Optik 127 (2016) 9532–9537
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Optik
j o ur nal ho me pa ge: www.elsevier.de/ijleo
Short note
Predictive synchronization of chaotic and hyperchaotic
energy resource systems
Imen Benchabane, Abdelkrim Boukabou
∗
Department of Electronics, Jijel University, Ouled Aissa, Jijel 18000, Algeria
a r t i c l e i n f o
Article history:
Received 10 March 2016
Accepted 3 May 2016
Keywords:
Energy resource system
Chaotic and hyperchaotic behaviors
Predictive synchronization
a b s t r a c t
The problem of chaos synchronization for energy resource system is investigated. In this
paper, a simple stability criterium for both chaotic and hyperchaotic energy resource sys-
tems is obtained. A unified prediction-based control strategy is designed to make these
systems synchronized. Numerical simulations verify the effectiveness of our methodology.
© 2016 Published by Elsevier GmbH.
1. Introduction
Synchronization of real world chaos-based systems has become a new and important area of research [1]. Since the idea
of synchronizing chaotic systems has been introduced by Pecora and Carroll in 1990 [2], many authors developed different
methods to solve this problem. More recently, predictive synchronization of chaotic satellite systems and hyperchaotic
systems were investigated in [3,4].
Sun et al. [5,6] proposed new chaotic and hyperchaotic systems to analyze the energy resource demand-supply in some
regions of China. Synchronization has been achieved using adaptive control [7] and linear control [8,9].
The aim of this paper is to apply prediction-based control to synchronize both chaotic and hyperchaotic energy resource
systems.
This paper is organized as follows: In Section 2 we apply predictive synchronization to chaotic energy resource system
and numerical results are given to show this process. In Section 3 we perform predictive synchronization on hyperchaotic
energy resource system and numerical simulations are provided. Finally, conclusion is given in Section 4.
2. Predictive synchronization of chaotic energy system
The three-dimensional (3-D) energy resource system [5] is expressed by the following set of ordinary differential equa-
tions
˙ x = a
1
x(1 - x/M) - a
2
(y + z)
˙ y = -b
1
y - b
2
z + b
3
x[N - (x - z)]
˙ z = c
1
z(c
2
x - c
3
)
(1)
∗
Corresponding author.
E-mail address: aboukabou@univ-jijel.dz (A. Boukabou).
http://dx.doi.org/10.1016/j.ijleo.2016.05.005
0030-4026/© 2016 Published by Elsevier GmbH.