Abstract and Applied Analysis

Volume 2014 (2014), Article ID 623129, 14 pages

http://dx.doi.org/10.1155/2014/623129

Research Article

Optimal Control Problem with Necessary Optimality Conditions for the Viscous Dullin-Gottwald-Holm Equation

Jinsoo Hwang

Department of Mathematics Education, Daegu University, Jillyang, Gyeongsan, Gyeongbuk 712-714, Republic of Korea

Received 20 September 2013; Revised 5 January 2014; Accepted 7 January 2014; Published 24 February 2014

Academic Editor: Ziemowit Popowicz

Copyright © 2014 Jinsoo Hwang. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

We study the quadratic cost optimal control problems for the viscous Dullin-Gottwald-Holm equation. The main novelty of this paper is to derive the necessary optimality conditions of optimal controls, corresponding to physically meaningful distributive observations. For this we prove the Gâteaux differentiability of nonlinear solution mapping on control variables. Moreover by making use of the second order Gâteaux differentiability of solution mapping on control variables, we prove the local uniqueness of optimal control. This is another novelty of the paper.

1. Introduction

Recently, in the study of shallow water wave, Dullin et al. [1] derived a new integrable shallow water wave equation with linear and nonlinear dispersion as follows:

where is fluid velocity, and are squares of length scales, and is the linear wave speed for undisturbed water at rest at spatial infinity, where and its spatial derivatives are taken to vanish. Letting , (1) reduces to the well-known Korteweg-de Vries (KDV) equation (linear dispersion case). And when letting , (1) reduces to the Camassa-Holm equation of [2] (nonlinear dispersion case). Usually we can rewrite (1) into

where is a momentum variable. Physically, the third and fourth terms of the left side of (2) represent convection and stretching effects of unidirectional propagation of shallow water waves over a flat bottom, respectively (see [2, 3]).

Many researchers studied the well-posedness of Cauchy problem for the DGH equation including various properties of the solution of it (see [4–6]).

Recently, Shen et al. [7] studied the optimal control problem of the following viscous DGH equation (cf. [3]):

where and stands for the viscosity constant of shallow water wave. As explained in Holm and Staley [8], the small viscosity makes sense to take into account the balance or relaxation between convection and stretching dynamics of shallow water wave.

In [7] Shen et al. studied the distributive optimal control problems of (3) (cf. [3]). For this purpose, they modified (3) to Dirichlet boundary value problem in short interval and proved the existence and uniqueness of in (3) by weak formulation. However the well-posedness of (3) with respect to is unclear and the proof contained in [7] relies on the size of which is an extra condition. Further, in [7] they employed the quadratic cost objective functional to be minimized within an admissible control set with the distributive observation of in (3) and only discussed the existence of optimal controls which minimize the quadratic cost. But the necessary optimality conditions of optimal controls have not been studied there.

As for the necessary optimality condition of optimal controls, we can find a recent paper Sun [9]. By employing the Dubovitskii and Milyutin functional analytic approach, Sun has established in [9, Theorem 3] the Pontryagin maximum principle of the optimal control for the viscous DGH equation with the quite general cost which depends on and not on . Meanwhile, in this paper, we propose the quadratic cost functional for , which is actually more reasonable than that for , and establish the necessary optimality conditions of optimal controls due to Lions [10] in Theorems 5 and 7 for the physically meaningful observations and , respectively. To this end, we successfully characterize the Gâteaux derivative of in the direction , where is a Hilbert space of control variables and is an optimal control for quadratic cost.

Actually, the extension of optimal control theory to quasilinear equations is not easy. Some researches have been devoted to the study of optimal control or identification problems in specific quasilinear equations. For instance, we can refer to Hwang and Nakagiri [11, 12] and Hwang [13, 14].

The aim of this paper can be summarized as follows. Firstly, we clarify the well-posedness of (3) with respect to in the Hadamard sense with appropriate initial value condition in short interval as posed in [7]. Secondly, based on the well-posedness result, we expand the optimal control theory due to Lions [10] with emphasis on deriving necessary optimality conditions of optimal controls in the following distributive control system:

where , is a forcing term, is a controller, is a control, and denotes the state for a given .

In order to apply the variational approach due to Lions [10] to our problem, we propose the quadratic cost functional as studied in Lions [10] which is to be minimized within ;   is an admissible set of control variables in . We show the existence of which minimizes the quadratic cost functional . Then, we establish the necessary conditions of optimality of the optimal control for some physically meaningful observation cases employing the associate adjoint systems. For this we successfully prove the Gâteaux differentiability of the nonlinear solution mapping , which is used to define the associate adjoint systems.

Moreover, in this paper we discuss the local uniqueness of optimal control. As widely known, it is unclear and difficult to verify the uniqueness of optimal control in nonlinear control problems. By employing the idea given in Ryu [15], we show the strict convexity of the quadratic cost in local time interval by utilizing the second order Gâteaux differentiability of the nonlinear solution mapping . Whence by proving strict convexity of the quadratic cost with respect to the control variable, we prove the local uniqueness of optimal control. This is another novelty of the paper.

2. Preliminaries

For fixed , we set and . The scalar products and norms on and , , are denoted by , and , , , respectively. Then, by virtue of Poincare inequality, we can replace these scalar products and norms by and , , respectively. Let us denote the topological dual spaces of , , by , . We denote their duality pairing between and by , .

We consider the following Dirichlet boundary value problem for the viscous Dullin-Gottwald-Holm (DGH) equation:

where ,   is a forcing function, and is an initial value.

In order to define weak solutions of (5), we define some Hilbert spaces. At first, is defined by

endowed with the norm

where denotes the first order distributional derivatives of . Further, is defined by

endowed with the norm

where denotes the first order distributional derivatives of . We note here that and are continuously imbedded in and , respectively (cf. Dautray and Lions [16, page 555]).

From now on, we will omit writing the integral variables in the definite integral without any confusion.

Lemma 1. Let satisfy the boundary conditions of (5) and . Then one has

where is a constant.

Proof. According to the boundary conditions of , we have

Since is an isomorphism, we can deduce that

where are constants. Thus we prove this lemma.

The following variational formulation is used to define the weak solution of (5).

Definition 2. A function is said to be a weak solution of (5) if and satisfies

In order to verify the well-posedness of (5), we partially refer to the result by Shen et al. [7]. The well-posedness of (5) in the sense of Hadamard can be given as follows.

Theorem 3. Assume that , , and . Then the problem (5) has a unique solution in . And the solution mapping of into is a local Lipschitz continuous; that is, for each and , one has the inequality

where is a constant which depends on and .

Remark 4. In [7], the well-posedness of (5) is partially verified, which is indeed the case that the viscosity constant is large enough. However, as we will see in the Appendix, such an extra assumption can be removed.

Proof of Theorem 3. By utilizing the result of [7], combined with Lemma 1, we can know that (5) possesses a unique solution under the data condition .

Based on the above result, we prove the inequality (14). For that purpose, we denote by and by . Then, we can observe from (5) that

where and , . Multiplying in both sides of (15), we have

And we integrate (16) over to have

By Sobolev embedding theorem, , , and , the right members of (17) can be estimated as follows:

where are constants. We replace the right hand side of (17) by the right members of (18). Then we have

where is a constant, depending on and . And we apply the Gronwall inequality to (19) to obtain

where is a constant, depending on and . Next we estimate in (15) as follows:

By Sobolev embedding theorem, we have the following inequality:

where , are constants, depending on and . By (21) and (22) we can obtain

where , are constants, depending on and . We can deduce that (20) and (23) imply

where is a constant, depending on and . Finally from Lemma 1 and (24) we have

where , are constants, depending on and . Thus we complete the proof.

3. Quadratic Cost Optimal Control Problems

In this section we study the quadratic cost optimal control problems for the viscous DGH equation due to the theory of Lions [10]. Let be a Hilbert space of control variables, and let be an operator,

called a controller. We consider the following nonlinear control system:

where , , , and is a control. By virtue of Theorem 3 and (26), we can define uniquely the solution map of into . We will call the solution of (27) the state of the control system (27). The observation of the state is assumed to be given by

where is an operator called the observer and is a Hilbert space of observation variables. The quadratic cost function associated with the control system (27) is given by

where is a desired value of and is symmetric and positive; that is,

for some . Let be a closed convex subset of , which is called the admissible set. An element which attains the minimum of over is called an optimal control for the cost (29).

In this section we will characterize the optimal controls by giving necessary conditions for optimality. For this it is necessary to write down the necessary optimality condition,

and to analyze (31) in view of the proper adjoint state system, where denote the Gâteaux derivative of at . And we study local uniqueness of the optimal control.

As indicated in Section 1, we show the existence of an optimal control and give the characterizations of them.

3.1. Existence of the Optimal Control

Now we show the existence of an optimal control for the cost (29).

Theorem 5. Assume that the hypotheses of Theorem 3 are satisfied. Then there exists at least one optimal control for the control problem (27) with the cost (29).

Proof. Set . Since is nonempty, there is a sequence in such that

Obviously is bounded in . Then by (30) there exists a constant such that

This shows that is bounded in . Since is closed and convex, we can choose a subsequence (denoted again by ) of and find a such that

as . From now on, each state corresponding to is the solution of

where . By (33) the term is estimated as

Hence we can deduce from Theorem 3 that

for some . And also from Lemma 1 we can know that

for some . Therefore, by the extraction theorem of Rellich’s, we can find a subsequence of , say again , and find a such that

By using the fact that is compact and by virtue of (39), we can refer to the result of the Aubin-Lions-Temam’s compact imbedding theorem (cf. Temam [17, page 271]) to verify that is precompact in . Hence there exists a subsequence such that

Since , we know that . And from (40) we can choose a subsequence of , denoted again by such that

We use (39)–(41) and apply the Lebesgue dominated convergence theorem to have

as . We replace and by and , respectively, and take in (35). Then by the standard argument in Dautray and Lions [16, pages 561–565], we conclude that the limit satisfies

in weak sense, where . Moreover the uniqueness of weak solutions in (43) via Theorem 3 enables us to conclude that in , which implies weakly in . Since is continuous on and is lower semicontinuous, it follows that

It is also clear from that . Hence

But since by definition, we conclude that . This completes the proof.

3.2. Gâteaux Differentiability of Solution Mapping

In order to characterize the optimal control which satisfies the necessary optimality condition (31), we need to prove the Gâteaux differentiability of the mapping of .

Definition 6. The solution map of into is said to be Gâteaux differentiable at if for any there exists a such that

The operator denotes the Gâteaux derivative of at and the function is called the Gâteaux derivative in the direction , which plays an important role in the nonlinear optimal control problem.

Theorem 7. The map of into is Gâteaux differentiable at and such the Gâteaux derivative of at in the direction , say , is a unique solution of the following problem:

where and .

Proof. Let , . We set and

Then satisfies

where and .

By the continuity of (14), we have

where is a constant, depending on and . Hence we have

Therefore, we can infer that there exists a and a sequence tending to such that

as . Since the imbedding is compact ([17, page 271]), it is implied from (52) that

for some tending to as . Whence by (50)–(53) and Lebesgue dominated convergence theorem we can easily show that

as , where and . And also we can deduce from (49), (52), and (56) that

as .

Hence we can see from (52) to (57) that weakly in as in which is a solution of (47). This convergence can be improved by showing the strong convergence of also in the topology of .

Subtracting (47) from (49) and denoting by , we obtain that

where and .

From (54) and (55) we know that

In order to estimate we multiply in both sides of (58) and integrate it over to have

The integral parts of the right member of (60) can be estimated as follows:

where , , and are constants. We replace the right hand side of (62) by the right members of (61)–(65). And we apply the Gronwall inequality to the replaced inequality; then we arrive at

where is a constant. By virtue of (59) and (66) we deduce that

As in (21)–(23), we have from (58), (66), and (67) that

Therefore (67) and (68) mean

Whence from Lemma 1

This completes the proof.

Theorem 7 means that the cost is Gâteaux differentiable at in the direction and the optimality condition (31) is rewritten by

where is the canonical isomorphism onto and is a desired value.

3.3. Necessary Condition of Optimal Control

In this section we will characterize the optimal controls by giving necessary condition (71) for optimality for the following physically meaningful observations.

(1)We take and and observe

(2)We take and and observe

Since by Theorem 3, the above observations are meaningful.

Due to Lions [10], we construct the necessary condition of optimal control via appropriate adjoint equation. In order to follow the idea we need to introduce and analyze the following adjoint equation for distributive observations:

where or , , and . In order to show the well-posedness of (74), we introduce the solution Hilbert space defined by

equipped with the norm

We remark that is continuously embedded in (cf. Dautray and Lions [16, page 555]).

In the following proposition we show the well-posedness of (74).

Proposition 8. Assume that ; then by reversing the direction of time , (74) admits a unique solution satisfying

where and .

The proof of Proposition 8 is given in the Appendix.

Remark 9. As we will see, there are some merits in taking as the solution space for adjoint equations. For the observation (72), even though we can take the adjoint system in the space with additional boundary conditions, we can derive the same necessary optimality condition of optimal controls through the less regular solution . Therefore, is preferred solution space of adjoint equation for the observation (72). And also, for the observation (73), we need to solve adjoint equation in because of the less regular data condition than that of the observation (72).

3.3.1. Case of the Observation (72)

In this subsection we consider the cost functional expressed by

where is a desired value. Let be the optimal control subject to (27) and (78). Then the optimality condition (71) is represented by

where is the solution of (47).

Now we will formulate the following adjoint system to describe the optimality condition:

where and .

Remark 10. Taking into account the observation conditions , we can assert that (80), reversing the direction of time , admits a unique solution by Proposition 8.

Now we proceed the calculations. We multiply both sides of the weak form of (80) by and integrate it over . Then we have

where . By (47) for , we can verify by integration by parts that the left hand side of (81) yields

where . Therefore, by (81) and (82) we can deduce that the optimality condition (79) is equivalent to

Hence, we give the following theorem.

Theorem 11. The optimal control for (78) is characterized by the following system of equations and inequality:

where and .

3.3.2. Case of the Observation (73)

We consider the following momentum’s distributive cost functional expressed by

where and . Let be the optimal control subject to (27) and (87). Then the optimality condition (71) is rewritten as

where and is the solution of (47). As before we formulate the following adjoint system to describe the optimality condition:

where and .

Remark 12. Since the observation conditions , we know that . Hence by reversing the direction of time and applying Proposition 8, we deduce that (89) admits a unique solution .

As we did before, we multiply both sides of the weak form of (89) by and integrate it over . Then we have

where , , and . By (47) for the integration by parts of the left hand side of (90) yields

where . Therefore, combining (90) and (91), we can deduce that the optimality condition (88) is equivalent to

Hence, we give the following theorem.

Theorem 13. The optimal control for (87) is characterized by the following system of equations and inequality:

where and .

3.4. Local Uniqueness of an Optimal Control

We note that the uniqueness of an optimal control in nonlinear problem is not assured. However, referring to the result in [15], we can show the local uniqueness of the optimal control for our problem. In order to show the uniqueness of optimal control by using strict convexity of quadratic cost (cf. [18]) we consider the following proposition.

Proposition 14. The map of into is second order Gâteaux differentiable at and such the second order Gâteaux derivative of at in the direction , say , is a unique solution of the following problem:

where , , and z is the solution of (47).

Proof. The proof is similar to that of Theorem 7.

Lemma 15. Let be the solution of (96). Then we can show that

where is a constant.

Proof. Let be the solution of (47). Then, using the same arguments as in (5), we can deduce that

where and , are constants which does not depend on . And also for the solution of (96), we can show that

where are constants. Combining (98) with (99), we have (97).

We prove the local uniqueness of the optimal control.

Theorem 16. When is small enough, then there is a unique optimal control for the problem (29) for observations (72) and (73).

Proof. We prove the case (73). Then the same result will be followed for the case (72).

We show the local uniqueness by proving the strict convexity of the map . Therefore as in [18], we need to show for all

For simplicity, we denote , , and by , , and , respectively.

We calculate

where and . From (101) we obtain the second order Gâteaux derivative of as follows:

where .

By Lemma 15 and (102) we deduce that

where and are constants. Here we can take small enough so that the right hand side of (103) is strictly greater than . Therefore we obtain the strict convexity of the quadratic cost , , which prove this theorem.

Remark 17. If we assume is large enough then we can obtain the strict convexity of the quadratic cost (29) in global sense. Therefore we can obtain the desired result of Theorem 16 in global sense for the cost (29).

4. Conclusions

In conclusion, in this paper we considered the optimal distributed control for the viscous Dullin-Gottwald-Holm equation due to Lions [10]. In order to apply the variational approach due to Lions [10] to our problem, we proposed the quadratic cost functional as studied in Lions [10] which is to be minimized within an admissible set of control variables. We showed the existence of optimal controls which minimizes the quadratic cost functional. Then, we established the necessary conditions of optimality of the optimal control for some physically meaningful observation cases employing the associate adjoint systems. For this we successfully proved the Gâteaux differentiability of the nonlinear solution mapping which is used to define the associate adjoint systems. Moreover, by proving strict convexity of the quadratic cost with respect to the control variable, we discussed the local uniqueness of optimal control.

Appendix

Proof of Proposition 8. For simplicity we omit in (74) and put . By reversing time , (74) is transformed as

We apply the Galerkin procedure as in Dautray and Lions [16]. Let be a basis of . For each we define an approximate solution of (A.1) by which satisfies

where . We multiply both sides of (A.2) by and sum over to have

We note here that

Hence we can rewrite (A.3) as follows:

By employing Schwartz’s, Young’s inequality and Sobolev imbedding theorem, we can estimate the right hand side of (A.5) as follows:

where are constants. We put and replace the right hand side of (A.5) by those right members of (A.6) to obtain

where and are constants. Integrating (A.7) over and applying the Gronwall’s inequality to it, we have

Thus we know that

Hence by replacing by in (A.1) and dividing , we obtain the following equality:

which implies via (A.9) that

Therefore we have the boundedness of in . Hence by standard manipulations of Dautray and Lions [16], we can know that there exists a unique limit of in which is the unique solution of (A.1). This proves the well-posedness of (74).

Conflict of Interests

The author declares that there is no conflict of interests regarding the publication of this paper.

Acknowledgment

This paper was supported by the Daegu University Research Grant 2010.

References

H. R. Dullin, G. A. Gottwald, and D. D. Holm, “An integrable shallow water equation with linear and nonlinear dispersion,” Physical Review Letters, vol. 87, pp. 194501–194504, 2001.

R. Camassa and D. D. Holm, “An integrable shallow water equation with peaked solitons,” Physical Review Letters, vol. 71, no. 11, pp. 1661–1664, 1993.

C. Shen and A. Gao, “Optimal control of the viscous weakly dispersive Degasperis-Procesi equation,” Nonlinear Analysis: Theory, Methods and Applications, vol. 72, no. 2, pp. 933–945, 2009.

X. Ai, L. Tian, C. Shen, and G. Guilong, “On the low regularity solutions for the generalized Dullin-Gottwald-Holm equation,” International Journal of NonLinear Science, vol. 7, pp. 113–118, 2009.

O. G. Mustafa, “Existence and uniqueness of low regularity solutions for the dullin-gottwald-holm equation,” Communications in Mathematical Physics, vol. 265, no. 1, pp. 189–200, 2006.

L. Tian, G. Gui, and Y. Liu, “On the well-posedness problem and the scattering problem for the Dullin-Gottwald-Holm equation,” Communications in Mathematical Physics, vol. 257, no. 3, pp. 667–701, 2005.

C. Shen, L. Tian, and A. Gao, “Optimal control of the viscous Dullin-Gottwalld-Holm equation,” Nonlinear Analysis: Real World Applications, vol. 11, no. 1, pp. 480–491, 2010.

D. D. Holm and M. F. Staley, “Wave structure and nonlinear balances in a family of 1 + 1 evolutionary PDEs,” SIAM Journal on Applied Dynamical Systems, vol. 2, no. 1, pp. 323–380, 2003.

B. Sun, “Maximum principle for optimal distributed control of the viscous DullinGottwaldHolm equation,” Nonlinear Analysis: Real World Applications, vol. 13, no. 1, pp. 325–332, 2012.

J. L. Lions, Optimal Control of Systems Governed by Partial Differential Equations, Springer, Berlin, Germany, 1971.

J.-S. Hwang and S.-I. Nakagiri, “Optimal control problems for Kirchhoff type equation with a damping term,” Nonlinear Analysis: Theory, Methods and Applications, vol. 72, no. 3-4, pp. 1621–1631, 2010.

J.-S. Hwang and S.-I. Nakagiri, “Optimal control problems for the equation of motion of membrane with strong viscosity,” Journal of Mathematical Analysis and Applications, vol. 321, no. 1, pp. 327–342, 2006.

J.-S. Hwang, “Optimal control problems for an extensible beam equation,” Journal of Mathematical Analysis and Applications, vol. 353, no. 1, pp. 436–448, 2009.

J. Hwang, “Parameter identification problems for an extensible beam equation,” Journal of Mathematical Analysis and Applications, vol. 359, pp. 682–695, 2009.

S.-U. Ryu, “Optimal control problems governed by some semilinear parabolic equations,” Nonlinear Analysis, Theory, Methods and Applications, vol. 56, no. 2, pp. 241–252, 2004.

R. Dautray and J. L. Lions, Mathematical Analysis and Numerical Methods for Science and Technology, vol. 5 of Evolution Problems I, Springer, 1992.

R. Temam, Navier Stokes Equation, North-Holland, 1984.

E. Zeidler, NonLinear Functional Analysis and Its Applications, II/B, NonLinear Monotone Operator, Springer, Berlin, Germany, 1990.