標題: Titlebook: Analysis and Simulation of Chaotic Systems; Frank C. Hoppensteadt Textbook 2000Latest edition Springer Science+Business Media New York 200 [打印本頁] 作者: 監(jiān)管 時間: 2025-3-21 18:55
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書目名稱Analysis and Simulation of Chaotic Systems讀者反饋
書目名稱Analysis and Simulation of Chaotic Systems讀者反饋學科排名
作者: 注入 時間: 2025-3-21 22:36
Iterations and Perturbations,stion is: Under what conditions will a periodic solution result? The answers for externally forced systems are quite different from those for feedback systems that are found in Sections 3.5, 7.4, 7.5, and 8.4.作者: 舞蹈編排 時間: 2025-3-22 02:10
Quasistatic-State Approximations,nents can try to reach some equilibrium, while the other components change hardly at all. It is not surprising that such perturbation problems can be studied using stability methods, because both deal with how solutions approach equilibria. These problems differ from those in Chapter 7, where oscill作者: GORGE 時間: 2025-3-22 06:42 作者: 厚顏無恥 時間: 2025-3-22 11:37 作者: critique 時間: 2025-3-22 13:31
,Simulation of Designs – Modelsim Tool,a: First, when ε = 0, the solution is ., and so on. This is a . [0, T], and the error estimate .(ε. holds as ε → 0 uniformly for 0 ≤ . ≤ .. However, since the solution .(.) approaches . as . → ∞, we cannot expect Taylor’s formula to be valid uniformly for 0 ≤ . < ∞.作者: 攤位 時間: 2025-3-22 18:57
,Synthesis of Designs – Synplify Tool,studied using stability methods, because both deal with how solutions approach equilibria. These problems differ from those in Chapter 7, where oscillations occurred on a fast time scale relative to other changes. In this chapter we study problems that try to equilibrate on a fast time scale while other components in the system change more slowly作者: 大都市 時間: 2025-3-22 23:05 作者: 很是迷惑 時間: 2025-3-23 04:26 作者: obviate 時間: 2025-3-23 09:29
Applied Mathematical Scienceshttp://image.papertrans.cn/a/image/156258.jpg作者: 鉤針織物 時間: 2025-3-23 12:05 作者: 嚴重傷害 時間: 2025-3-23 17:33
Introduction to Digital VLSI Systems Design,This chapter contains material intended to provide the reader with some background in topics of dynamical systems that are used later. There is a large literature on each topic in this chapter, and the presentation here provides only an overview of topics relevant to the remainder of the book作者: chance 時間: 2025-3-23 19:01 作者: 彎彎曲曲 時間: 2025-3-24 01:30
Writing a Test Bench for the Design,It is often possible to reduce stability and oscillation problems for differential equations to problems for systems of algebraic or operator equations, which can be studied using implicit function theorems and fixed point-methods.作者: avarice 時間: 2025-3-24 04:45 作者: garrulous 時間: 2025-3-24 09:44
Linear Systems,A linear system of ordinary differential equations has the form . Given an .-dimensional vector . and an . × . matrix .(.) of functions of ., we seek a solution vector .(.). We write ., . ∈ . and . ∈ . and sometimes . = ./. or 作者: 改正 時間: 2025-3-24 10:58 作者: 桶去微染 時間: 2025-3-24 18:24
Stability Methods for Nonlinear Systems,A mechanical or an electrical device can be fabricated to a level of accuracy that is restricted by technical or economic constraints.What happens to the output if the construction is a little off specifications? Does output remain near design values? How sensitive is the design to variations in fabrication parameters?作者: 保留 時間: 2025-3-24 21:10
Bifurcation and Topological Methods,It is often possible to reduce stability and oscillation problems for differential equations to problems for systems of algebraic or operator equations, which can be studied using implicit function theorems and fixed point-methods.作者: 侵害 時間: 2025-3-24 23:14
Methods of Averaging,Regular perturbation methods are based on Taylor’s formula and on implicit function theorems. However, there are many problems to which Taylor’s formula cannot be applied directly. In these cases perturbation methods based on multiple time or space scales can often be used, sometimes even for chaotic systems作者: pulmonary-edema 時間: 2025-3-25 06:07
,Simulation of Designs – Modelsim Tool,lution . = 0 is stable under persistent disturbances, but not exponentially asymptotically stable. A solution can be constructed using Taylor’s formula: First, when ε = 0, the solution is ., and so on. This is a . [0, T], and the error estimate .(ε. holds as ε → 0 uniformly for 0 ≤ . ≤ .. However, s作者: 關心 時間: 2025-3-25 09:00
,Synthesis of Designs – Synplify Tool,stion is: Under what conditions will a periodic solution result? The answers for externally forced systems are quite different from those for feedback systems that are found in Sections 3.5, 7.4, 7.5, and 8.4.作者: PATRI 時間: 2025-3-25 15:37
,Synthesis of Designs – Synplify Tool,nents can try to reach some equilibrium, while the other components change hardly at all. It is not surprising that such perturbation problems can be studied using stability methods, because both deal with how solutions approach equilibria. These problems differ from those in Chapter 7, where oscill作者: Cardiac-Output 時間: 2025-3-25 18:33 作者: Eructation 時間: 2025-3-25 22:19
,Synthesis of Designs – Synplify Tool,stion is: Under what conditions will a periodic solution result? The answers for externally forced systems are quite different from those for feedback systems that are found in Sections 3.5, 7.4, 7.5, and 8.4.作者: Exclaim 時間: 2025-3-26 02:17 作者: 有害處 時間: 2025-3-26 04:59
https://doi.org/10.1007/b98824Chaotic Systems; Implicit function; Mathematical Models; Nonlinear system; bifurcation; calculus; computer作者: Synapse 時間: 2025-3-26 08:59
978-1-4757-7386-6Springer Science+Business Media New York 2000作者: Chagrin 時間: 2025-3-26 15:40
Textbook 2000Latest editiondinary and partial differential equations are developed throughout the book. For the second edition, the author has restructured the chapters, placing special emphasis on introductory materials in Chapters 1 and 2 as distinct from presentation materials in Chapters 3 through 8. In addition, more mat作者: BUMP 時間: 2025-3-26 19:30 作者: 弄臟 時間: 2025-3-26 22:37
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