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Investigation of Chaos-Generating Circuit Composed of RL Circuits

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Investigation of Chaos-Generating Circuit Composed of RL Circuits

Yoshinori DOIKE

Yoko UWATE

Yoshifumi NISHIO

and Jingmin XIN

(

Tokushima University) (

Xi’an Jiaotong University)

1. Introduction

Recently, chaos phenomena attract many researchers’

attentions. In the field of electrical and electronic engi- neering, various applications using chaos have been pro- posed. To implement these systems, we have to under- stand chaos phenomena in detail. In this study, simple chaotic circuits using two coupled RL circuits are pro- posed. We observe the generation of interesting chaotic phenomenon.

2. Circuit model

Figure 1 shows the circuit model. In this circuit, two RL circuits are coupled via simple comparators of opera- tional amplifiers. The rectangular voltage wave is inputted to the other input terminals of the comparators and the comparators produce the output voltage ± E which is their power supply voltage according to the input signals. Fig- ure 2(a) shows the rectangular voltage waveform V

S

(t).

is the amplitude of the rectangular voltage and T is the period of the waveform. E is the output voltage of the comparators, namely the DC supply voltage of the opera- tional amplifiers.

+ -

- +

R

R L

L

i

1

v

2

v

1

VS

v

1

i

2

v

2

Figure 1:

Circuit model.

(a) (b)

Figure 2:

Rectangular voltage waveform.

By using the following variables and the parameters, v

n

= Ex

n

, t = RCτ, T =

RL

β, (n = 1, 2)

the normalized circuit equations are given as follows.

x

1

=

 

 

 

(x

10

R

L

+ R

R )e

τ

+ R

L

R (x

2

> V

α

)

(x

10

+ R

L

+ R

R )e

τ

R

L

R (x

2

< V

α

)

x

2

=

 

 

 

(x

20

+ R

L

+ R

R )e

τ

R

L

R (x

1

> V

α

)

(x

20

R

L

+ R

R )e

−τ

+ R

L

R (x

1

< V

α

).

(1)

where V

α

corresponds to V

S

and is shown in Fig. 2(b), x

10

, x

20

are initial values and R

L

is internal resistance of L.

3. Computer calculated results

Figures 3 and 4 show computer calculated results for V

α

= 0.0005, β = 22 R

L

= 17 and R = 1000. We observe chaos phenomenon.

Figure 3: Attractor

x1−x2.

Figure 4: Waveform.

4. Circuit experimental results

Figures 5 and 6 show circuit experiment results for R

1

= 1.003[kΩ], R

2

= 1.005[kΩ], R

L1

= 14.61[kΩ], R

L2

= 14.93[kΩ] and f = 110[kHz], V

S

= 6[V ]. We observe chaos phenomenon.

Figure 5: Attractor

v1−v2.

Figure 6: Waveform.

5. Conclusions

In this study, we have proposed a simple chaotic oscil- lator including two RL circuits. We have confirmed that the circuit generated chaotic oscillation by both computer calculations and circuit experiments.  

14

平成25年度電気関係学会四国支部連合大会 講演論文集 (2013 徳島大学)

2013 SHIKOKU-SECTION JOINT CONVENTION RECORD OF THE INSTITUTES OF ELECTRICAL AND RELATED ENGINEERS (TOKUSHIMA)

1-14

Figure 2: Rectangular voltage waveform.

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