Comparative Analysis of the Chaotic Behavior of a Five-Dimensional Fractional Hyperchaotic System with Constant and Variable Order

: A five-dimensional hyperchaotic system is a dynamical system with five state variables that exhibits chaotic behavior in multiple directions. In this work, we incorporated a 5D hyperchaotic system with constant-and variable-order Caputo and the Caputo–Fabrizio fractional derivatives. These fractional 5D hyperchaotic systems are solved numerically. Through simulations, the chaotic behavior of these fractional-order hyperchaotic systems is analyzed and a comparison between constant-and variable-order fractional hyperchaotic systems is presented


Introduction
A hyperchaotic system is a system that shows multiple chaotic behaviors simultaneously.These type of systems have more complex chaotic dynamics than regular chaotic systems.Hyperchaotic systems involve the presence of multiple positive Lyapunov exponents that indicate a higher degree of unpredictability and complexity in their behavior.The unique characteristics of hyperchaotic systems make them valuable in various fields where randomness, complexity, and security are important considerations.
For years, hyperchaotic systems have progressed consistently since their introduction by Rossler [1].Recently, numerous distinct hyperchaotic systems have been developed, such as the 2D hyperchaotic system for image encryption proposed by Erkan, Toktas, and Lai [2].Erkan et al. also [3] designed a two dimensional hyperchaotic system using the optimization benchmark function.Zhu et al. [4] constructed a 2D hyperchaotic map with application in pseudo-random number generation and color image encryption.Gao [5] presented an image encryption algorithm based on a 2D hyperchaotic system.A 2D cosine-sine interleaved chaotic system for secure communications was introduced by Tang et al. [6].A simple chaotic model with complex chaotic behavior was also studied by Tang et al. [7].Further developments in 3D hyperchaotic systems with applications in secure transmission were studied by Li et al. [8].A non-degenerate hyperchaotic map with an ultra-wide parameter range was presented by Huang et al. [9].Cui and Li [10] proposed a hyperchaotic system with four dimensions.The dynamics of a multi-stable 4D hyperchaotic Lorenz system, along with its applications, were studied by Leutcho et al. [11].Advancements in dynamical systems with five state variables with more than one positive Lyapunov exponent were studied by Ojoniyi and Njah [12], along with coexisting hidden attractors.A multistable 5D memristive hyperchaotic system with coexisting multiple attractors was studied by Yu et al. [13].Li and Cui [14] proposed a 5D hyperchaotic system and provided a dynamical analysis.
Instead of using integer-order derivatives and integrals, hyperchaotic systems can be described with fractional-order derivatives.Fractional derivatives are a generalization of the concept of derivatives to non-integer (fractional) orders.This advanced mathematical framework effectively models systems with memory and hereditary properties, which are common in various complex physical, biological, and engineering systems.Key types of fractional derivatives include Riemann-Liouville [30], Liouville-Caputo [30], Caputo-Fabrizio [31], and more.These equations allow for a more nuanced description of system dynamics.The synchronization of chaotic systems with fractional orders facilitates secure communication and information transmission.By incorporating fractional calculus [30], hyperchaotic systems can capture complex behaviors that may not be fully captured by integer-order models.This introduces additional complexity into the dynamics of hyperchaotic systems, which includes long-range memory effects, non-local interactions, and anomalous diffusion.Iskakova et al. [32] studied the dynamics of a 4D hyperchaotic system using integerand fractional-order derivatives.Feng et al. [33] considered a fractional-order 3D Lorenz chaotic system and 2D discrete polynomial hyperchaotic map for high-performance multiimage encryption.Az-Zo'bi et al. [34] studied the dynamics of a generalized time-fractional viscous-capillarity compressible fluid model.Sene [35] presented the theory and applications of a fractional-order chaotic system with a Caputo operator.
In this work, we study the complex and dynamical behavior of a five-dimensional hyperchaotic system.We will incorporate the 5D hyperchaotic system proposed by Azzawi and Hasan [44] with constant-and variable-order Caputo and Caputo-Fabrizio (CF) fractional derivatives.
In fractional derivatives with a constant order, the derivative remains constant throughout the process, while a variable-order fractional derivative [45] is a generalization of the traditional fractional derivative (order of the derivative remains constant in traditional fractional calculus) where the order of differentiation varies as a function of time or space.By allowing the fractional order to vary, variable-order fractional derivatives provide a more versatile and responsive method for modeling and studying intricate systems.The application of variable-order fractional derivatives can be seen in neural networks [46], solid mechanics [47], dynamic analyses of a nonlinear oscillator [48], etc.
In our current work, we consider the following fractional-order 5D hyperchaotic system.
• 5D constant-order fractional Caputo hyperchaotic system: • 5D variable-order fractional Caputo hyperchaotic system: • 5D constant-order fractional Caputo-Fabrizio hyperchaotic system: • 5D variable-order fractional Caputo-Fabrizio hyperchaotic system: where Here, x, y, z, u, v are driving variables and a, b, c, p are constants.The paper is organized in the following manner.Section 2 provides the preliminaries.In Section 3, we obtain the numerical solution and simulations for the 5D constantand variable-order fractional Caputo hyperchaotic systems.In Section 4, we obtain the numerical solution and simulations for the 5D constant-and variable-order fractional Caputo-Fabrizio hyperchaotic system.Finally, the conclusion is provided in Section 5.

Computational Techniques for Solving a 5D Constant-and Variable-Order Fractional Caputo Hyperchaotic System
In this section, we compute the numerical solutions for the 5D constant-order fractional Caputo hyperchaotic system and the 5D variable-order fractional Caputo hyperchaotic system.
To find the numerical solution for a 5D constant-order fractional Caputo hyperchaotic system, we take into account the method as proposed in [50] and will take into account the numerical method proposed by Perez et al. [49] to compute the numerical solution for the 5D variable-order fractional Caputo hyperchaotic system.

Computational Techniques for Solving a 5D Constant-Order Caputo Hyperchaotic System
Consider the 5D constant-order fractional Caputo hyperchaotic system, which is as follows: where LC 0 D ϱ 0 represents the Caputo fractional derivative with constant order.To find the numerical solution, consider the following equation: where Using the numerical method given by [50], Equation ( 10) can be reformulated as follows: at time t = t n+1 , Equation ( 11) is as follows: at time t = t n , Equation ( 11) is as follows: From ( 12) and ( 13) Using Lagrange polynomial interpolation, the numerical solution of Equation ( 10) is as follows: Hence, the numerical solutions for the 5D constant-order fractional hyperchaotic system are given as follows: where where ϑ 2 (t, y) = x − y. where where where ϑ 5 (t, v) = x + p y z.
By solving the above equations, we can obtain the solutions for the 5D constant-order fractional Caputo hyperchaotic system.

Computational Techniques for Solving a 5D Variable-Order Fractional Caputo Hyperchaotic System
Consider the 5D variable-order fractional Caputo hyperchaotic system, which is given as follows: where LC 0 D ϱ(t) 0 represents the Caputo fractional derivative with variable order.To find the numerical solutions, consider the following equation: where, S(t) = {x(t), y(t), z(t), u(t), v(t)} and S(0) = {x(0), y(0), z(0), u(0), v(0)}.Equation ( 22) is simplified as presented in [50] to obtain At t = t n+1 , Equation ( 23) is formulated as follows: The function f (w, S(w)) is approximated using the two-step Lagrange polynomial interpolation in an interval [t k , t k+1 ] Now, considering Equations ( 24) and (25), we have For ease of calculation, we define the following expressions: From ( 26) and ( 27) Hence, for the variable-order hyperchaotic system with a Caputo derivative, the numerical solutions are as follows: where where ϑ 2 (t, y) = x − y. where where where ϑ 5 (t, v) = x + p y z.By solving the above equations, we can obtain the solutions for the 5D variable-order fractional Caputo hyperchaotic system.

Computational Techniques for Solving the 5D Constant-and Variable-Order Fractional CF Hyperchaotic Systems
In this section, we compute the numerical solutions for the 5D constant-order fractional CF hyperchaotic system and the 5D variable-order fractional CF hyperchaotic system.
To find the numerical solution for the 5D constant-order fractional CF hyperchaotic system, we take into account the method proposed by Toufik and Atangana [51] and will take into account the numerical method proposed by Perez et al. [49].

Numerical Solutions for Solving the 5D Constant-Order Fractional CF Hyperchaotic System
Consider the 5D constant-order fractional CF hyperchaotic system, which is as follows: where CF D ϱ t is the constant-order CF fractional derivative.
Using the method referenced in [50], we rewrite the above equation as follows: At time t = t n+1 , Equation (37) becomes At time t = t n , Equation ( 37) can be used to obtain the following: From Equations ( 38) and ( 39), we can obtain the following: t n ϑ(w, S(w))dw.(40) Lagrange polynomial interpolation on ϑ(w, S(w)) leads to the following: Substituting ϑ (w, S(w)) in Equation ( 40), we can obtain the following: Substituting h = t n − t n−1 and after solving this, we have Hence, the numerical solutions for the 5D constant-order fractional CF hyperchaotic system are given as follows: where, ϑ 1 (t, x) = y z − c v.
Solving the above equations, we can obtain the solutions for the 5D variable-order fractional CF hyperchaotic system.

A Computational Method for Solving the 5D Variable-Order Fractional CF Hyperchaotic System
Consider the 5D variable-order fractional CF hyperchaotic system, which is given as follows: where is the variable-order CF fractional derivative.
Solving the above equations, we can obtain the solutions for the 5D variable-order fractional CF hyperchaotic system.
The next section presents the simulations used to understand the chaotic behavior of the 5D constant-and variable-order fractional CF hyperchaotic systems using phase portraits and 3D graphs.

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In Figure 1, the phase portraits illustrating the behavior of the 5D constant-and variable-order fractional hyperchaotic systems with the Caputo derivative are presented.

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Figures 2-4 present the 3D graphs used to illustrate the behavior of the 5D constantand variable-order fractional hyperchaotic systems with Caputo derivative.

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In Figures 5 and 6, the phase portraits illustrating the behavior of the 5D constant-and variable-order fractional hyperchaotic systems with the CF derivative are given.• Figures 7-9 present the 3D graphs illustrating the behavior of the constant-and variable-order fractional hyperchaotic systems with the CF derivative.
A difference can be observed between the dynamics of the behavior of the solution of the hyperchaotic system with constant order and the dynamics of the solution's behavior with the variable order.We observe that when the order of the fractional derivative varies with respect to time, the intrinsic dynamics of the hyperchaotic system are captured more effectively as compared to the constant-order fractional hyperchaotic system.This shows that the variable-order hyperchaotic system provides a more comprehensive analysis and better understanding of the chaotic behavior of the system compared to the constantorder system.
Further, in Figures 1-9, we can observe a difference in the chaotic behavior of the hyperchaotic system with two different fractional derivatives (Caputo and CF).We observe that due to the exponential kernel in the CF derivative, we see more complexity in the chaotic behaviour of the fractional hyperchaotic system with the CF derivative as compared to the fractional hyperchotic system with the Caputo derivative.

Conclusions
In this study, we examined both the constant-and variable-order fractional 5D hyperchaotic systems using the Caputo and CF derivatives.Numerical solutions for all four cases are presented in Sections 3 and 4, along with the simulations.Figures 1-4 show the chaotic behavior of the 5D constant-and variable-order Caputo fractional hyperchaotic systems at fractional order ϱ = 0.8999.Figures 5-9 illustrate the same for the CF fractional systems.By observing the figures, we conclude that the simulations highlight differences between constant-and variable-order Caputo and CF derivatives.Varying the fractional order with respect to t adds complexity to the chaotic behavior.As we examined the hyperchaotic system with two different fractional derivatives (Caputo and CF), our results demonstrate that the selection of fractional derivative markedly influences the chaotic behavior of the system.We observe that the CF derivative provides a more profound insight into the complexity of the 5D hyperchaotic system compared to the Caputo derivative.The exponential kernel in the CF derivative induces extensive interactions, leading to an intricate and unpredictable behavior.We also observe that hyperchaotic systems with a variableorder fractional derivative enable a more comprehensive analysis of the chaotic regions as compared to hyperchaotic systems with constant-order fractional derivatives.Hence, a hyperchaotic system with a variable-order fractional derivative deepens the understanding of the system's dynamics.