Titlebook: Deterministic Nonlinear Systems; A Short Course Vadim S. Anishchenko,Tatyana E. Vadivasova,Galina Textbook 2014 Springer International Pub

烈酒

書(shū)目名稱Deterministic Nonlinear Systems影響因子(影響力)




書(shū)目名稱Deterministic Nonlinear Systems影響因子(影響力)學(xué)科排名




書(shū)目名稱Deterministic Nonlinear Systems網(wǎng)絡(luò)公開(kāi)度




書(shū)目名稱Deterministic Nonlinear Systems網(wǎng)絡(luò)公開(kāi)度學(xué)科排名




書(shū)目名稱Deterministic Nonlinear Systems被引頻次




書(shū)目名稱Deterministic Nonlinear Systems被引頻次學(xué)科排名




書(shū)目名稱Deterministic Nonlinear Systems年度引用




書(shū)目名稱Deterministic Nonlinear Systems年度引用學(xué)科排名




書(shū)目名稱Deterministic Nonlinear Systems讀者反饋




書(shū)目名稱Deterministic Nonlinear Systems讀者反饋學(xué)科排名

放縱

Accord

野蠻

,Systems with Phase Space Dimension , ≥ 3: Deterministic Chaos,uilibrium states and limit cycles increases significantly, and many of them have not yet been studied. Some saddle sets become possible, such as an equilibrium state of the saddle-focus type and a saddle limit cycle. A cycle of the saddle-focus type and a saddle torus can be realized in a phase spac

思想上升

From Order to Chaos: Bifurcation Scenarios (Part I),ce of nonlinearity increases, the dynamical regime becomes more complicated. Simple attractors in the phase space of a dissipative system are replaced by more complicated ones. Under certain conditions, nonlinearity can lead to the onset of dynamical chaos. Moving along a relevant direction in the p

inspired

inspired

Robust and Nonrobust Dynamical Systems: Classification of Attractor Types,yagin systems on the plane, there appears a class of robust systems with nontrivial hyperbolicity, i.e., systems with chaotic dynamics. Chaotic attractors of robust hyperbolic systems are, in the rigorous mathematical sense, strange attractors. They usually represent some mathematical idealization a

氣候

dithiolethione

HEED

Quasiperiodic Oscillator with Two Independent Frequencies,ct that they include two or more independent frequencies in the oscillation spectrum: . where ..(.) = ..., . = 1, 2, ., .. As a result, .(.) in (12.1) is 2.-periodic in each argument ..(.), but the quasiperiodic process itself is, in the general case, non-periodic, i.e., .(.) ≠ .(. + ..).