Abstract
The present work is intended to investigate optimal control for time-dependent variational–hemivariational inequalities in which the constraint set depends on time. Based on the existence, uniqueness and boundedness of the solution to the inequality, we deliver two continuous dependence results with respect to the time, and then, an existence result for an optimal control problem is presented. Finally, a semipermeability problem and a quasistatic frictional contact problem are given to illustrate our main results.
Similar content being viewed by others
Avoid common mistakes on your manuscript.
1 Introduction
Let X be a reflexive Banach space and for every \(t\in {\mathbb {R}}_{+}:= [0, +\infty )\) K(t) be a nonempty, closed and convex subset of X. Let \(A:{\mathbb {R}}_{+}\times X\rightarrow X^{*}\) and \(\varphi :X\times X\rightarrow {\mathbb {R}}\) be given maps to be specified later, \(j :X \rightarrow {\mathbb {R}}\) be a locally Lipschitz function and \(f:\mathbb {R}_+ \rightarrow X^{*}\) be fixed. The problem we will study in this paper is the following time-dependent variational–hemivariational inequality.
Problem 1
Find \(u:{\mathbb {R}}_{+} \rightarrow X\) such that, for all \(t\in {\mathbb {R}}_{+}\), \(u(t)\in K(t)\) and
Hemivariational inequalities were introduced by Panagiotopoulos (see [14, 16, 17]) in the 1980s involving Clarke’s generalized directional derivative of a locally Lipschitz function. Variational–hemivariational inequalities are the important generalization of variational inequalities and hemivariational inequalities which can be seen as a very effective mathematical tool which brings variational inequalities and hemivariational inequalities together since it involves both convex and nonconvex functions. They appear in a variety of mechanical problems, for example the unilateral contact problems in nonlinear elasticity, the problems describing the adhesive and friction effects, the nonconvex semipermeability problems, the masonry structures and the delamination problems in multilayered composites (see, e.g., [9, 15]). For more about the existence, continuous dependence and convergence of solutions to several variational and hemivariational inequalities and related optimal control, we refer to [1, 8, 10, 11, 18, 19, 21,22,23] and the references therein.
The goal of this paper is to study the optimal control for time-dependent variational–hemivariational inequalities. Based on the existence, uniqueness and boundedness of the solution to the inequality (see [10, 18]), we deliver some dependence results with respect to the time when the constraints have different forms in which the Mosco convergence is involved. Moreover, an existence result for an optimal control problem is presented. It is worth pointing out that there are several novelties of the present paper. On the one hand, we consider the constraint sets depending on the time in the inequality problem, which is first investigated, and this study develops the theory of variational–hemivariational inequalities. On the other hand, we obtain that if \(t_n\rightarrow \overline{t}\) in \({\mathbb {R}}_+\), then \(u(t_n)\rightarrow u(\overline{t})\) in X, when the constraint set K(t) has different forms. Finally, we illustrate the abstract result to a semipermeability problem and a quasistatic frictional contact problem.
The rest of this paper is organized as follows: In Sect. 2, we review some of the standard facts which are used in the theory of variational and hemivariational inequalities. An existence and uniqueness result is given at the end of the section. Section 3 is first devoted to the proofs of continuous dependence results for the time-dependent variational–hemivariational inequality. An optimal control problem is then considered. In the last section, we apply the main results in Sect. 3 to a semipermeability problem and a quasistatic frictional contact problem.
2 Preliminaries
Let \((X, \Vert \cdot \Vert _{X})\) be a Banach space. We denote by \(X^{*}\) its dual space and by \(\langle \cdot ,\cdot \rangle _{X}\) the duality pairing between \(X^{*}\) and X. Let \(C({\mathbb {R}}_{+};X)\) be the space of continuous functions defined on \(\mathbb {R}_+\) with values in X.
Definition 2
A function \(f :X \rightarrow {\mathbb {R}}\) is said to be lower semicontinuous (l.s.c.) at u, if for any sequence \(\{u_{n}\}_{n\ge 1}\subset X\) with \(u_{n}\rightarrow u\), we have \(f(u) \le \liminf f(u_{n})\). A function f is said to be l.s.c. on X, if f is l.s.c. at every \(u \in X\).
Definition 3
[2, 4] Let \(\varphi :X \rightarrow \mathbb {R}\cup \{ +\infty \}\) be a proper, convex and l.s.c. function. The mapping \(\partial \varphi :X \rightarrow 2^{X^{*}}\) defined by
for \(u \in X\) is called the subdifferential of \(\varphi \). An element \(u^{*} \in \partial \varphi (u)\) is called a subgradient of \(\varphi \) in u.
Definition 4
[2, 4] Given a locally Lipschitz function \(\varphi :X \rightarrow {\mathbb {R}}\), we denote by \(\varphi ^{0}(u;v)\) the (Clarke) generalized directional derivative of \(\varphi \) at the point \(u\in X\) in the direction \(v\in X\) defined by
The generalized gradient of \(\varphi \) at \(u\in X\), denoted by \(\partial \varphi (u)\), is a subset of \(X^{*}\) given by
Definition 5
[4, 12] Let \(K,K_n(n\in \mathbb {N}) \subset X\) be nonempty subsets. We say that \(K_n\) converge to K in the Mosco sense, as \(n\rightarrow \infty \), denoted by \(K_n \ {\mathop {\longrightarrow }\limits ^{M}} \ K\) if and only if the two conditions hold:
-
(m1)
for each \(u\in K\), there exists \(\{u_n\}_{n\in {\mathbb {N}}}\) such that \(u_n\in K_n\) and \(u_n\rightarrow u\) in X as \(n\rightarrow \infty \),
-
(m2)
for each subsequence \(\{u_n\}_{n\in {\mathbb {N}}}\) such that \(u_n\in K_n\) and \(u_n\rightharpoonup u\) in X, we have \(u\in K\).
At the end of this section, we provide a result on existence, uniqueness and boundedness of solution to the variational–hemivariational inequality.
Problem 6
Find \(u \in K\) such that
Theorem 7
[10, 18] Assume that (2), (3), (4), (5), (6) hold and the following smallness condition is satisfied:
Then for any \(f\in X^{*}\), Problem 6 has a unique solution \(u\in K\). Moreover, u satisfies the following estimate:
3 Optimal Control
In this section we study the dependence of the solution to Problem 1 with respect to the time t and an optimal control problem. In the following, we will provide two dependence results.
At first, we consider the following hypotheses on the data of Problem 6:
The following result concerns the first dependence result to Problem 1.
Theorem 8
Assume that (2), (5), (6), (9), (10), (11) hold and the following smallness condition is satisfied:
Then, for every \(t\in {\mathbb {R}}_+\), Problem 1 has a unique solution \(u(t)\in K(t)\) and
Moreover, suppose also that (12), (13), (14) hold. If \(t_n\rightarrow \overline{t}\) in \({\mathbb {R}}_+\), then \(u(t_n)\rightarrow u(\overline{t})\) in X.
Proof
The existence and boundedness of solutions to Problem 1 can be deduced from Theorem 7.
Now, we prove the dependence result.
Let \(t_n,\overline{t}\in {\mathbb {R}}_+\) and \(t_n\rightarrow \overline{t}\) as \(n\rightarrow +\infty \). Let \(u_n = u(t_n) \in K(t_n)\) be the unique solution to Problem 1 corresponding to \(t_n\), i.e.,
It follows from (16) that \(\{ u_n \}\) is a bounded sequence in X. Therefore, by the reflexivity of X, passing to a subsequence if necessary, \(u_{n}\rightharpoonup \overline{u}\) in X as \(n \rightarrow \infty \) for some \(\overline{u} \in X\). We will show that \(\overline{u}=u(\overline{t})\) is the solution to Problem 1.
As \(u_n \in K(t_n)\) and \(K(t_n) \ {\mathop {\longrightarrow }\limits ^{M}} \ K(\overline{t})\), we have \(\overline{u} \in K(\overline{t})\). Moreover, we can find a sequence \(\{u'_n\}\) such that \(u'_n\in K(t_n)\) and \(u_n\rightarrow \overline{u}\) in X, as \(n \rightarrow \infty \). We set \(v=u'_n\) in (17), and obtain
Using hypotheses (13), (14), we have
It is well known that a monotone Lipschitz continuous operator is pseudomonotone, and hence, (11) implies that \(A(t,\cdot )\) is pseudomonotone for all \(t\in \mathbb {R}_+\). Therefore, we infer
Subsequently, we will pass to the limit in (17). Let \(w \in K(\overline{t})\). From (m1) in Definition 5, we find a sequence \(\{w_n\}\) such that \(w_n\in K(t_n)\) and \(w_n\rightarrow w\) in X, as \(n \rightarrow \infty \). Setting \(v=w_n\) in (1) we obtain
Then, we have
Since \(w \in K(\overline{t})\) is arbitrary, we obtain that
which implies that \(\overline{u} \in K(\overline{t})\) solves Problem 1. Since the solution of Problem 1 is unique, every subsequence \(\{ u_n \}\) converges weakly to the same limit, and hence, the whole original sequence \(\{ u_n \}\) converges weakly to \(\overline{u}=u(\overline{t}) \in K(t)\).
Finally, we show that \(u_n\rightarrow \overline{u}\), as \(n\rightarrow \infty \). Since \(K(t_n) \ {\mathop {\longrightarrow }\limits ^{M}} \ K(\overline{t})\) as \(n\rightarrow \infty \), we can find a sequence \(\{\tilde{u}_n \}\), \(\tilde{u}_n \in K(t_n) \) such that \(\tilde{u}_n \rightarrow \overline{u}\), as \(\rho \rightarrow 0\). Choosing \(v=\tilde{u}_n \) in (17), we have
Passing to the upper limit in the last inequality, as \(n\rightarrow \infty \), and exploiting (11), (13), (14), we deduce \(\limsup \Vert u_n-\tilde{u}_n\Vert _{X}^{2}\le 0\). Hence, we obtain \(\Vert u_n-\tilde{u}_n\Vert _{X}\rightarrow 0\). Therefore, we have
which implies that \(u_n\rightarrow \overline{u}\) in X, as \(\rho \rightarrow 0\). This completes the proof. \(\square \)
Next, we consider the constraint sets K(t) and function \(\varphi \) which satisfy the following hypotheses:
Remark 9
We observe that if K(t), for \(t > 0\), is defined by (18), then \(K(t_n) \rightarrow K(t)\) in the sense of Mosco, as \(t_n \rightarrow t\), see [12].
Next, we give the second dependence result to Problem 1.
Theorem 10
Assume that (2), (5), (6), (10), (11), (15), (18), (19) are satisfied. If \(t_n\rightarrow \overline{t}\) in \({\mathbb {R}}_+\), then \(u(t_n)\rightarrow u(\overline{t})\) in X.
Proof
Let \(t,t_n\in {\mathbb {R}}_+\) and \(t_n\rightarrow t\) as \(n\rightarrow +\infty \). We have
By the definition of \(K(t_n)\), we get \(\frac{u(t_n)-d(t_n)\theta }{c(t_n)}\in K\). Let \(c_n=\frac{c(t)}{c(t_n)}\). Taking \(v=c_n (u(t_n)-d(t_n)\theta )+d(t)\theta \in K(t)\) in (20) we obtain
Taking \(v_n=\frac{1}{c_n}(u(t)-d(t)\theta )+d(t_n)\theta \in K(t_n)\) in (21) and multiplying by \(c_n \), we obtain
Adding the above two inequalities, we deduce that
From (5)(c) and (d), we have
By using the identity
we obtain
Moreover, it follows from (6)(b) that
Hence,
From (16), it follows that there exists a constant \(k>0\) such that \(\Vert u(t_n)\Vert _X\le k\) and \(\Vert u(t)\Vert _X\le k\) for sufficiently large n. Then, there exists a constant \(N_k>0\) such that
Then, we have
From the following fact
it follows that
Since \(c(t_n)\rightarrow c(t)\), \(d(t_n)\rightarrow d(t)\) and \(f(t_n)\rightarrow f(t)\) as \(n\rightarrow +\infty \), we deduce that the right hand of the above inequality tends to 0 as \(n\rightarrow +\infty \), and hence, \(u(t_n)\rightarrow u(t)\) as \(n\rightarrow +\infty \). Therefore, we obtain that \(u\in C({\mathbb {R}}_+;X)\). \(\square \)
Remark 11
We observe that if \(d(t)=0\) for all \(t\in \mathbb {R}_+\) in (18), then from the proof of the above theorem, we can omit the condition (13).
We consider the following special case.
Problem 12
Find \(u:{\mathbb {R}}_{+} = [0, +\infty )\rightarrow X\) such that, for all \(t\in {\mathbb {R}}_{+}\), \(u(t)\in K\) and
The following result is a consequence of Theorem 10.
Theorem 13
Assume that (2), (5), (6), (10), (11), (15), (19) are satisfied. If \(t_n\rightarrow \overline{t}\) in \({\mathbb {R}}_+\), then \(u(t_n)\rightarrow u(\overline{t})\) in K.
Finally, we provide an existence result for an optimal control problem governed by Problem 1.
Consider a closed interval \([a,b]\subset {\mathbb {R}}_+\) and a cost functional \(F :[a,b]\times X \rightarrow \mathbb {R}\), and find a solution \(t^{*}\in [a,b]\) to the following problem:
where \(u = u(t) \in K(t)\) denotes the unique solution of Problem 1 corresponding to the time t.
We are now in a position to state the main result on the existence of solutions to problem (23). We admit the following hypothesis:
Theorem 14
Assume all the hypotheses of Theorem 8 or Theorem 10 are satisfied. If (24) holds, then the problem (23) has at least one solution.
Proof
Let \(\{( t_n,u_{n})\}\subset [a,b]\times X\) be a minimizing sequence of the functional F, i.e.,
where \(t_{n}\in [a,b]\) and \(u_{n} \in K(t_n)\) is the unique solution of Problem 1 that corresponds to \(t_n\), i.e., \(u_{n}=u(t_n)\). It is clear that \(\{ t_n \}\) is bounded. Then, there is a subsequence of \(\{ t_n \}\), denoted in the same way, such that \(t_n \rightarrow {\overline{t}}\) for some \({\overline{t}}\in [a,b]\). From Theorem 8 or Theorem 10, we infer that the sequence \(\{ u_n \} \subset K(t_n)\) converges weakly in X to the unique solution \(u({\overline{t}}) \in K({\overline{t}})\) of Problem 1. Finally, from (24), we have
which shows that \(\overline{t}\) is a solution of the problem (23). This completes the proof. \(\square \)
4 Applications
4.1 Semipermeability Problem
In this part we consider a semipermeability problem (see [3, 14,15,16]) to illustrate our main results of Sect. 3.
Let \(\Omega \) be a bounded domain of \(\mathbb {R}^d\) with Lipschitz continuous boundary \(\partial \Omega = \Gamma \) which consists of two disjoint measurable parts \(\Gamma _{1}\) and \(\Gamma _{2}\) such that \(m(\Gamma _{1}) > 0\). Consider the following semipermeability problem.
Problem 15
Find a temperature \(u :\Omega \times {\mathbb {R}}_{+} \rightarrow {\mathbb {R}}\) such that
The description of Problem 15 can be found in [23] when U is independent of t.
We introduce the following spaces:
Since \(m(\Gamma _{1}) > 0\), on V we can consider the norm \(\Vert v \Vert _V = \Vert \nabla v\Vert _{L^2(\Omega )^d}\) for \(v \in V\) which is equivalent on V to the \(H^1(\Omega )\) norm. By \(\gamma :V \rightarrow L^2(\Gamma )\) we denote the trace operator which is known to be linear, bounded and compact. Moreover, by \(\gamma v\) we denote the trace of an element \(v \in H^1(\Omega )\).
We need the following hypotheses study Problem 15:
By standard procedure, we obtain the variational formulation of Problem 15 with the following form.
Problem 16
Find \(u:{\mathbb {R}}_+\rightarrow V\) such that for all \(t\in {\mathbb {R}}_+\), \(u(t)\in U(t)\) and
for all \(v \in U(t)\).
Theorem 17
Assume that (31)–(35) hold and the following smallness condition is satisfied:
Then, Problem 16 has a unique solution \(u \in C({\mathbb {R}}_{+};V)\).
Proof
We can apply Theorem 7 in the following functional framework: \(X=V\), \(K=U\), \(f(t) = f_1(t)\) for all \(t \in \mathbb {R}_+\) and
From the proof of [23, Theorem 32], the operator A and functions \(\varphi \) and j satisfy hypotheses (11), (5) and (6) with \(\alpha _{A1}=\alpha _a\), \(\alpha _{\varphi }=L_k L_g\Vert \gamma \Vert ^2\) and \(\alpha _j = \alpha _h\), respectively. \(\square \)
We conclude this part with the following example.
Example 18
Hypothesis (12) is satisfied for the following constraint sets for a bilateral obstacle problem:
where \(\psi _1,\psi _2 \in C({\mathbb {R}}_+;V)\). It is clear that for every \(t\in {\mathbb {R}}_+\), U(t) is closed convex subset of V. We will show that
In fact, let \(v_n\in U(t_n)\) be such that \(v_n\rightharpoonup v\) in V, as \(n\rightarrow \infty \). Since
we obtain \(v_n-\psi _{1}(t_n)\in \{ \, z \in V \mid z \ge 0 \ \ \text{ a.e. } \text{ in } \ \ \Omega \,\}\) and \(v_n-\psi _{2}(t_n)\in \{ \, z \in V \mid z \le 0 \ \ \text{ a.e. } \text{ in } \ \ \Omega \,\}\). Moreover, since the sets \(\{ \, z \in V \mid z \ge 0 \ \ \text{ a.e. } \text{ in } \ \ \Omega \,\}\) and \(\{ \, z \in V \mid z \le 0 \ \ \text{ a.e. } \text{ in } \ \ \Omega \,\}\) are weakly closed by Mazur’s theorem, we deduce that \(v-\psi _{1}(t)\in \{ \, z \in V \mid z \ge 0\ \ \text{ a.e. } \text{ in } \ \ \Omega \,\}\) and \(v-\psi _{2}(t)\in \{ \, z \in V \mid z \le 0 \ \ \text{ a.e. } \text{ in } \ \ \Omega \,\}\), and hence, \(v\in U(t)\).
On the other hand, for any \(v \in U(t)\), there exist \(v_1\in \{ \, z \in V \mid z \ge 0 \ \ \text{ a.e. } \text{ in } \ \ \Omega \,\}\) and \(v_2\in \{ \, z \in V \mid z \le 0 \ \ \text{ a.e. } \text{ in } \ \ \Omega \,\}\) such that \({v}=v_1+\psi _{1}(t)=v_2+\psi _{2}(t)\).
Since \(\psi _1,\psi _2 \in C({\mathbb {R}}_+;V)\), it is clear that \((\psi _{1}(t_n), \psi _{2}(t_n))\rightarrow (\psi _{1}(t), \psi _{2}(t))\) in \(V\times V\). Put \(v_n=v_1+\psi _{1}(t_n)\). Then, for n large enough, we get \(v_n\in U(t_n)\). Hence, \(v_n=v_1+\psi _{1}(t_n)\rightarrow v_1+\psi _{1}(t)=v_2+\psi _{2}(t) = v\) in V. Therefore, the convergence (40) holds.
4.2 Quasistatic Frictional Contact Problem
In this part, we consider a quasistatic frictional contact problem which variational formulation is a time-dependent variational–hemivariational inequality. For more frictional contact problems, we refer to [5,6,7, 13].
An elastic body occupies an open, bounded and connected set \(\Omega \subset {\mathbb {R}}^{d}\), \(d=1\), 2, 3. The boundary of \(\Omega \) is denoted by \(\Gamma =\partial \Omega \) and it is assumed to be Lipschitz continuous. We also suppose that \(\Gamma \) consists of three mutually disjoint and measurable parts \(\overline{\Gamma }_{1}\), \(\overline{\Gamma }_{2}\) and \(\overline{\Gamma }_{3}\) such that \(\mathrm{meas}\,(\Gamma _{1}) > 0\). Let \({\varvec{\nu }}= (\nu _i)\) be the outward unit normal at \(\Gamma \) and let \(\mathbb {S}^{d}\) be the space of second order symmetric tensors on \({\mathbb {R}}^{d}\). For a vector field, notation \(u_{\nu }\) and \({\varvec{u}}_{\tau }\) represent the normal and tangential components of \({\varvec{u}}\) on \(\Gamma \) given by \(u_{\nu }={\varvec{u}}\cdot {\varvec{\nu }}\) and \({\varvec{u}}_{\tau }={\varvec{u}}-u_{\nu }{\varvec{\nu }}\). Also, \(\sigma _{\nu }\) and \({\varvec{\sigma }}_{\tau }\) represent the normal and tangential components of the stress field \({\varvec{\sigma }}\) on the boundary, i.e., \(\sigma _{\nu }=({\varvec{\sigma }}{\varvec{\nu }})\cdot {\varvec{\nu }}\) and \({\varvec{\sigma }}_{\tau } ={\varvec{\sigma }}{\varvec{\nu }}-\sigma _{\nu }{\varvec{\nu }}\).
The classical model for the quasistatic frictional contact problem is as follows:
Problem 19
Find a displacement field \({\varvec{u}}:\Omega \times {\mathbb {R}}_{+} \rightarrow {\mathbb {R}}^{d}\), a stress field \({\varvec{\sigma }}:\Omega \times {\mathbb {R}}_{+} \rightarrow \mathbb {S}^{d}\) and an interface force \(\eta :\Gamma _{3}\times {\mathbb {R}}_{+} \rightarrow {\mathbb {R}}\) such that
The description of Problem 19 can be found in [9, 10, 20] for fixed \(t\in {\mathbb {R}}_{+}\).
We will use the spaces V and \({\mathcal {H}}\) defined by
The space \({\mathcal {H}}\) will be endowed with the Hilbertian structure given by the inner product
and the associated norm \(\Vert \cdot \Vert _{\mathcal {H}}\). On the space V we consider the inner product and the corresponding norm given by
Let \(\gamma :V\rightarrow L^{2}(\Gamma ;{\mathbb {R}}^{d})\) be the trace operator. By the Sobolev trace theorem, we have
We need the following hypotheses on the data of Problem 19:
We also assume that the densities of body forces and surface tractions satisfy
We introduce the set of admissible displacement fields U(t) for \(t\in {\mathbb {R}}_+\) defined by
and define an element \({\varvec{f}}:{\mathbb {R}}_{+}\rightarrow V^{*}\) by
for all \({\varvec{v}}\in V\), \(t\in {\mathbb {R}}_{+}\).
The variational formulation of Problem 19 has the following form.
Problem 20
Find \({\varvec{u}}:{\mathbb {R}}_+\rightarrow V\) such that, for all \(t\in {\mathbb {R}}_+\), \(u(t)\in U(t)\) and
Theorem 21
Assume that (48), (49), (50) hold and the following smallness condition is satisfied:
Then, Problem 20 has a unique solution \({\varvec{u}}\in C({\mathbb {R}}_{+};V)\).
Proof
We apply Theorem 10 in the following functional framework: \(X=V\), \(K(t)=U(t)\) and
For any \(g_0>0\), let
Then, \(K=\frac{g_0}{g(t)}K(t)\) and (18) is obvious with \(c_1(t)=c_2(t)=\frac{g_0}{g(t)}\) and \(d_1(t)=d_2(t)=0\).
From the proof of [10, Theorem 32], the operator A and functions \(\varphi \) and j satisfy hypotheses (11), (5) and (6) with \(\alpha _{A1}=\alpha _{{\mathcal {A}}}\), \(\alpha _{\varphi }=L_{F_b} \Vert \gamma \Vert ^2\) and \(\alpha _j = \alpha _{j_\nu } \Vert \gamma \Vert ^2\), respectively. From Remark 11, we complete the proof. \(\square \)
References
Benraouda, A., Sofonea, M.: A convergence result for history-dependent quasivariational inequalities. Appl. Anal. 96, 2635–2651 (2017)
Clarke, F.H.: Optimization and Nonsmooth Analysis. Wiley, New York (1983)
Duvaut, G., Lions, J.-L.: Inequalities in Mechanics and Physics. Springer, Berlin (1976)
Denkowski, Z., Migórski, S., Papageorgiou, N.S.: An Introduction to Nonlinear Analysis: Theory. Kluwer Academic, Boston (2003)
Han, J.F., Migórski, S.: A quasistatic viscoelastic frictional contact problem with multivalued normal compliance, unilateral constraint and material damage. J. Math. Anal. Appl. 443, 57–80 (2016)
Han, W.M., Sofonea, M.: Quasistatic Contact Problems in Viscoelasticity and Viscoplasticity. Studies in Advanced Mathematics, vol. 30. International Press, Providence (2002)
Han, W., Migórski, S., Sofonea, M.: A class of variational–hemivariational inequalities with applications to frictional contact problems. SIAM J. Math. Anal. 46, 3891–3912 (2014)
Jiang, C.J., Zeng, B.: Continuous dependence and optimal control for a class of variational–hemivariational inequalities. Appl. Math. Optim. 82, 637–656 (2020)
Migórski, S., Ochal, A., Sofonea, M.: Nonlinear Inclusions and Hemivariational Inequalities: Models and Analysis of Contact Problems. Springer, New York (2013)
Migórski, S., Ochal, A., Sofonea, M.: A class of variational–hemivariational inequalities in reflexive Banach spaces. J. Elast. 127, 151–178 (2017)
Migorski, S., Zeng, B.: On convergence of solutions to history-dependent variational–hemivariational inequalities. J. Math. Anal. Appl. 471, 496–518 (2019)
Mosco, U.: Convergence of convex sets and of solutions of variational inequalities. Adv. Math. 3, 510–585 (1969)
Motreanu, D., Sofonea, M.: Quasivariational inequalities and applications in frictional contact problems with normal compliance. Adv. Math. Sci. Appl. 10, 103–118 (2000)
Naniewicz, Z., Panagiotopoulos, P.D.: Mathematical Theory of Hemivariational Inequalities and Applications. Marcel Dekker, New York (1995)
Panagiotopoulos, P.D.: Nonconvex problems of semipermeable media and related topics. Z. Angew. Math. Mech. 65, 29–36 (1985)
Panagiotopoulos, P.D.: Inequality Problems in Mechanics and Applications. Convex and Nonconvex Energy Functions. Birkhäuser, Basel (1985)
Panagiotopoulos, P.D.: Hemivariational Inequalities, Applications in Mechanics and Engineering. Springer, Berlin (1993)
Sofonea, M.: Optimal control of a class of variational–hemivariational inequalities in reflexive Banach spaces. Appl. Math. Optim. 79, 621–646 (2019)
Sofonea, M., Benraouda, A.: Convergence results for elliptic quasivariational inequalities. Z. Angew. Math. Phys. 68, 10 (2017)
Sofonea, M., Matei, A.: Mathematical Models in Contact Mechanics. London Mathematical Society, Lecture Note Series 398. Cambridge University Press, Cambridge (2012)
Sofonea, M., Migórski, S.: A class of history-dependent variational–hemivariational inequalities. Nonlinear Differ. Equ. Appl. 23, 38 (2016)
Zeng, B., Migórski, S.: Variational–hemivariational inverse problems for unilateral frictional contact. Appl. Anal. 23(2), 293–312 (2020)
Zeng, B., Liu, Z.H., Migórski, S.: On convergence of solutions to variational–hemivariational inequalities. Z. Angew. Math. Phys. 69, 87 (2018)
Funding
The work was supported by the Natural Science Foundation of Guangxi Province (No. 2019GXNSFBA185005), the Start-up Project of Scientific Research on Introducing talents at school level in Guangxi University for Nationalities (No. 2019KJQD04) and the Xiangsihu Young Scholars Innovative Research Team of Guangxi University for Nationalities (No. 2019RSCXSHQN02).
Author information
Authors and Affiliations
Contributions
The author read and approved the final manuscript.
Corresponding author
Ethics declarations
Conflict of interests
The author declares to have no competing interests.
Additional information
Communicated by Rosihan M. Ali.
Publisher's Note
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Rights and permissions
About this article
Cite this article
Zeng, B. Optimal Control for Time-Dependent Variational–Hemivariational Inequalities. Bull. Malays. Math. Sci. Soc. 44, 1961–1977 (2021). https://doi.org/10.1007/s40840-020-01042-2
Received:
Revised:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s40840-020-01042-2
Keywords
- Time-dependent variational–hemivariational inequality
- Optimal control
- Continuous dependence
- Constraint set
- Semipermeability problem
- Quasistatic frictional contact problem