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## Nonlinear Systems: Asymptotic Methods, Stability, Chaos, Control, and Optimization

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Research Article | Open Access

Volume 2011 |Article ID 723629 | 11 pages | https://doi.org/10.1155/2011/723629

# Numerical Integration and Synchronization for the 3-Dimensional Metriplectic Volterra System

Accepted29 Jun 2010
Published02 Aug 2010

#### Abstract

The main purpose of this paper is to study the metriplectic system associated to 3-dimensional Volterra model. For this system we investigate the stability problem and numerical integration via Kahan's integrator. Finally, the synchronization problem for two coupled metriplectic Volterra systems is discussed.

#### 1. Introduction

To give a unification of the conservative and dissipative dynamics, Kaufman  has introduced the concept of metriplectic system.

Let be a local coordinate system on . We consider be a Hamilton-Poisson system on with Hamiltonian , where and

We add to the Hamilton-Poisson system (1.1) a dissipation term of the form , where is a symmetric matrix which satisfies certain compatibility conditions, and , where and are a Casimir function (i.e., ). One obtains a family of metriplectic systems of the form This family of metriplectic systems have the same Hamiltonian and the same Casimir function . For each , the metriplectic systems (1.2) can be viewed as a perturbation of Hamilton-Poisson system (1.1).

The differential systems of the form (1.2) and their applications have been studied in connection with several dynamical systems derived from mathematical physics; see for instance, .

Another way for giving rise to a dynamical system of the form of (1.2) is based on the definition of a metriplectic structure on . These systems can be expressed in terms of Leibniz bracket, see .

The paper is structured as follows. In Section 2, the metriplectic system associated to dimensional Volterra model (2.8) is constructed. For this dynamical system, the stability of equilibrium states is investigated. In Section 3, we discuss the numerical integration for the system (2.8).

Synchronization problem for dynamical systems has received a great deal of interest due to their application in different fields of science; see . For this reason, Section 4 is dedicated to synchronization problem for two coupled metriplectic Volterra systems of the form of (2.8).

#### 2. The Metriplectic System Associated to 3-Dimensional Volterra Model

Let be a Hamilton-Poisson system given by (1.1). For this system we determine the symmetric matrix , where

If is a Casimir function for the configuration , then we take , where is a parameter.

For , and the matrix determined by relations (2.1), we write the differential system (1.2) in the following tensorial form:

System (2.2) is a metriplectic system in (see [2, 7]), that is the following conditions are satisfied:

System (2.2) is called the metriplectic system associated to Hamilton-Poisson system (1.1) and is denoted by

Let us construct a metriplectic system of the form of (2.2), starting a Hamilton-Poisson realization of the dimensional Volterra model.

The phase space of the dimensional Volterra model consists of variables , ; see [13, 14]. This is described by the equations

It is well known that system (2.4) has a Hamilton-Poisson realization with the Casimir (see ), where

We apply now relations (2.1) to the function given by (2.6). Then the symmetric matrix is

We take and given by (2.6), the skew-symmetric matrix given by (2.5) and the symmetric matrix given by (2.7). For the function with , system (2.2) becomes

Proposition 2.1. The dynamical system given by (2.8) is a metriplectic system on .

Proof. We have , and , . Then that is, is a Casimir of Hamilton-Poisson system .
We prove that conditions and from (2.3) are verified.
We have , and  , , Then Hence (2.8) is a metriplectic system.

System (2.8) is called the 3-dimensional metriplectic Volterra system. For , it is reduced to Volterra model (2.4).

System (2.8) can be written in the form , , where

Proposition 2.2. The function given by (2.6) is a constant of the motion for the metriplectic Volterra system, that is, it is conserved along the solutions of the dynamics (2.8).
The function decreases along the solutions of system (2.8).

Proof. We have
The derivative of along the solutions of system (2.8) verifies the condition Indeed,

Remark 2.3. If , then is not a constant of motion for the metriplectic system (2.8).

Proposition 2.4. If , then the equilibrium states of the dynamics of (2.8) are for all .
For , the equilibrium states of the dynamics of (2.8) are and  , for all

Proof. The equilibria are the solutions of system , .

Proposition 2.5. The equilibrium states , are unstable.

Proof. Let be the matrix of the linear part of the system (2.8), that is, The characteristic polynomial of the matrix is with the roots , Then the assertion follows via Lyapunov's theorem .

Remark 2.6. The dynamics of (2.4) and (2.8) have not the same equilibria.
For , have the following behaviors (see ): is unstable if and spectrally stable if ; is unstable, and is unstable if and spectrally stable if .

#### 3. Numerical Integration of the Metriplectic Volterra System (2.8)

For (2.8), Kahan's integrator (see for details ) can be written in the following form:

Remark 3.1. Taking in relations (3.1) we obtain the numerical integration for Volterra model (2.4) via Kahan's integrator.

Proposition 3.2. Kahan's integrator (3.1) preserves the constant of motion of the dynamics of (2.8).

Proof. Indeed, adding all equations (3.1) we obtain Hence

For the initial conditions , , and , the solutions of Volterra model (2.4) (using Kahan's integrator (3.1) with ), are represented in the system of coordinates in Figure 1.

For the same initial conditions, the solutions of the metriplectic Volterra system (2.8) for (using Kahan's integrator (3.1) with ), are represented in the system of coordinates in Figure 2.

Remark 3.3. Using Runge-Kutta 4 steps integrator, we obtain almost the same result; see Figure 3.

#### 4. The Synchronization of Two Metriplectic Volterra Systems

In this section we apply Pecora and Carroll method for constructing the drive-response configuration (see ).

Let us build the configuration with the drive system given by the metriplectic Volterra system (2.8), and a response system (this is obtained from (2.8) by replacing with and adding for ). Suppose that these systems are coupled. More precisely, the second system is driven by the first one, but the behavior of the first system is not affected by the second one.

Therefore, the drive and response systems are given by respectively where are three control functions.

We define the synchronization error system as the subtraction of the metriplectic Volterra model (4.1) from the controlled metriplectic Volterra model (4.2): By subtracting (4.2) from (4.1) and using notation (4.3) we can get We define the active control inputs as follows: where and , are real functions which depend on Then the differential system of errors (4.7) is given by If we choose then the active controls defined by (4.5) become Using (4.8), the system of errors (4.7) becomes

Proposition 4.1. The equilibrium state of the differential system (4.10) is asymptotically stable.

Proof. An easy computation shows that the all conditions of Lyapunov-Malkin theorem  are satisfied, and so we have that the equilibrium state is asymptotically stable.

Numerical simulations are carried out using the software MATHEMA-TICA 6. We consider the case . The fourth-order Runge-Kutta integrator is used to solve systems (4.1), (4.2), and (4.10) with the control functions given by (4.9).

The initial values of the drive system (4.1) and response system (4.2) are , , and , , These choices result in initial errors of , , and

The dynamics of the metriplectic Volterra system (4.1) to be synchronized with the dynamic of (4.2) accompanied with the control functions given by (4.9) and the dynamics of synchronization errors given by (4.10) are shown in Figures 5, 6, and 7.

According to numerical simulations, by a good choice of parameters the synchronization error states converge to zero, and hence the synchronization between two coupled metriplectic Volterra systems is achieved.

Remark 4.2. Taking in (4.1), (4.2), (4.8), and (4.9), we obtain the synchronization between two coupled Volterra models of the form of (2.4).

#### 5. Conclusion

It is well known that many nonlinear differential systems like the Euler equations of fluid dynamics, the soliton equations can be written in the Hamiltonian form. An interesting example of nonlinear lattice equations is Volterra lattice (see ) which is a model for vibrations of the particles on lattices. Also the behavior of viscoelastic materials is an example where the dynamics is governed by Volterra equations. The metriplectic systems will be successfully used in mathematical physics, fluid mechanics, and information security; see for instance [4, 5, 10, 12].

In this paper we have build a metriplectic system on associated to Volterra model. For the metriplectic Volterra system (2.8), we have presented some relevant geometrical and dynamics properties and the numerical integration. Finally, using the Pecora and Carroll method, the synchronization problem for two coupled metriplectic Volterra systems of the form of (2.8) is discussed. This technique is realized since a suitable control has been chosen to achieve synchronization.

1. A. N. Kaufman, “Dissipative Hamiltonian systems: a unifying principle,” Physics Letters A, vol. 100, no. 8, pp. 419–422, 1984. View at: Publisher Site | Google Scholar | MathSciNet
2. P. Birtea, M. Boleanţu, M. Puta, and R. M. Tudoran, “Asymptotic stability for a class of metriplectic systems,” Journal of Mathematical Physics, vol. 48, no. 8, Article ID 082703, 7 pages, 2007.
3. M. Grmela, “Bracket formulation of dissipative fluid mechanics,” Physics Letters A, vol. 102, no. 8, pp. 355–358, 1984. View at: Publisher Site | Google Scholar | MathSciNet
4. P. J. Morrison, “A paradigm for joined Hamiltonian and dissipative systems,” Physica D, vol. 18, no. 1–3, pp. 410–419, 1986.
5. D. Fish, Geometrical structures of the metriplectic dynamical systems, Ph.D. thesis, Portland, Ore, USA, 2005.
6. P. Guha, “Metriplectic structure, Leibniz dynamics and dissipative systems,” Journal of Mathematical Analysis and Applications, vol. 326, no. 1, pp. 121–136, 2007.
7. G. Ivan and D. Opriş, “Dynamical systems on Leibniz algebroids,” Differential Geometry—Dynamical Systems, vol. 8, pp. 127–137, 2006.
8. J.-P. Ortega and V. Planas-Bielsa, “Dynamics on Leibniz manifolds,” Journal of Geometry and Physics, vol. 52, no. 1, pp. 1–27, 2004.
9. H. N. Agiza and M. T. Yassen, “Synchronization of Rössler and Chen chaotic dynamical systems using active control,” Physics Letters A, vol. 278, no. 4, pp. 191–197, 2001. View at: Publisher Site | Google Scholar | MathSciNet
10. O. T. Chiş and D. Opriş, “Synchronization and cryptography using chaotic dynamical systems,” in Proceedings of the International Conference of Differential Geometry and Dynamical Systems, vol. 16 of BSG Proceedings [BGSP], pp. 47–56, Geometry Balkan Press, Bucharest, Romania, 2009. View at: Google Scholar
11. M.-C. Ho, Y.-C. Hung, and I.-M. Jiang, “On the synchronization of uncertain chaotic systems,” Chaos, Solitons & Fractals, vol. 33, pp. 540–546, 2007. View at: Publisher Site | Google Scholar
12. L. M. Pecora and T. L. Carroll, “Synchronization in chaotic systems,” Physical Review Letters, vol. 64, no. 8, pp. 821–824, 1990.
13. L. D. Fadeev and L. A. Takhtajan, Hamiltonian Methods in the Theory of Solitons, Springer, Berlin, Germany, 1986.
14. M. Puta and M. Khashan, “Poisson geometry of the Volterra model,” Analele Universităţii din Timişoara, Seria Matematică—Informatică, vol. 39, pp. 377–384, 2001.
15. M. W. Hirsch and S. Smale, Differential Equations, Dynamical Systems, and Linear Algebra, Academic Press, New York, NY, USA, 1974. View at: MathSciNet
16. W. Kahan, “Unconventional numerical methods for trajectory calculations,” Unpublished lecture notes, 1993. View at: Google Scholar
17. D. V. Zenkov, A. M. Bloch, and J. E. Marsden, “The energy-momentum method for the stability of non-holonomic systems,” Dynamics and Stability of Systems, vol. 13, no. 2, pp. 123–165, 1998.
18. Y. B. Suris, “Integrable discretizations for lattice system: local equations of motion and their Hamiltonian properties,” Reviews in Mathematical Physics, vol. 11, no. 6, pp. 727–822, 1999. Download other formatsMore  Order printed copiesOrder 