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International Journal of Electrical and Computer Engineering (IJECE)
Vol. 11, No. 1, February 2021, pp. 328~335
ISSN: 2088-8708, DOI: 10.11591/ijece.v11i1.pp328-335  328
Journal homepage: http://ijece.iaescore.com
Application of particle swarm optimization with ANFIS model
for double scroll chaotic system
W. A. Wali
Department of Computer Engineering, College of Engineering, Basrah University, Iraq
Article Info ABSTRACT
Article history:
Received Mar 21, 2020
Revised Jun 22, 2020
Accepted Jul 10, 2020
The predictions for the original chaos patterns can be used to correct
the distorted chaos pattern which has changed due to any changes whether
from undesired disturbance or additional information which can hide under
chaos pattern. This information can be recovered when the original chaos
pattern is predicted. But unpredictability is most features of chaos, and time
series prediction can be used based on the collection of past observations of
a variable and analysis it to obtain the underlying relationships and then
extrapolate future time series. The additional information often prunes away
by several techniques. This paper shows how the chaotic time series
prediction is difficult and distort even if neuro-fuzzy such as adaptive neural
fuzzy inference system (ANFIS) is used under any disturbance. The paper
combined particle swarm (PSO) and (ANFIS) to exam the prediction model
and predict the original chaos patterns which comes from the double
scroll circuit. Changes in the bias of the nonlinear resistor were used as
a disturbance. The predicted chaotic data is compared with data from
the chaotic circuit.
Keywords:
ANFIS
Chaotic time series
PSO
This is an open access article under the CC BY-SA license.
Corresponding Author:
Wasan Wali,
Department of Computer Engineering,
Basrah University,
Basrah, Iraq.
Email: wasan.wali@uobasrah.edu.iq
1. INTRODUCTION
Nonlinear prediction of chaotic time series is very challenging in the prediction area [1]. Neural
networks and related neuro-fuzzy models such as (ANFIS) have been the subjects of interest due to their
many practical applications in modeling complex nonlinear systems [2-4] and in chaotic time series
predictions [5-10] but when the number of observations for training is limited or the data does not have
a similar pattern they can neither reconstruct the dynamics nor learn the shape of attractor and the prediction
become more difficult. In this paper, we used the asymmetrical double scroll attractor as an obstacle for
the best technique which is the ANFIS model to predict the original pattern and propose the odd information
which does not match with the original pattern. This oddness in information can be with purpose or as
distortions. The paper shows how it is difficult and the distortions that happened on the perditions of
chaotic attractor by using the ANFIS model under disturbance. Chaos in electrical circuits has drawn strong
attention [10-15] since the circuit provides a simple vehicle for the experimental observation and computer
simulation of chaotic phenomena. The double scroll circuit is used for nonlinear time series analysis methods
for confirming the chaotic behavior Figure 1 shows the double scroll circuit, circuitry, and nonlinear resistor
characteristic. Figure 2 shows symmetric double spiral attractor.
Int J Elec & Comp Eng ISSN: 2088-8708 
Application of particle swarm optimization with ANFIS model for… (W. A. Wali)
329
Chaotic systems are sensitive dependency on initial conditions and densely distributed periodic
points [16]. The data collected along inevitable noise makes the prediction of a chaotic system hard to
achieve. This difficulty proposes the modelling chaotic time series. Artificial Intelligence techniques have
gained significant importance in modelling because of their ability to learn from historical observations data
and predict highly nonlinear systems. ANFIS is a type of system that incorporates neural and fuzzy logic.
Neurons learn from experience and performed by optimization of the antecedent and conclusion parts
parameters. This paper uses ANFIS to predict a time series generated by a double scroll circuit but using
asymmetrical attractor as kind of the noise via generated asymmetrical data pattern and evaluates the ANFIS
prediction in this case. Figure 3 shows the block diagram of ANFIS prediction.
Figure 1. Double scroll circuit and nonlinear resistor characteristics
Figure 2. Symmetrical double strange attractor
Figure 3. Block diagram of ANFIS prediction
2. ASYMMETRICAL DOUBLE STRANGE ATTRACTOR
Generally, the phenomenon of multiple attractors is mostly in symmetric dynamical systems
[17-18]. These exhibit pairs of mutually symmetric attractors, as a parameter, are varied. The symmetry in
double scroll strange attractor, which was observed from the electronic circuits, may not be held in special
cases for various reasons, for example, switching characteristics of the diodes because of the differences in
bias values or imperfect matching transistors or any other reasons that can make asymmetry in the strange
attractor. Analysis of the nonlinear resistor circuit that is shown in Figure 4 indicates that the break voltage of
the v-i characteristic is bias dependent. This can be related to the switching characteristics of the diodes.
Thus it is expected that the bias sources +Vcc and –Vcc, play a certain role as a bifurcation element. Figure 5
shows the effect of the bias on a double scroll attractor.
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 11, No. 1, February 2021 : 328 - 335
330
Figure 4. Nonlinear resistors
Figure 5. Asymmetrical double strange attractor
The prediction of a chaotic system from noisy observations is very hard. Noisy data could be
contaminated from different types of sources. Noise can be propagated into the prediction model and make
real problems in many of chaos real-life applications. Noise on chaotic time series prediction has been barely
considered [19] to improve the performance prediction in the presence of noise. In this work, we focus on
how to make a change in bias as disturbance data among the original data to examine the prediction of
ANFIS based on chaotic noisy observations. Figure 6 shows the block diagram of the disturbance
prediction system.
Figure 6. Disturbance on a chaotic system
Int J Elec & Comp Eng ISSN: 2088-8708 
Application of particle swarm optimization with ANFIS model for… (W. A. Wali)
331
3. COMBINED PSO WITH ANFIS TO REJECT THE BIAS DISTURBANCE
The idea behind PSO is each particle keeps track of the coordinates in the space of the problem
which is associated with the best solution [20]. Many studies have combined PSO with fuzzy and ANFIS in
different applications [21-25]. In most of them the PSO tries to optimize the ANFIS parameters to give
the best solutions. In our work, the PSO plays an important role in removing any undesired data and
improving the prediction signal. PSO starts by taking the time-series data from the circuit under change as
the initial first swarm generation. The closeness of each particle to the best solution depends on the objective
function. The objective is the chaotic time-series data from the original double scroll circuit without any
disturbance. Figure 7 and Figure 8 show the PSO-ANFIS model block diagram. Figure 9 shows the graphical
representations. Considering the search space of 2-dimension and (n) particles as an initial population was
taken from the circuit after the change of bias. There is a part of these particles that have a wrong position
due to the change. Each particle has a specified position and velocity that is associated with its particular best
performance in the swarm. Each particle tries to modify its position with its objective which is specified from
the chaotic time-series data from the original double scroll circuit
Figure 7. Disturbance on a chaotic system Figure 8. PSO-ANFIS prediction block diagram
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 11, No. 1, February 2021 : 328 - 335
332
Figure 9. PSO graphical representations
4. RESULTS AND ANALYSIS
The simulation was implemented using Matlab and the results arranged as the following:
 Generate the chaotic time-series data from the double scroll circuit (Vc1 and Vc2) which show in
Figure 10.
 Make the change in +Vcc1 in nonlinear resistor which is shown in Figure 1
 Generate more chaotic data from the chaotic circuit after the change.
 Use ANFIS to predict chaotic data. Figure 11 shows the comparison between the simulations data from
the circuit and predications of the ANFIS model. The figure shows the distortions in the attractor
 The distortions because of the additional changed data.
The simulation was implemented using Matlab and the results arranged as the following:
 Generate the chaotic time-series data from the double scroll circuit (Vc1 and Vc2) which show in
Figure 10.
 Make the change in +Vcc1 in nonlinear resistor which is shown in Figure 1
 Generate more chaotic data from the chaotic circuit after the change.
 Use ANFIS to predict chaotic data. Figure 11 shows the comparison between the simulations data from
the circuit and predications of the ANFIS model. The figure shows the distortions in the attractor
 The distortions because of the additional changed data.
 Applied the PSO on the ANFIS model data. Figures 12, 13, and 14 show the ANFIS predictions model
after PSO which applied according to the flowchart in Figure 7.
Int J Elec & Comp Eng ISSN: 2088-8708 
Application of particle swarm optimization with ANFIS model for… (W. A. Wali)
333
 Figure 12 shows the particles update in their positions according to the individual nearest objectives taken
from the circuit without disturbance.
 Figures 13 and 14 show PSO-ANFIS prediction on the attractor.
PSO-ANFIS can be used to predict and separate any kind of hidden pieces of information from any
noisy source signal as shown in Figure 15 and it was tested under incomplete chaotic data which gave a good
estimation hence, we can say it deserved to be under consideration.
Figure 10. Double scroll circuit Figure 11. Double scroll circuit
Figure 12. Particles updated in their positions
according to the individual nearest objectives
Figure 13. PSO-ANFIS prediction
Figure 14. PSO-ANFIS prediction
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 11, No. 1, February 2021 : 328 - 335
334
Figure 15. PSO-ANFIS model used for prediction and sperations
5. CONCLUSION
However, PSO-ANFIS shows the difficultly to predict the original double scroll attractor when it is
distorted, still, it is a good method to recover particles which were absent due to any change and recover
the original pattern. This method also can be used to recover the hidden information under the attractor by
recognizing the odd particles after they were compared with original attractor data.
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Application of particle swarm optimization with ANFIS model for double scroll chaotic system

  • 1. International Journal of Electrical and Computer Engineering (IJECE) Vol. 11, No. 1, February 2021, pp. 328~335 ISSN: 2088-8708, DOI: 10.11591/ijece.v11i1.pp328-335  328 Journal homepage: http://ijece.iaescore.com Application of particle swarm optimization with ANFIS model for double scroll chaotic system W. A. Wali Department of Computer Engineering, College of Engineering, Basrah University, Iraq Article Info ABSTRACT Article history: Received Mar 21, 2020 Revised Jun 22, 2020 Accepted Jul 10, 2020 The predictions for the original chaos patterns can be used to correct the distorted chaos pattern which has changed due to any changes whether from undesired disturbance or additional information which can hide under chaos pattern. This information can be recovered when the original chaos pattern is predicted. But unpredictability is most features of chaos, and time series prediction can be used based on the collection of past observations of a variable and analysis it to obtain the underlying relationships and then extrapolate future time series. The additional information often prunes away by several techniques. This paper shows how the chaotic time series prediction is difficult and distort even if neuro-fuzzy such as adaptive neural fuzzy inference system (ANFIS) is used under any disturbance. The paper combined particle swarm (PSO) and (ANFIS) to exam the prediction model and predict the original chaos patterns which comes from the double scroll circuit. Changes in the bias of the nonlinear resistor were used as a disturbance. The predicted chaotic data is compared with data from the chaotic circuit. Keywords: ANFIS Chaotic time series PSO This is an open access article under the CC BY-SA license. Corresponding Author: Wasan Wali, Department of Computer Engineering, Basrah University, Basrah, Iraq. Email: wasan.wali@uobasrah.edu.iq 1. INTRODUCTION Nonlinear prediction of chaotic time series is very challenging in the prediction area [1]. Neural networks and related neuro-fuzzy models such as (ANFIS) have been the subjects of interest due to their many practical applications in modeling complex nonlinear systems [2-4] and in chaotic time series predictions [5-10] but when the number of observations for training is limited or the data does not have a similar pattern they can neither reconstruct the dynamics nor learn the shape of attractor and the prediction become more difficult. In this paper, we used the asymmetrical double scroll attractor as an obstacle for the best technique which is the ANFIS model to predict the original pattern and propose the odd information which does not match with the original pattern. This oddness in information can be with purpose or as distortions. The paper shows how it is difficult and the distortions that happened on the perditions of chaotic attractor by using the ANFIS model under disturbance. Chaos in electrical circuits has drawn strong attention [10-15] since the circuit provides a simple vehicle for the experimental observation and computer simulation of chaotic phenomena. The double scroll circuit is used for nonlinear time series analysis methods for confirming the chaotic behavior Figure 1 shows the double scroll circuit, circuitry, and nonlinear resistor characteristic. Figure 2 shows symmetric double spiral attractor.
  • 2. Int J Elec & Comp Eng ISSN: 2088-8708  Application of particle swarm optimization with ANFIS model for… (W. A. Wali) 329 Chaotic systems are sensitive dependency on initial conditions and densely distributed periodic points [16]. The data collected along inevitable noise makes the prediction of a chaotic system hard to achieve. This difficulty proposes the modelling chaotic time series. Artificial Intelligence techniques have gained significant importance in modelling because of their ability to learn from historical observations data and predict highly nonlinear systems. ANFIS is a type of system that incorporates neural and fuzzy logic. Neurons learn from experience and performed by optimization of the antecedent and conclusion parts parameters. This paper uses ANFIS to predict a time series generated by a double scroll circuit but using asymmetrical attractor as kind of the noise via generated asymmetrical data pattern and evaluates the ANFIS prediction in this case. Figure 3 shows the block diagram of ANFIS prediction. Figure 1. Double scroll circuit and nonlinear resistor characteristics Figure 2. Symmetrical double strange attractor Figure 3. Block diagram of ANFIS prediction 2. ASYMMETRICAL DOUBLE STRANGE ATTRACTOR Generally, the phenomenon of multiple attractors is mostly in symmetric dynamical systems [17-18]. These exhibit pairs of mutually symmetric attractors, as a parameter, are varied. The symmetry in double scroll strange attractor, which was observed from the electronic circuits, may not be held in special cases for various reasons, for example, switching characteristics of the diodes because of the differences in bias values or imperfect matching transistors or any other reasons that can make asymmetry in the strange attractor. Analysis of the nonlinear resistor circuit that is shown in Figure 4 indicates that the break voltage of the v-i characteristic is bias dependent. This can be related to the switching characteristics of the diodes. Thus it is expected that the bias sources +Vcc and –Vcc, play a certain role as a bifurcation element. Figure 5 shows the effect of the bias on a double scroll attractor.
  • 3.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 11, No. 1, February 2021 : 328 - 335 330 Figure 4. Nonlinear resistors Figure 5. Asymmetrical double strange attractor The prediction of a chaotic system from noisy observations is very hard. Noisy data could be contaminated from different types of sources. Noise can be propagated into the prediction model and make real problems in many of chaos real-life applications. Noise on chaotic time series prediction has been barely considered [19] to improve the performance prediction in the presence of noise. In this work, we focus on how to make a change in bias as disturbance data among the original data to examine the prediction of ANFIS based on chaotic noisy observations. Figure 6 shows the block diagram of the disturbance prediction system. Figure 6. Disturbance on a chaotic system
  • 4. Int J Elec & Comp Eng ISSN: 2088-8708  Application of particle swarm optimization with ANFIS model for… (W. A. Wali) 331 3. COMBINED PSO WITH ANFIS TO REJECT THE BIAS DISTURBANCE The idea behind PSO is each particle keeps track of the coordinates in the space of the problem which is associated with the best solution [20]. Many studies have combined PSO with fuzzy and ANFIS in different applications [21-25]. In most of them the PSO tries to optimize the ANFIS parameters to give the best solutions. In our work, the PSO plays an important role in removing any undesired data and improving the prediction signal. PSO starts by taking the time-series data from the circuit under change as the initial first swarm generation. The closeness of each particle to the best solution depends on the objective function. The objective is the chaotic time-series data from the original double scroll circuit without any disturbance. Figure 7 and Figure 8 show the PSO-ANFIS model block diagram. Figure 9 shows the graphical representations. Considering the search space of 2-dimension and (n) particles as an initial population was taken from the circuit after the change of bias. There is a part of these particles that have a wrong position due to the change. Each particle has a specified position and velocity that is associated with its particular best performance in the swarm. Each particle tries to modify its position with its objective which is specified from the chaotic time-series data from the original double scroll circuit Figure 7. Disturbance on a chaotic system Figure 8. PSO-ANFIS prediction block diagram
  • 5.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 11, No. 1, February 2021 : 328 - 335 332 Figure 9. PSO graphical representations 4. RESULTS AND ANALYSIS The simulation was implemented using Matlab and the results arranged as the following:  Generate the chaotic time-series data from the double scroll circuit (Vc1 and Vc2) which show in Figure 10.  Make the change in +Vcc1 in nonlinear resistor which is shown in Figure 1  Generate more chaotic data from the chaotic circuit after the change.  Use ANFIS to predict chaotic data. Figure 11 shows the comparison between the simulations data from the circuit and predications of the ANFIS model. The figure shows the distortions in the attractor  The distortions because of the additional changed data. The simulation was implemented using Matlab and the results arranged as the following:  Generate the chaotic time-series data from the double scroll circuit (Vc1 and Vc2) which show in Figure 10.  Make the change in +Vcc1 in nonlinear resistor which is shown in Figure 1  Generate more chaotic data from the chaotic circuit after the change.  Use ANFIS to predict chaotic data. Figure 11 shows the comparison between the simulations data from the circuit and predications of the ANFIS model. The figure shows the distortions in the attractor  The distortions because of the additional changed data.  Applied the PSO on the ANFIS model data. Figures 12, 13, and 14 show the ANFIS predictions model after PSO which applied according to the flowchart in Figure 7.
  • 6. Int J Elec & Comp Eng ISSN: 2088-8708  Application of particle swarm optimization with ANFIS model for… (W. A. Wali) 333  Figure 12 shows the particles update in their positions according to the individual nearest objectives taken from the circuit without disturbance.  Figures 13 and 14 show PSO-ANFIS prediction on the attractor. PSO-ANFIS can be used to predict and separate any kind of hidden pieces of information from any noisy source signal as shown in Figure 15 and it was tested under incomplete chaotic data which gave a good estimation hence, we can say it deserved to be under consideration. Figure 10. Double scroll circuit Figure 11. Double scroll circuit Figure 12. Particles updated in their positions according to the individual nearest objectives Figure 13. PSO-ANFIS prediction Figure 14. PSO-ANFIS prediction
  • 7.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 11, No. 1, February 2021 : 328 - 335 334 Figure 15. PSO-ANFIS model used for prediction and sperations 5. CONCLUSION However, PSO-ANFIS shows the difficultly to predict the original double scroll attractor when it is distorted, still, it is a good method to recover particles which were absent due to any change and recover the original pattern. This method also can be used to recover the hidden information under the attractor by recognizing the odd particles after they were compared with original attractor data. REFERENCES [1] J. SIDorowich, "Modeling of chaotic time series for prediction, interpolation, and smoothing," IEEE International Conference on Acoustics, Speech, and Signal Processing, vol. 4, pp. 121-124, 1992. [2] F. Prado, et al., "Forecasting based on an ensemble Autoregressive Moving Average-Adaptive neuro-Fuzzy inference system-Neural network - Genetic Algorithm Framework," Energy, vol. 197, pp. 117-159, 2020. [3] S. Kar, et al., "Applications of neuro fuzzy systems: A brief review and future outline," Applied Soft Computing, vol. 15, pp. 243-259, 2014, [4] M. Malekizadeh, et al., "Short-term load forecast using ensemble neuro-fuzzy model," Energy, vol. 196, pp. 117-127, 2020. [5] S. Ganjefar, “Optimization of quantum-inspired neural network using memetic algorithm for function approximation and chaotic time series prediction," Neurocomputing, vol. 291, pp. 175-186, 2018. [6] H. Rad, et al., "Prediction of rock mass rating system based on continuous functions using Chaos–ANFIS model," International Journal of Rock Mechanics and Mining Sciences, vol. 73, pp. 1-9, 2015. [7] M. Abdollahzade, et al., "A new hybrid enhanced local linear neuro-fuzzy model based on the optimized singular spectrum analysis and its application for nonlinear and chaotic time series forecasting," Information Sciences, vol. 295, pp. 107-125, 2015. [8] Y.Bodyanskiy, et al., “Hybrid adaptive wavelet-neuro-fuzzy system for chaotic time series identification," Information Sciences, vol. 220, pp. 170-179, 2013. [9] A. Pano-Azucena, et al., "Prediction of chaotic time series by using ANNs, ANFIS and SVMs," 7th International Conference on Modern Circuits and Systems Technologies, pp. 1-4, 2018. [10] M. Nhabangue,et al., "Chaotic time series prediction with functional link extreme learning ANFIS (FL-ELANFIS)," International Conference on Power, Instrumentation, Control and Computing, pp. 1-6, 2018. [11] A. Davies, W. Schwarz, "Nonlinear Dynamics of Electronic Systems," Proceedings Of The Workshop Ndes World Scientific, 1993. [12] W. Marszalek, el al., "2D Bifurcations and Chaos in Nonlinear Circuits: a Parallel Computational Approach," 15th International Conference on Synthesis, Modeling, Analysis and Simulation Methods and Applications to Circuit Design (SMACD), pp. 1-300, 2018. [13] B. Samardzic, et al., "Analysis of spatial chaos appearance in cascade connected nonlinear electrical circuits," Chaos, Solitons & Fractals, vol. 95, pp. 14-20, 2017. [14] C. Wang, et al, "Capturing and shunting energy in chaotic Chua circuit,” Chaos, Solitons & Fractals, vol. 134, 2020. [15] G. Leutcho, et al., "Dynamical analysis of a novel autonomous 4-D hyperjerk circuit with hyperbolic sine nonlinearity: Chaos, antimonotonicity and a plethora of coexisting attractors," Chaos, Solitons & Fractals, vol. 107, pp. 67-87, 2018.
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