• 検索結果がありません。

Synchronization Phenomena and Circuit Experiment of Star-Coupled van der Pol Oscillators with Additional Oscillators

N/A
N/A
Protected

Academic year: 2021

シェア "Synchronization Phenomena and Circuit Experiment of Star-Coupled van der Pol Oscillators with Additional Oscillators"

Copied!
1
0
0

読み込み中.... (全文を見る)

全文

(1)

Synchronization Phenomena and Circuit Experiment of Star-Coupled van der Pol Oscillators with Additional Oscillators

Minh Hai TRAN Yoko UWATE Yoshifumi NISHIO

Tokushima University

1 Introduction

In our previous study, we investigated synchroniza- tion phenomena observed by adding different frequency van der Pol oscillators coupled with star combination.

By computer simulations, we confirmed some of oscil- lators in the system were synchronized at anti-phase.

In this study, we carry out circuit experiments with 4 van der Pol oscillators system. In addition, we exam- ine in detail 4 van der Pol oscillators and 5 van der Pol oscillators.

2 Circuit Model

The circuit model used in the first pattern is shown in Fig. 1. Three van der Pol oscillators are connected as the star combination. In addition, we add a differ- ent frequency oscillator to the star-coupled van der Pol oscillators. We change the frequency of the 4th oscil- lator and investigate the influence of the 4th oscillator to the overall star circuit.

i R1 C v 1

v 2

v 3

v v 4

i R3 i R4

i R2

v R 1 R

2L

2L 2L

2L 2L 2L 2L 2L

(4) (2)

(1) (3)

I 4A I 4B I 3B

I 2A

I 1A

I 2B

C C

0

I 3A

C n: number of oscillator. (n: 1-4)

Fig. 1 Circuit model.

Three van der Pol oscillators are connected as the star combination. In addition, we add a different fre- quency oscillator to the star-coupled van der Pol oscil- lators. We change the frequency of the 4th oscillator and investigate the influence of the 4th oscillator to the overall star circuit.

3 Simulation Result

The amplitudes of the oscillator are shown in the Figs. 2. In Fig. 2, when the ω increase from 1 to 1.2, the amplitudes of the 3rd and the 4th oscillator become gradually smaller. Next, when the ω is increased to 1.4, the amplitudes of the 3rd and the 4th oscillator are perfect stop. When ω above 1.4, the amplitudes of the 4th oscillator go on increasing. However, the

amplitudes of the 3rd oscillator are almost unchanged.

Fig. 2 Amplitude of oscillator 3 and oscillator 4.

We build a real circuit as Fig. 4 to confirm the results above. The frequency ω is changed by altering the tunnel diode of the fourth oscillator. Figure 4 shows one of my obtained circuit experimental results.

x 1

x

2

x 3

x 4

Fig. 3 Simulation result.

Fig. 4 Circuit experimental result.

In Fig. 4, circuit experimental result also fit theoret- ical analysis results with computer calculations. The 3th oscillators stop.

4 Conclusion

We have investigated synchronization phenomena and oscillation of five oscillators with different frequen- cies. By carrying out computer simulations and circuit experiments, we have confirmed that oscillation of the 3th oscillators are death by increasing ω.

平成

29

年度電気関係学会四国支部連合大会 講演論文集

(2017

愛媛大学)

2017 SHIKOKU-SECTION JOINT CONVENTION RECORD OF THE INSTITUTES OF ELECTRICAL AND RELATED ENGINEERS (EHIME)

1-20

20

Fig. 2 Amplitude of oscillator 3 and oscillator 4.

参照

関連したドキュメント

Therefore, motivated by the impact of topological structures and the delays on the dynamics of the networks, this paper mainly focuses on the effect of delays on inner

Coupled singular parabolic systems with memory: Inspired by the results in [2, 26, 40], it would be quite interesting to consider the null controllability of coupled system of

The evolution of chaotic behavior regions of the oscillators with hysteresis is presented in various control parameter spaces: in the damping coefficient—amplitude and

Ntouyas; Existence results for a coupled system of Caputo type sequen- tial fractional differential equations with nonlocal integral boundary conditions, Appl.. Alsaedi; On a

We show how known nonconstructive lower bound proofs based on the Lov´ asz Local Lemma can be made randomized-constructive using the recent algorithms of Moser and Tardos.. We also

A Melnikov analysis of single-degree-of-freedom (DOF) oscillators is performed by tak- ing into account the first (classical) and higher-order Melnikov functions, by

In this paper, we study the existence and nonexistence of positive solutions of an elliptic system involving critical Sobolev exponent perturbed by a weakly coupled term..

The commutative case is treated in chapter I, where we recall the notions of a privileged exponent of a polynomial or a power series with respect to a convenient ordering,