標(biāo)題: Titlebook: Dissipative Structures and Chaos; Hazime Mori,Yoshiki Kuramoto Textbook 1998 Springer-Verlag Berlin Heidelberg 1998 Chaos.Chaotic Attracto [打印本頁] 作者: CT951 時(shí)間: 2025-3-21 16:54
書目名稱Dissipative Structures and Chaos影響因子(影響力)
書目名稱Dissipative Structures and Chaos影響因子(影響力)學(xué)科排名
書目名稱Dissipative Structures and Chaos網(wǎng)絡(luò)公開度
書目名稱Dissipative Structures and Chaos網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱Dissipative Structures and Chaos被引頻次
書目名稱Dissipative Structures and Chaos被引頻次學(xué)科排名
書目名稱Dissipative Structures and Chaos年度引用
書目名稱Dissipative Structures and Chaos年度引用學(xué)科排名
書目名稱Dissipative Structures and Chaos讀者反饋
書目名稱Dissipative Structures and Chaos讀者反饋學(xué)科排名
作者: 石墨 時(shí)間: 2025-3-21 20:57
The Early Life of Ronald Harold Coaserocedure, we derived the Newell-Whitehead (NW) equation using phenomenological considerations. In this chapter, we investigate how different types of amplitude equations are derived to describe a variety of physical conditions. We then study the properties of these equations.作者: squander 時(shí)間: 2025-3-22 03:13 作者: IOTA 時(shí)間: 2025-3-22 08:02
The Later Years of Merton Millerhat follows, we consider a relatively simple example forming the subject of a great deal of present study, that of a collection of limit cycles oscillators, and basing our investigation on the method of phase dynamics, we discuss the fundamental points regarding synchronization phenomena.作者: 津貼 時(shí)間: 2025-3-22 09:26
Introduction themselves. Following this line of reasoning, questions regarding the microscopic physical source of dissipative phenomena can be separated from the study of dissipative phenomena themselves. Such microscopic considerations are beyond the scope of this book.作者: Concomitant 時(shí)間: 2025-3-22 15:51 作者: Concomitant 時(shí)間: 2025-3-22 17:25 作者: carotenoids 時(shí)間: 2025-3-22 23:48 作者: verdict 時(shí)間: 2025-3-23 01:43
Lara Behrens,Christoph Moss,Mona Sadrowskiiodic orbits that determine the form and structure of the chaotic behavior exhibited by any given system. In this chapter we consider the problem of identifying the descriptive signature of such a set of orbits, and we establish the point of view from which we will elucidate the nature of chaos.作者: Obstreperous 時(shí)間: 2025-3-23 08:05
https://doi.org/10.1007/978-1-4615-4619-1n question and the values of the various parameters characterizing it. For a nonequilibrium open system, as the values of such parameters are changed, the qualitative nature of the system’s behavior is seen to assume many forms, as it experiences the emergence, development and bifurcation of chaos.作者: Recess 時(shí)間: 2025-3-23 10:21 作者: 主動(dòng) 時(shí)間: 2025-3-23 15:44 作者: 打火石 時(shí)間: 2025-3-23 19:30
The Statistical Physics of Aperiodic Motiony structure of unstable manifolds can be directly understood in terms of the spectrum .(.), and also that a fixed relationship exists between the spectra of this expansion rate and the local dimension.作者: 隨意 時(shí)間: 2025-3-24 00:11 作者: opinionated 時(shí)間: 2025-3-24 05:19
A Physical Approach to Chaosiodic orbits that determine the form and structure of the chaotic behavior exhibited by any given system. In this chapter we consider the problem of identifying the descriptive signature of such a set of orbits, and we establish the point of view from which we will elucidate the nature of chaos.作者: 無畏 時(shí)間: 2025-3-24 08:31 作者: 一夫一妻制 時(shí)間: 2025-3-24 12:23 作者: Stable-Angina 時(shí)間: 2025-3-24 15:09 作者: Nausea 時(shí)間: 2025-3-24 19:18
Introduction to Part III: What Is a Leader? and in many cases it appears on a macroscopic scale. For this reason, the most natural theoretical description of these phenomena should begin with a consideration of macro-level, nonlinear evolution equations such as the Navier-Stokes equation. Each chapter in Part I is based on this consideration作者: 詼諧 時(shí)間: 2025-3-25 01:20 作者: instate 時(shí)間: 2025-3-25 06:04
The Early Life of Ronald Harold Coasetem in question can be reduced to a relatively simple form we refer to as an amplitude equation. Then, as a representative example of this reduction procedure, we derived the Newell-Whitehead (NW) equation using phenomenological considerations. In this chapter, we investigate how different types of 作者: 大吃大喝 時(shí)間: 2025-3-25 08:26 作者: AFFIX 時(shí)間: 2025-3-25 13:30
https://doi.org/10.1057/9781137341280 the statement, “Slow degrees of freedom govern the dynamics of the system,” was extremely effective. In Chap. 2, the weakly unstable mode in the neighborhood of the bifurcation point served as the slow degree of freedom, while in Chap. 3 this was the concentration of the inhibiting substance presen作者: 虛弱的神經(jīng) 時(shí)間: 2025-3-25 16:25 作者: 天文臺(tái) 時(shí)間: 2025-3-25 23:12 作者: OVERT 時(shí)間: 2025-3-26 01:50
Lara Behrens,Christoph Moss,Mona Sadrowskind unpredictable solutions - chaotic orbits - come to be widely understood as universal phenomena in nonlinear dynamical systems. As we understand it now, chaos can be thought of as the main cause of the diversity that we see displayed in Nature’s perpetually changing panorama.作者: 賞心悅目 時(shí)間: 2025-3-26 08:04 作者: Parabola 時(shí)間: 2025-3-26 12:12
https://doi.org/10.1007/978-1-4615-4619-1 of a bifurcation parameter can cause various saddle points to enter and leave attractors. Chaotic bifurcations result from the collision of an attractor with such points and their resultant inclusion into the attractor.作者: ungainly 時(shí)間: 2025-3-26 13:43 作者: 用肘 時(shí)間: 2025-3-26 17:21
https://doi.org/10.1007/978-1-4615-4619-1eat variety of chaotic phenomena that we observe results from the limitless variation in the types of invariant sets contained by the systems we encounter. The nature of the invariant sets that appear in any given system and the resulting behavior that it exhibits depend both on the type of system i作者: Estrogen 時(shí)間: 2025-3-27 01:02
On Social Goods and Social Bads ‘islands around islands’ self-similar hierarchical structure. Chaotic orbits are often trapped for long times within such structure, and as a result the longtime correlation . appears. In this situation, for . > 0 the probability distribution of mixing P(.;.) obeys the anomalous scaling relation .(作者: intuition 時(shí)間: 2025-3-27 02:17 作者: 拍下盜公款 時(shí)間: 2025-3-27 07:03 作者: adequate-intake 時(shí)間: 2025-3-27 13:15 作者: atopic-rhinitis 時(shí)間: 2025-3-27 14:15
On the Rationale of the Corporate Systemom synchronous to asynchronous motion in a system of two coupled chaotic oscillators. With the elucidation of the geometric structure of this intermittent chaos due to Platt et al. (1993) and Ott and Sommerer (1994), the importance of this type of system has come to be recognized.作者: troponins 時(shí)間: 2025-3-27 21:22
Introductionnd unpredictable solutions - chaotic orbits - come to be widely understood as universal phenomena in nonlinear dynamical systems. As we understand it now, chaos can be thought of as the main cause of the diversity that we see displayed in Nature’s perpetually changing panorama.作者: CAGE 時(shí)間: 2025-3-28 01:25 作者: 陶醉 時(shí)間: 2025-3-28 02:46
On the Structure of Chaosom synchronous to asynchronous motion in a system of two coupled chaotic oscillators. With the elucidation of the geometric structure of this intermittent chaos due to Platt et al. (1993) and Ott and Sommerer (1994), the importance of this type of system has come to be recognized.作者: 階層 時(shí)間: 2025-3-28 10:17
https://doi.org/10.1007/978-3-642-80376-5Chaos; Chaotic Attractors; Dissipative Structures; Energy Dissipation; Geometric and Statistic Descripti作者: membrane 時(shí)間: 2025-3-28 11:02
978-3-642-80378-9Springer-Verlag Berlin Heidelberg 1998作者: cartilage 時(shí)間: 2025-3-28 16:43 作者: Immortal 時(shí)間: 2025-3-28 21:51
A Representative Example of Dissipative Structureture of the governing laws, there are various external factors whose combined influence causes the behavior to become even more complex. For this reason, it is very important in an attempt to understand dissipative behavior that we carefully select a few model examples from the multitude and concent作者: 可用 時(shí)間: 2025-3-29 00:01 作者: RAGE 時(shí)間: 2025-3-29 05:48
Reaction—Diffusion Systems and Interface Dynamicss based on amplitude equations are in general not suited to describe patterns peculiar to such ‘excitable’ systems because, while excitability originates in a particular property of global flow in phase space, amplitude equations are obtained by considering only local flow. In fact, BZ reaction syst作者: 高度贊揚(yáng) 時(shí)間: 2025-3-29 09:45
Phase Dynamics the statement, “Slow degrees of freedom govern the dynamics of the system,” was extremely effective. In Chap. 2, the weakly unstable mode in the neighborhood of the bifurcation point served as the slow degree of freedom, while in Chap. 3 this was the concentration of the inhibiting substance presen作者: 修飾語 時(shí)間: 2025-3-29 11:42
Foundations of Reduction Theory derived phenomenologically. In the present chapter, we consider the theoretical foundation of perhaps the most important types of model equations considered in Part I, amplitude equations and phase equations. The degrees of freedom contained in the corresponding reduced equations are generally char作者: Calibrate 時(shí)間: 2025-3-29 15:35
Dynamics of Coupled Oscillator Systemsous media. In the present chapter we consider another important class of dissipative systems consisting of a large number of degrees of freedom, those composed of aggregates of isolated elements. A neural network consisting of intricately coupled excitable oscillators (neurons) is one example of suc作者: 有其法作用 時(shí)間: 2025-3-29 19:55
Introductionnd unpredictable solutions - chaotic orbits - come to be widely understood as universal phenomena in nonlinear dynamical systems. As we understand it now, chaos can be thought of as the main cause of the diversity that we see displayed in Nature’s perpetually changing panorama.作者: hemophilia 時(shí)間: 2025-3-30 00:58
A Physical Approach to Chaos Almost any nonequilibrium open system will, when some bifurcation parameter characterizing the system is made sufficiently large, display chaotic behavior. It can be said that chaos is Nature’s universal dynamical form. Chaos is characterized by the coexistence of an infinite number of unstable per作者: synovial-joint 時(shí)間: 2025-3-30 08:03
Bifurcation Phenomena of Dissipative Dynamical Systems of a bifurcation parameter can cause various saddle points to enter and leave attractors. Chaotic bifurcations result from the collision of an attractor with such points and their resultant inclusion into the attractor.作者: 鋼筆尖 時(shí)間: 2025-3-30 11:30
The Statistical Physics of Aperiodic Motionine the form and structure of chaos? By introducing the expansion rate of neighboring orbits, which expresses the stretching and folding of segments of .., and the local dimension, which describes the self-similarity of the nested structure of strange attractors, the geometric and statistical descri作者: GONG 時(shí)間: 2025-3-30 12:55 作者: Munificent 時(shí)間: 2025-3-30 17:16
