: pulmonary 時(shí)間: 2025-3-24 20:42
https://doi.org/10.1007/978-3-663-16065-6In this section we shall use the results presented so far to formulate several variational principles for t he equations describing deformations and the optimal shape of elastic columns. We shall use the classical (Bernoulli-Euler) rod theory as well as generalized rod theories. The variational principles that we will formulate will be used to作者: vector 時(shí)間: 2025-3-25 01:08
Variational Principles for Elastic Rods and ColumnsIn this section we shall use the results presented so far to formulate several variational principles for t he equations describing deformations and the optimal shape of elastic columns. We shall use the classical (Bernoulli-Euler) rod theory as well as generalized rod theories. The variational principles that we will formulate will be used to作者: 松軟 時(shí)間: 2025-3-25 04:24 作者: 大笑 時(shí)間: 2025-3-25 09:24
https://doi.org/10.1007/978-3-476-03451-9e is based upon the . characteristics of motion; that is, the relations between its scalar and vector characteristics are considered simultaneously in one particular inst ant of time. The problem of describing the global characteristics of motion has been reduced to the integration of differential equations of motion.作者: 浸軟 時(shí)間: 2025-3-25 12:51
The Hamilton-Jacobi Method of Integration of Canonical Equationsilton canonical differential equations . UPi oq, where .(. , ...,.,.l, ...,.) is th e Hamiltonian function. In writing (2.1.1) we assumed that the nonconservative (nonpotential) generalized forces are equal to zero : 作者: 鼓掌 時(shí)間: 2025-3-25 18:15
The Hamiltonian Variational Principle and Its Applicationse is based upon the . characteristics of motion; that is, the relations between its scalar and vector characteristics are considered simultaneously in one particular inst ant of time. The problem of describing the global characteristics of motion has been reduced to the integration of differential equations of motion.作者: 載貨清單 時(shí)間: 2025-3-25 22:49
Textbook 2004 Serbia, and numerous foreign universities. The objective of the authors has been to acquaint the reader with the wide possibilities to apply variational principles in numerous problems of contemporary analytical mechanics, for example, the Noether theory for finding conservation laws of conservativ作者: Ambulatory 時(shí)間: 2025-3-26 02:31
An Introduction to Modern Variational Techniques in Mechanics and Engineering作者: 背信 時(shí)間: 2025-3-26 06:57
An Introduction to Modern Variational Techniques in Mechanics and Engineering978-0-8176-8162-3作者: glacial 時(shí)間: 2025-3-26 08:58 作者: 敵手 時(shí)間: 2025-3-26 14:04 作者: 無(wú)動(dòng)于衷 時(shí)間: 2025-3-26 16:53 作者: obeisance 時(shí)間: 2025-3-26 22:13 作者: ARM 時(shí)間: 2025-3-27 03:36
Transformation Properties of the Lagrange— D’Alembert Variational Principle: Conservation Laws of Nother , which is based upon the transformation properties of the Hamiltonian action integral ∫. Ldu. However , the approach based upon the Lagrange-D’Alembert differential variational principle admits the possibility to include into consideration purely nonconservative dynamical systems for which . ≠0.作者: 護(hù)航艦 時(shí)間: 2025-3-27 07:00 作者: 調(diào)整校對(duì) 時(shí)間: 2025-3-27 10:57 作者: fiscal 時(shí)間: 2025-3-27 15:34
https://doi.org/10.1007/978-3-476-03451-9method , for solving nonlinear problems for which an exact, complete solu tion of the Hamilton-J acobi nonlinear partial differential equa t ion is not available. An exha ust ive review of applica t ions of the Hamilton-Jacobi metho d is pr esented in the monographs of Kevorkian and Kole [60] and Neyfeh [76].作者: 表皮 時(shí)間: 2025-3-27 20:55 作者: sulcus 時(shí)間: 2025-3-27 22:28
The Elements of Analytical Mechanics Expressed Using the Lagrange-D’Alembert Differential Variationaional principle, whose applications are very wide and encompass holonomic and nonholonomic dynamical systems and also conservative and purely nonconservative systems as well. The elements of this part of contemporary analytical mechanics in fact, constitute the content of this chapter.作者: capsule 時(shí)間: 2025-3-28 05:45
A Field Method Suitable for Application in Conservative and Nonconservative Mechanicsmethod , for solving nonlinear problems for which an exact, complete solu tion of the Hamilton-J acobi nonlinear partial differential equa t ion is not available. An exha ust ive review of applica t ions of the Hamilton-Jacobi metho d is pr esented in the monographs of Kevorkian and Kole [60] and Neyfeh [76].作者: 煩人 時(shí)間: 2025-3-28 08:10 作者: 亞當(dāng)心理陰影 時(shí)間: 2025-3-28 11:59
Textbook 2004egral variational principle. These two variational principles form the main subject of contemporary analytical mechanics, and from them the whole colossal corpus of classical dynamics can be deductively derived as a part of physical theory. In recent years students and researchers of engineering and作者: 禍害隱伏 時(shí)間: 2025-3-28 15:39
10樓作者: Concerto 時(shí)間: 2025-3-28 22:30
10樓作者: Tonometry 時(shí)間: 2025-3-28 23:01
10樓作者: 澄清 時(shí)間: 2025-3-29 06:32
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