G. Caginalp introduced in  the following phase-field system
where u is the order parameter and is the (relative) temperature. These equations model phase transition processes such as melting-solidification processes and have been studied, see  -  , for a similar phase-field model with a nonlinear term.
These Cahn-Hilliard phase-fiel system are known as the conserved phase-field system (see  -  ) based on type III heat conduction and with two temperatures (see  ). The authors have proved the existence and the uniqueness of the solutions, the existence of global attractor and of exponential attractors with singularly or regular potentials.
In  , Ntsokongo and Batangouna have studied the following Cahn-Hilliard phase- field system
where, u is the order parameter and is the (relative) temperature, they have proved the existence and the uniqueness solution with Dirichlet boundary condition and regular potentials.
In this paper, we consider the following Cahn-Hilliard hyperbolic phase-fiel system
which is the perturbed phase-field system of Cahn-Hilliard phase-field system (3)-(4) with. In the above hyperbolic system is a bounded and regular domain of with or 3 and f is the nonlinear regular potentials.
The hyperbolic system has been extensively studied for Dirichlet boundary conditions and regular or singular potentials (see  -  ). Whose certain have to end at existence of global attractor or at the existence of exponential attractors (see  ).
In this paper we prove the existence and the uniqueness of solutions of (5)-(8). We consider the regular potential which satisfies the following properties:
We denote by the usual L2-norm (with associated product scalar (.,.)) and set
, where denotes the minus Laplace operator with Dirichlet
boundary conditions. More generally, denote the norm of Banach space X.
Throughout this paper, the same letters and denote (generally positive) constants which may change from line to line, or even a same line.
3. A Priori Estimates
We multiply (5) by and (6) by, integrate over and add the two resulting differential equalities. We find
Finaly, we conclude that,
Multiply (6) by and integrate over. We get.
In this study, we have three main results; existence theorem, uniqueness theorem and existence theorem with more regularity.
4. Existence and Uniqueness of Solutions
Theorem 4.1. (Existence) We assume then the system (5) - (8) possesses at least one solution such that
and, for all.
The proof is based on a priori estimates obtained in the previous section and on a standard Galerkin scheme.
Theorem 4.2. (Uniqueness) Let the assumpptions of Theorem 4.1 hold. Then, the system (5) - (8) possesses a unique solution such that
and for all.
Proof. Let and be two solutions of the system (5)-(8) with initial data and, respectively. We set and, then is solution of the following system
We multiply (12) by and integrate over. We find
Multiplying (13) by and integrating over, we get
Now summing (14) and (15) we obtain
Lagrange theorem gives a estimates
Inserting the above estimate into (16), we have
Applying Gronwall’s lemma, we obtain for all
We deduce the continuous dependence of the solution relative to the initial conditions, hence the uniqueness of the solution.
The existence and uniqueness of the solution of problem (5)-(8) being proven in a larger space, we will seek the solution with more regularity.
Theorem 4.3. Assume
then the system (5)-(8) possesses a unique solution such that
and, for all.
Proof. Following theorems 4.1 and 4.2, the system (5)-(8) possesses the unique solution such that
and, for all.
Multiply (2.1) by and integrate over. We have
we deduce the following inequality
Thanks to use, we find the following estimate
Since, then the estimate (17) implies
Multiplying (6) by and integrating over, we get
Now summing (18) and (19), we obtain
Appling the Gronwall’s lemma, we deduce that,
Multiplying (5) by and integrating ovre, we obtain
Thanks to use and the fact that, we get
Inserting the above estimate into (20), we obtain
which implies that.
Multiplying (6) by and integrating over, we find
We have just shown the theorems of existence and uniqueness of the solutions for perturbed Cahn-Hilliard hyperbolic phase-field system with regular potentials.
 Caginalp, G. (1988) Conserved-Phase Field System: Implications for Kinetic Undercooling. Physical Review B, 38, 789-791.
 Gatti, S. and Pata, V. (2004) Exponential Attractor for a Conserved Phase-Field System with Memory. Physica D: Nonlinear Phenomena, 189, 31-48.
 Miranville, A. (2013) On the Conserved Phase-Field Model. Journal of Mathematical Analysis and Applications, 400, 143-152.
 Colli, P., Gilardi, G., Laurenot, Ph. and Novick-Cohen, A. (1999) Uniqueness and Long-Time Behavior for the Conserved Phase-Field System Memory. Discrete and Continuous Dynamical Systems—Series A, 5, 375-390.
 Miranville, A. and Quintanilla, R. (2011) A Type III Phase-Field System with a Logarithmic Potential. Applied Mathematics Letters, 24, 1003-1008.
 Ntsokongo, A.J. and Batangouna, N. (2016) Existence and Uniqueness of Solutions for a Conserved Phase-Field Type Model. AIMS Mathematics, 1, 144-155.
 Goyaud, M.E.I., Moukamba, F., Moukoko, D. and Langa, F.D.R. (2015) Existence and Uniqueness of Solution for Caginalp Hyperbolic Phase Field System with Polynomial Growth Potential. International Mathematical Forum, 10, 477-486.