By Valeri M. Mladenov, Plamen Ch. Ivanov

ISBN-10: 3319086715

ISBN-13: 9783319086712

ISBN-10: 3319086723

ISBN-13: 9783319086729

This e-book constitutes the refereed lawsuits of the twenty second foreign convention on Nonlinear Dynamics of digital structures, NDES 2014, held in Albena, Bulgaria, in July 2014. The forty seven revised complete papers provided have been rigorously reviewed and chosen from sixty five submissions. The papers are equipped in topical sections on nonlinear oscillators, circuits and digital structures; networks and nonlinear dynamics and nonlinear phenomena in organic and physiological systems.

**Read or Download Nonlinear Dynamics of Electronic Systems: 22nd International Conference, NDES 2014, Albena, Bulgaria, July 4-6, 2014. Proceedings PDF**

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**Extra info for Nonlinear Dynamics of Electronic Systems: 22nd International Conference, NDES 2014, Albena, Bulgaria, July 4-6, 2014. Proceedings**

**Example text**

11 Time (b) Normalized data. (a) Original data. Fig. 1. ] (a) Original data. ] (b) Normalized data. Fig. 2. Time series of the environmental sound and its normalized data 3 Time Synchronization Method Using Natural Environmental Fluctuations as the Additive Sequences of Noise-Induced Synchronization In our proposed scheme, we apply natural ﬂuctuations to the nonlinear oscillators as the common noise of noise-induced synchronization phenomenon. As A Study on Performance Improvement of Natural Synchronization Scheme 25 the natural environmental ﬂuctuations, we use temperature or humidity of the air, environmental sounds and so on.

1. Behavior of the waveforms t0+kT A Stability Analysis Method for Period-1 Solution following equation ⎧ ⎪ ⎪ ⎨ x(t) = φ x (t; t0 , x0 , u0 , λ1 ) , ⎪ ⎪ ⎩ u(t) = φ (t; t , x , u , λ ) u 0 0 0 39 for mass-1, (3) for mass-2, (4) 1 ⎧ ⎪ ⎪ ⎨ y(t) = ψy (t; t0 , y0 , v0 , λ2 ) , ⎪ ⎪ ⎩ v(t) = ψv (t; t0 , y0 , v0 , λ2 ) ∈ R4 → R4 , x0 , u0 , y0 , and v0 mean the initial where (φ, ψ) = (φ x , φu ) , ψy , ψv value at t = t0 . Next, we define the local section consists of scalar function q. = (x, y) ∈ R4 : q(x, y, λq ) = 0, q : R4 → R .

3. Circuital implementation of the Lorenz system. 74kΩ, R16 = 100kΩ, R17 = 1kΩ, R18 = 1kΩ, R19 = 9kΩ, C1 = 200nF , C2 = 200nF , C3 = 200nF , Vcc = 9V. ⎧ ⎨ X˙ = α(Y − X) Y˙ = ρX − 30XZ − Y ⎩ ˙ Z = 100XY − βZ 30 (6) ﬁxing a time scaling κ = C11R5 = C21R11 = C3 1R17 = 5000, ρ = 28, and β = 83 . In this case, the bifurcation parameter α is implemented through represented by resistor R5 . The transformer is inserted following the same considerations made for the Chua’s circuit, as reported in Fig. 4 with a primary winding connected to a square pulse wave of amplitude A = 2V and 50% duty cycle.

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