Freezing influence on the histological structure of Mediterranean mussel (<i>Mytilus galloprovincialis</i>)

Mariyana Strateva; Deyan Stratev; Georgi Zhelyazkov; Mariyana Strateva; Deyan Stratev; Georgi Zhelyazkov

doi:10.3934/agrfood.2023015

AIMS Agriculture and Food

2023, Volume 8, Issue 2: 278-291. doi: 10.3934/agrfood.2023015

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Research article

Freezing influence on the histological structure of Mediterranean mussel (Mytilus galloprovincialis)

1.
Department of Veterinary Anatomy, Histology and Embryology, Faculty of Veterinary Medicine, Trakia University, 6000 Stara Zagora, Bulgaria
2.
Department of Food Quality and Safety and Veterinary Legislation, Faculty of Veterinary Medicine, Trakia University, 6000 Stara Zagora, Bulgaria
3.
Department of Animal husbandry–Non-ruminants and other animals, Faculty of Agriculture, Trakia University, 6000 Stara Zagora, Bulgaria

Received: 18 November 2022 Revised: 20 February 2022 Accepted: 21 February 2023 Published: 01 March 2023

The objective of this study was to establish the morphological changes in the structure of Mediterranean mussel (Mytilus galloprovincialis) after frozen storage. Two hundred Mediterranean mussels (M. galloprovincialis) were collected from the Black Sea coastal waters. Forty mussels were subjected to histological analysis in fresh state. The remaining 160 mussels were divided into 4 groups and slowly frozen in a conventional freezer at −18 ℃ and subsequently stored at the same temperature for 3, 6, 9 and 12 months, respectively. The histological assessment of posterior adductor muscle and foot found a change in their morphological profile and overall structure. The fewest changes in the histostructure were recorded after a 3-month period and the most after a 12-month period of storage in frozen state. The results from that study can be used as an unambiguous marker in selecting optimum conditions for storage of mussels in frozen state.

Keywords:

Citation: Mariyana Strateva, Deyan Stratev, Georgi Zhelyazkov. Freezing influence on the histological structure of Mediterranean mussel (Mytilus galloprovincialis)[J]. AIMS Agriculture and Food, 2023, 8(2): 278-291. doi: 10.3934/agrfood.2023015

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Abstract

1. Introduction

In structural mechanics, particularly in the field of elasticity, there are equations that describe the behavior of thin plates under loads. These equations are often partial differential equations that govern the displacement of a thin plate. The plate equation depends on factors like material properties, geometry, and boundary conditions. In the context of geophysics, "plate equation" could refer to the equations that describe the movement and interaction of tectonic plates on the Earth's surface. Plate tectonics is a theory that explains the movement of the Earth's lithosphere (the rigid outer layer of the Earth) on the more fluid asthenosphere beneath it. In mathematics, specifically in the field of differential equations, the term "plate equation" might be used to refer to certain types of equations. For instance, in polar coordinates, Laplace's equation takes a specific form that is sometimes informally referred to as the "plate equation". Plate equation models are hyperbolic systems that arise in several areas in real-life problems, (see, for instance, Kizilova et al.^[1], Lasiecka et al. ^[2] and Huang et al.^[3]). The theory of plates is the mathematical formulation of the mechanics of flat plates. It is defined as flat structural components with a low thickness compared to plane dimensions. The advantage of the theory of plates comes from the disparity of the length scale to reduce the problem of the mechanics of three-dimensional solids to a two-dimensional problem. The purpose of this theory is to compute the stresses and deformation in a loaded plate. The equation of plates results from the composition of different subsets of plates: The equilibrium equations, constitutive, kinematic, and force resultant, ^[4,5,6].

Following this, there are a wide number of works devoted to the analysis and control of the academic model of hyperbolic systems, the so-called plate equations, For example, the exact and the approximate controllability of thermoelastic plates given by Eller et al. ^[7] and Lagnese and Lions in ^[8] treated the control of thin plates and Lasiecka in ^[9] considered the controllability of the Kirchoff plate. Zuazua ^[10] treated the exact controllability for semi-linear wave equations. Recently many problems involving a plate equations were considered by researchers. Let us cite as examples the stabilization of the damped plate equation under general boundary conditions by Rousseau an Zongo ^[11]; the null controllability for a structurally damped stochastic plate equation studied by Zhao ^[12], Huang et al. ^[13] considerrd a thermal equation of state for zoisite: Implications for the transportation of water into the upper mantle and the high-velocity anomaly in the Farallon plate. Kaplunov et al. ^[14] discussed the asymptotic derivation of 2D dynamic equations of motion for transversely inhomogeneous elastic plates. Hyperbolic systems have recently continued to be of interest to researchers and many results have been obtained. We mention here the work of Fu et al. ^[15] which discusses a class of mixed hyperbolic systems using iterative learning control. Otherwise, for a class of one-dimension linear wave equations, Hamidaoui et al. stated in ^[16] an iterative learning control. Without forgetting that for a class of second-order nonlinear systems Tao et al. proposed an adaptive control based on an disturbance observer in ^[17] to improve the tracking performance and compensation. In addition to these works, the optimal control of the Kirchoff plate using bilinear control was considered by Bradly and Lenhart in ^[18], and Bradly et al. in ^[19]. In fact, in this work we will talk about a bilinear plate equation and we must cite the paper of Zine ^[20] which considers a bilinear hyperbolic system using the Riccati equation. Zine and Ould Sidi ^[19,22] that introduced the notion of partial optimal control of bilinear hyperbolic systems. Li et al. ^[23] give an iterative method for a class of bilinear systems. Liu, et al. ^[24] extended a gradient-based iterative algorithm for bilinear state-space systems with moving average noises by using the filtering technique. Furthermore, flow analysis of hyperbolic systems refers to the problems dealing with the analysis of the flow state on the system domain. We can refer to the work of Benhadid et al. on the flow observability of linear and semilinear systems ^[25], Bourray et al. on treating the controllability flow of linear hyperbolic systems ^[26] and the flow optimal control of bilinear parabolic systems are considered by Ould Sidi and Ould Beinane on ^[27,28].

For the motivation the results proposed in this paper open a wide range of applications. We cite the problem of iterative identification methods for plate bilinear systems ^[23], as well as the problem of the extended flow-based iterative algorithm for a plate systems ^[24].

This paper studies the optimal control problem governed by an infinite dimensional bilinear plate equation. The objective is to command the flow state of the bilinear plate equation to the desired flow using different types of bounded feedback. We show how one can transfer the flow of a plate equation close to the desired profile using optimization techniques and adjoint problems. As an application, we solve the partial flow control problem governed by a plate equation. The results open a wide way of applications in fractional systems. We began in section two by the well-posedness of our problem. In section three, we prove the existence of an optimal control solution of (2.3). In section four, we state the characterization of the optimal control. In section five we debate the case of time bilinear optimal control. Section six, proposes a method for solving the flow partial optimal control problem governed by a plate equation.

2. Well-posedness of the problem

Consider $\Theta$ an open bounded domain of $I\!\!R^2$ with $C^2$ boundary, for a time $m$ , and $\Gamma = \partial\Theta \times (0, m)$ . The control space time set is such that

$\begin{equation} Q \in U_{p} = \{ Q\in L^{\infty}([0,m];L^{\infty}(\Theta)){\mbox{ such that }} -p\leq Q(t) \leq p\}, \end{equation}$

(2.1)

with $p$ as a positive constant. Let the plate bilinear equation be described by the following system

$\begin{equation} \left \{ \begin{array}{lll} {\frac{{\partial }^2 {u} }{{\partial t}^2} } + \Delta^{2} u = Q(t)u_{t}, & & (0,m) \times \Theta, \\ u(x,0) = u_0(x) ,\; {\frac{{\partial } u }{{\partial t}} } (x,0) = u_1(x), & & \Theta,\\ u = \frac{\partial u}{\partial \nu} = 0, & & \Gamma, \end{array} \right. \end{equation}$

(2.2)

where $u_{t} = \frac{\partial u}{\partial t}$ is the velocity. The state space is $H_{0}^{2}(\Theta)\times L^{2}(\Theta)$ , (see Lions and Magenes ^[29] and Brezis ^[30]). We deduce the existence and uniqueness of the solution for (2.2) using the classical results of Pazy ^[31]. For $\lambda > 0$ , we define $\nabla u$ as the flow control problem governed by the bilinear plate equation (2.2) as the following:

$\begin{equation} \min\limits_{Q\ \in U_{p} }C_{\lambda}(Q), \end{equation}$

(2.3)

where $C_{\lambda}$ , is the flow penalizing cost defined by

$\begin{align} C_{\lambda}(Q) = \frac{1}{2}\Big\|\nabla u-u^{d}\Big\|^{2}_{(L^2(0,m;L^2(\Theta)))^{n}} + \frac{\lambda}{2}\int_{0}^{m} \int_{\Theta} Q^2(x,t)dxdt\\ = \frac{1}{2}\sum\limits_{i = 1}^{n} \Big\|\frac{\partial u}{\partial x_{i}} - u_{i}^{d}\Big\|^{2}_{L^2(0,m;L^2(\Theta))} + \frac{\lambda}{2}\int_{0}^{m} \int_{\Theta} Q^2(x,t)dxdt, \end{align}$

(2.4)

where $u^d = (u_{1}^{d}, ....u_{n}^{d})$ is the flow target in $L^2(0, m;L^2(\Theta))$ . One of the important motivations when considering the problem (2.3) is the isolation problems, where the control is maintained to reduce the flow temperature on the surface of a thin plate (see El Jai et al. ^[32]).

3. Existence of solution

Lemma 3.1. If $(u_{0}, u_{1}) \in H_{0}^{2}(\Theta)\times L^{2}(\Theta)$ and $Q \in U_{p}$ , then the solution $(u, u_{t})$ of (2.2) satisfies the following estimate:

$\Big\| (u, u_{t}) \Big\|_{{\cal C}(0,m; H_{0}^{2}(\Theta)\times L^{2}(\Theta))} \leq T (1+ \eta m)e^{\eta K m},$

where $T = \Big\| (u_{0}, u_{1}) \Big\|_{ H_{0}^{2}(\Theta)\times L^{2}(\Theta)}$ and $K$ is a positive constant ^[18,19].

Using the above Lemma 3.1, we prove the existence of an optimal control solution of (2.3).

Theorem 3.1. $(u^{*}, Q^*)\in {\cal C}([0, m];\; \; H_{0}^{2}(\Theta)\times U_{p})$ , is the solution of (2.3), where $u^{*}$ is the output of (2.2) and $Q^*$ is the optimal control function.

Proof. Consider the minimizing sequence $(Q_{n})_{n}$ in $U_{p}$ verifying

$C^{*} = \lim\limits_{n\rightarrow +\infty}C_{\lambda}(Q_n) = \inf\limits_{Q\in L^{\infty}(0,m; L^{\infty}(\Theta))} C_{\lambda}(Q).$

We choose $\bar{u}^{n} = (u^{n}, \frac{\partial u^{n}}{\partial t})$ to be the corresponding state of Eq (2.2). Using Lemma 3.1, we deduce

$\begin{equation} \Big\| u^{n}(x,t) \Big\|_{H_{0}^{2}(\Theta)}^{2} + \Big\| u_{t}^{n} (x,t) \Big\|_{ L^{2}(\Theta)}^{2} \leq T_{1} e^{\eta K m} {\mbox{ for }} 0\leq t\leq m {\mbox{ and }} T_{1}\in I\!\!R^{+}. \end{equation}$

(3.1)

Furthermore, system (2.2) gives

$\Big\| u^{n}_{tt}(x,t) \Big\|_{H^{-2}(\Theta)}^{2} \leq T_{2} \Big\| u_{t}^{n} (x,t) \Big\|_{ L^{2}(\Theta)}^{2} {\mbox{ with }} T_{2}\in I\!\!R^{+}.$

Then easily from (3.1), we have

$\begin{equation} \Big\| u^{n}_{tt}(x,t) \Big\|_{H^{-2}(\Theta)}^{2} \leq T_{3} e^{\eta K m} {\mbox{ for }} 0\leq t\leq m {\mbox{ and }} T_{3}\in I\!\!R^{+}. \end{equation}$

(3.2)

Using (3.1) and (3.2), we have the following weak convergence:

$\begin{equation} \begin{array}{lll} Q_{n} \rightharpoonup Q^{*}, & & L^{2}(0,m ; L^{2}(\Theta)),\\ u^{n} \rightharpoonup u^{*}, & & L^{\infty}(0,m ; H_{0}^{2}(\Theta)),\\ u_{t}^{n} \rightharpoonup u^{*}_{t}, & & L^{\infty}(0,m ; L^{2}(\Theta)),\\ u_{tt}^{n} \rightharpoonup u^{*}_{tt}, & & L^{\infty}(0,m ; H^{-2}(\Theta)),\\ \end{array} \end{equation}$

(3.3)

From the first convergence property of (3.3) with a control sequence $Q_{n} \in U_{p}$ , easily one can deduce that $Q^{*} \in U_{p}$ ^[20].

In addition, the mild solution of (2.2) verifies

$\begin{align} \int_{0}^{m} u^{n}_{tt}f(t)dt+ \int_{0}^{m} \int_{\Theta}\Delta u^{n} \Delta f(t) dx dt = \int_{0}^{m} Q^{*}u_{t}^{n} f(t)dt, \forall f \in H_{0}^{2}(\Theta). \end{align}$

(3.4)

Using (3.3) and (3.4), we deduce that

$\begin{align} \int_{0}^{m} u^{*}_{tt}f(t)dt+ \int_{0}^{m} \int_{\Theta}\Delta u^{*} \Delta f(t) dx dt = \int_{0}^{m} Q^{*}u_{t}^{*} f(t)dt, \forall f \in H_{0}^{2}(\Theta), \end{align}$

(3.5)

which implies that $u^{*} = u(Q_{*})$ is the output of (2.2) with command function $Q^{*}$ .

Fatou's lemma and the lower semi-continuous property of the cost $C_{\lambda}$ show that

$\begin{align} C_{\lambda}(Q^{*}) \leq \frac{1}{2}\lim\limits_{k\rightarrow +\infty}\Big\|\nabla u^{k}-u^{d}\Big\|^{2}_{(L^2(0,m;L^2(\Theta)))^{n}} + \frac{\lambda}{2}\lim\limits_{k\rightarrow +\infty} \int_{0}^{m} \int_{\Theta} Q_{k}^2(x,t)dxdt\\ \leq \liminf\limits_{k\rightarrow +\infty} C_{\lambda}(Q_{n})\\ = \inf\limits_{Q \in U_{p}} C_{\lambda}(Q), \end{align}$

(3.6)

which allows us to conclude that $Q^{*}$ is the solution of problem (2.3). □

4. Characterization of solution

We devote this section to establish a characterization of solutions to the flow optimal control problem (2.3).

Let the system

$\begin{equation} \left \{ \begin{array}{lll} {\frac{{\partial^{2} } v }{{\partial t^{2}}} } = -\Delta^{2}v(x,t)+Q(x,t) v_{t} + d(x,t) v_{t}, & & (0, m)\times \Theta,\\ v(x,0) = v_{t}(x,0) = v_0(x) = 0, & & \Theta, \\ v = \frac{\partial v}{\partial \nu } = 0, & & \Gamma, \end{array} \right. \end{equation}$

(4.1)

with $d \in L^{\infty}(0, m; L^{\infty}(\Theta))$ verify $Q+\delta d \in U_{p}, \quad \forall \delta > 0$ is a small constant. The functional defined by $Q \in U_{p}\mapsto \bar{u}(Q) = (u, u_{t}) \in {\cal C}(0, m; H_{0}^{2}(\Theta)\times L^{2}(\Theta))$ is differentiable and its differential $\overline{v} = (v, v_{t})$ is the solution of (4.1) ^[21].

The next lemma characterizes the differential of our flow cost functional $C_{\lambda}(Q)$ with respect to the control function $Q$ .

Lemma 4.1. Let $Q \in U_{p}$ and the differential of $C_{\lambda}(Q)$ can be written as the following:

$\begin{align} \lim\limits_{k\longrightarrow 0} \frac{C_{\lambda}(Q+k d)-C_{\lambda}(Q)}{k} = \sum\limits_{i = 1}^{n} \int _{\Theta}\int_{0}^{m} \frac{\partial v(x,t)}{\partial x_{i}}(\frac{\partial u}{\partial x_{i}} - u_{i}^{d} )dtdx+ \varepsilon\int_{\Theta}\int_{0}^{m} d Q dt dx.\\ \end{align}$

(4.2)

Proof. Consider the cost $C_{\lambda}(Q)$ defined by (2.4), which is

$\begin{align} C_{\lambda}(Q) = \frac{1}{2} \sum\limits_{i = 1}^{n}\int_{\Theta}\int_{0}^{m}(\frac{\partial u}{\partial x_{i}} - u_{i}^{d} )^2 dt dx + \frac{\lambda}{2} \int_{\Theta}\int^{m}_{0} Q^2(t) dt dx. \end{align}$

(4.3)

Put $u_{k} = z(Q+k d)$ , $u = u(Q)$ , and using (4.3), we have

$\begin{align} \lim\limits_{k \longrightarrow 0} \frac{C_{\lambda}(Q+k d)-C_{\lambda}(Q)}{k} = \lim\limits_{\beta\longrightarrow 0}\sum\limits_{i = 1}^{n} \frac{1}{2}\int_{\Theta}\int_{0}^{m}\frac{( \frac{\partial u_{k}}{\partial x_{i}} - u_i^d)^{2}-( \frac{\partial u}{\partial x_{i}}-u_i^d)^{2}}{k}dt dx\\ + \lim\limits_{k \longrightarrow 0}\frac{\lambda}{2}\int_{\Theta} \int_{0}^{m}\frac{(Q+k d)^2-Q^2}{k}(t)dt dx. \end{align}$

(4.4)

Consequently

$\begin{align} \lim\limits_{k \longrightarrow 0} \frac{C_{\lambda}(Q +kd)-C_{\lambda}(Q )}{k} \\ = \lim\limits_{k \longrightarrow 0}\sum\limits_{i = 1}^{n}\frac{1}{2}\int_{\Theta}\int^{m}_{0}\frac{( \frac{\partial u_{k}}{\partial x_{i}}- \frac{\partial u}{\partial x_{i}})}{k}( \frac{\partial u_{k} }{\partial x_{i}}+ \frac{\partial u}{\partial x_{i}}-2u_i^d) dt dx \\ + \lim\limits_{k \longrightarrow 0} \int_{\Theta}\int_{0}^{m}(\lambda d Q+ k \lambda d^2)dt dx\\ = \sum\limits_{i = 1}^{n}\int_\Theta \int_{0}^{m}\frac{\partial v(x,t)}{\partial x_{i}}( \frac{\partial u(x,t)}{\partial x_{i}}-u_i^d)dt dx+\int_\Theta \int_{0}^{m}\lambda d Q dt dx. \end{align}$

(4.5)

□ We define the following family of adjoint equations for system (4.1)

$\begin{equation} \left \{ \begin{array}{lll} {\frac{{\partial^{2} } {w_{i}}}{{\partial t^{2}}} } +\Delta^{2} w_{i} = Q^*(x,t) (w_{i})_{t}+( \frac{\partial u}{\partial x_{i}} - u_{i}^{d}), & & (0, m)\times\Theta, \\ w_{i}(x,m) = (w_{i})_{t}(x,m) = 0, & & \Theta, \\ w_{i} = \frac{\partial w_{i}}{\partial \nu } = 0, & & \Gamma. \end{array} \right. \end{equation}$

(4.6)

Such systems allow us to characterize the optimal control solution of (2.3).

Theorem 4.1. Consider $Q \in U_{p}$ , and $u = u (Q)$ its corresponding state space solution of (2.2), then the control solution of (2.3) is

$\begin{equation} Q(x,t) = max(-p, min(\frac{-1}{\lambda}(u_{t})(\sum\limits_{i = 1}^{n}\frac{\partial w_{i}}{\partial x_{i}}),p)), \end{equation}$

(4.7)

where $w = (w_{1}....w_{n})$ with $w_{i} \in C ([ 0, T ]; H^{2}_{0}(\Theta))$ is the unique solution of (4.6).

Proof. Choose $d\in U_{p}$ such that $Q + k d \in U_{p}$ with $k > 0$ . The minimum of $C_{\lambda}$ is realized when the control $Q$ , verifies the following condition:

$\begin{equation} 0 \leq \lim\limits_{k\longrightarrow 0} \frac{C_{\lambda}(Q+k d)-C_{\lambda}(Q )}{k}. \end{equation}$

(4.8)

Consequently, Lemma 4.1 gives

$\begin{align} 0 \leq \lim\limits_{k\longrightarrow 0} \frac{C_{\lambda}(Q+k d)-C_{\lambda}(Q)}{k} \\ = \sum\limits_{i = 1}^{n}\int_\Theta \int_{0}^{m}\frac{\partial v(x,t)}{\partial x_{i}}( \frac{\partial u(x,t)}{\partial x_{i}}-u_i^d)dt dx+\int_\Theta \int_{0}^{m}\lambda d Q dt dx.\\\\ \end{align}$

(4.9)

Substitute by equation (4.6) and we find

$\begin{align} 0 \leq \sum\limits_{i = 1}^{n}\int_\Theta \int_{0}^{m}\frac{\partial v(x,t)}{\partial x_{i}}( {\frac{{\partial^{2} } {w_{i}}(x,t) }{{\partial t^{2}}} } +\Delta^{2} w_{i}(x,t)-Q(x,t)( w_{i})_{t}(x,t))dt dx+\int_\Theta \int_{0}^{m}\lambda d Q dt dx\\ \\ = \sum\limits_{i = 1}^{n}\int_\Theta \int_{0}^{m}\frac{\partial }{\partial x_{i}}( {\frac{{\partial^{2} } v}{{\partial t^{2}}} } +\Delta^{2} v-Q(x,t) v_{t})w_{i}(x,t)dt dx+\int_\Theta \int_{0}^{m}\lambda d Qdt dx\\ \\ = \sum\limits_{i = 1}^{n}\int_\Theta \int_{0}^{m}\frac{\partial }{\partial x_{i}}(d(x,t) u_{t})w_{i}dt dx+\int_\Theta \int_{0}^{m}\lambda dQ dt dx\\ \\ = \int_\Theta \int_{0}^{m}d(x,t)[u_{t}(\sum\limits_{i = 1}^{n}\frac{\partial w_{i}(x,t)}{\partial x_{i}})+\lambda Q dt dx].\\ \\ \end{align}$

(4.10)

It is known that if $d = d(t)$ in a chosen function with $Q+k d \in U_{p}$ , using Bang-Bang control properties, one can conclude that

$\begin{equation} Q(x,t) = max(-p, min(\frac{-u_{t}}{\lambda}(\sum\limits_{i = 1}^{n}\frac{\partial w_{i}}{\partial x_{i}}),p)) = max(-p, min( \frac{-u_{t}}{\lambda}Div(w), p)), \end{equation}$

(4.11)

with $Div(w) = \sum\limits_{i = 1}^{n}\frac{\partial w_{i}}{\partial x_{i}}$ . □

5. Flow time bilinear control problem

Now, we are able to discuss the case of bilinear time control of the type $Q = Q(t)$ . We want to reach a flow spatial state target prescribed on the whole domain $\Theta$ at a fixed time $m$ .

In such case, the set of controls (2.1) becomes

$\begin{equation} Q \in U_{p} = \{ Q\in L^{\infty}([0,m]){\mbox{ such that }} -p\leq Q(t) \leq p {\mbox{ for }} t \in (0, m)\}, \end{equation}$

(5.1)

with $p$ as a positive constant.

The cost to minimize is

$\begin{align} C_{\lambda}(Q) = \frac{1}{2}\Big\|\nabla u(x,m)-u^{d}\Big\|^{2}_{(L^2(\Theta))^{n}} + \frac{\lambda}{2}\int_{0}^{m} Q^2(t) dt\\ = \frac{1}{2}\sum\limits_{i = 1}^{n} \Big\|\frac{\partial u}{\partial x_{i}}(x,m) - u_{i}^{d}\Big\|^{2}_{L^2(\Theta)} + \frac{\lambda}{2}\int_{0}^{m} Q^2(t)dt, \end{align}$

(5.2)

where $u^d = (u_{1}^{d}, ....u_{n}^{d})$ is the flow spatial target in $L^2(\Theta)$ . The flow control problem is

$\begin{equation} \min\limits_{Q\ \in U_{p} }C_{\lambda}(Q), \end{equation}$

(5.3)

where $C_{\lambda}$ is the flow penalizing cost defined by (5.2), and $U_{p}$ is defined by (5.1).

Corollary 5.1. The solution of the flow time control problem (5.3) is

$\begin{align} Q(t) = max(-p, min(\int_{\Theta}\frac{-u_{t}}{\lambda} (\sum\limits_{i = 1}^{n}\frac{\partial w_{i}}{\partial x_{i}})dx,p)) \end{align}$

(5.4)

with $u$ as the solution of (2.2) perturbed by $Q(t)$ and $w_{i}$ as the solution of

$\begin{equation} \left \{ \begin{array}{lll} {\frac{{\partial^{2} } {w_{i}}}{{\partial t^{2}}} } +\Delta^{2} w_{i} = Q(t) (w_{i})_{t}, & & (0, m)\times\Theta, \\ w_{i}(x,m) = ( \frac{\partial u}{\partial x_{i}}(x,m) - u_{i}^{d}), & & \Theta, \\ (w_{i})_{t}(x,m) = 0, & & \Theta, \\ w_{i} = \frac{\partial w_{i}}{\partial \nu } = 0, & & \Gamma. \end{array} \right. \end{equation}$

(5.5)

Proof. Similar to the approach used in the proof of Theorem 4.1, we deduce that

$\begin{align} 0\leq \int_{0}^{m}d(t)[\int_\Theta u_{t}(\sum\limits_{i = 1}^{n}\frac{\partial w_{i}(x,t)}{\partial x_{i}})dx+\lambda Q ]dt, \end{align}$

(5.6)

where $d(t)\in L^{\infty}(0, m)$ , a control function such that $Q+k d \in U_{p}$ with a small positive constant $k$ . □

Remark 5.1. (1) In the case of spatiotemporal target, we remark that the error $(\frac{\partial u}{\partial x_{i}}(x, t) - u_{i}^{d})$ between the state and the desired one becomes a the change of velocity induced by the known forces acting on system (4.6).

(2) In the case of a prescribed time $m$ targets, we remark that the error $(\frac{\partial u}{\partial x_{i}}(x, m) - u_{i}^{d})$ between the state and the desired one becomes a Dirichlet boundary condition in the adjoint equation (5.5).

6. Partial flow optimal control problem

This section establishes the flow partial optimal control problem governed by the plate equation (2.2). Afterward we characterize the solution. Let $\theta\subset \Theta$ be an open subregion of $\Theta$ and we define

$\begin{array}{lll} \widetilde{P_{\theta}}: (L^2(\Theta)) & \longrightarrow & (L^2(\theta)) \\ \qquad \qquad u & \longrightarrow & \widetilde{P}_{\theta} u = u|_{\theta}, \end{array}$

and

$\begin{array}{lll} P_{\theta}: (L^2(\Theta))^{n} & \longrightarrow &(L^2(\theta))^{n} \\ \qquad \qquad u & \longrightarrow & P_{\theta} u = u|_{\theta}. \end{array}$

We define the adjoint of $P_{\theta}$ by

$P_{\theta}^{*}u = \left\{\begin{array}{lll} u \, \, in \, \, \Theta, \\ 0 \in \Theta \setminus \theta. \end{array} \right.$

Definition 6.1. The plate equation (2.2) is said to flow weakly partially controllable on $\theta \subset \Theta$ , if for $\forall \, \, \beta > 0$ , one can find an optimal control $Q\in L^{2}(0, m)$ such that

$|P_\theta \nabla u_Q(m)-u^d||_{(L^2(\theta))^{n}}\leq \beta,$

where $u^d = (z_{1}^{d}, ...., u_{n}^{d})$ is the desired flow in $(L^2(\theta))^{n}$ .

For $U_{p}$ defined by (5.1), we take the partial flow optimal control problem

$\begin{equation} \min\limits_{Q \in U_{p}} C_{\lambda}(Q), \end{equation}$

(6.1)

and the partial flow cost $C_{\lambda}$ is

$\begin{align} C_{\lambda}(Q) = \frac{1}{2}\Big\|P_\theta\nabla u(m)-u^{d}\Big\|^{2}_{(L^2(\theta))^{n}} + \frac{\lambda}{2} \int_{0}^{m} Q^2(t) dt\\ = \frac{1}{2}\sum\limits_{i = 1}^{n} \Big\|\widetilde{P}_{\theta}\frac{\partial u(T)}{\partial x_{i}} - u_{i}^{d}\Big\|^{2}_{(L^2(\theta))} + \frac{\lambda}{2} \int_{0}^{m} Q^2(t) dt. \end{align}$

(6.2)

Next, we consider the family of optimality systems

$\begin{equation} \left \{ \begin{array}{lll} {\frac{{\partial^{2} } {w_{i}} }{{\partial t^{2}}} } = \Delta^{2} w_{i}+Q(t) (w_{i})_{t},& & (0, m)\times\Theta,\\ w_{i}(x,m) = ( \frac{\partial u(m)}{\partial x_{i}} - \widetilde{P}_{\theta}^{*}u_{i}^{d}), & & \Theta, \\ (w_{i})_{t}(x,m) = 0, & & \Theta, \\ w_{i}(x,t) = \frac{\partial w_{i}(x,t)}{\partial \nu } = 0, & & \Gamma. \end{array} \right. \end{equation}$

(6.3)

Lemma 6.1. Let the cost $C_{\lambda}(Q)$ defined by (6.2) and the control $Q(t) \in U_{p}$ be the solution of (6.1). We can write

$\begin{align} \lim\limits_{k\longrightarrow 0} \frac{C_{\lambda}(Q+k d)-C_{\lambda}(Q )}{k} = \sum\limits_{i = 1}^{n} \int_\theta \widetilde{P}^*_{\theta}\widetilde{P}_{\theta}\left[ \int_{0}^{m}\frac{\partial^{2} w_{i}}{\partial t^{2}} \frac{\partial v(x,t)}{\partial x_{i}} dt+ \int_{0}^{m}w_{i} \frac{\partial }{\partial x_{i}}( \frac{\partial^{2} v}{\partial t^{2}}) dt\right]dx\\ + \int_{0}^{m}\lambda d Q dt, \end{align}$

(6.4)

where the solution of (4.1) is $v$ , and the solution of (6.3) is $w_{i}$ .

Proof. The functional $C_{\lambda}(Q)$ given by (6.2), is of the form:

$\begin{align} C_{\lambda}(Q) = \frac{1}{2} \sum\limits_{i = 1}^{n}\int_{\theta}(\widetilde{P}_{\theta}\frac{\partial u}{\partial x_{i}} - u_{i}^{d} )^2 dx + \frac{\lambda}{2} \int^{m}_{0} Q^2(t) dt. \end{align}$

(6.5)

Choose $u_{k} = u(Q+k d)$ and $u = u(Q)$ . By (6.5), we deduce

$\begin{align} \lim\limits_{k\longrightarrow 0} \frac{C_{\lambda}(Q+k d)-C_{\lambda}(Q)}{k} = \lim\limits_{k\longrightarrow 0}\sum\limits_{i = 1}^{n} \frac{1}{2}\int_{\theta}\frac{(\widetilde{P}_\theta \frac{\partial u_{k}}{\partial x_{i}}-u_i^d)^{2}-(\widetilde{P}_\theta \frac{\partial u}{\partial x_{i}}-u_i^d)^{2}}{k}dx\\ + \lim\limits_{k\longrightarrow 0}\frac{\lambda}{2}\int_{0}^{m}\frac{(Q+k d)^2-Q^2}{k}dt. \end{align}$

(6.6)

Furthermore,

$\begin{align} \lim\limits_{k\longrightarrow 0} \frac{C_{\lambda}(Q+k d)-C_{\lambda}(Q)}{k} \\ = \lim\limits_{k\longrightarrow 0}\sum\limits_{i = 1}^{n}\frac{1}{2}\int_{\theta}\widetilde{P}_{\theta}\frac{( \frac{\partial u_{k}}{\partial x_{i}}- \frac{\partial u}{\partial x_{i}})}{k}(\widetilde{P}_{\theta} \frac{\partial u_{k} }{\partial x_{i}}+ \widetilde{P}_{\theta} \frac{\partial u}{\partial x_{i}}-2u_i^d)dx \\ + \lim\limits_{k\longrightarrow 0}\frac{1}{2}\int_{0}^{m}(2\lambda d Q+k \lambda d^2)dt\\ = \sum\limits_{i = 1}^{n}\int_\theta \widetilde{P}_{\theta} \frac{\partial v(x,m)}{\partial x_{i}} \widetilde{P}_{\theta}( \frac{\partial u(x,m)}{\partial x_{i}}-\widetilde{P}_{\theta}^{*}u_i^d)dx+\int_{0}^{m}\lambda dQ dt \\ = \sum\limits_{i = 1}^{n} \int_\theta \widetilde{P}_{\theta} \frac{\partial v(x,m)}{\partial x_{i}} \widetilde{P}_{\theta}w_{i}(x,m)dx+\lambda \int_{0}^{m}dQ dt. \end{align}$

(6.7)

Using (6.3) to (6.7), we conclude

$\begin{align} \lim\limits_{k\longrightarrow 0} \frac{C_{\lambda}(Q+k d)-C_{\lambda}(Q)}{k} = \sum\limits_{i = 1}^{n} \int_\theta \widetilde{P}^*_{\theta}\widetilde{P}_{\theta}\left[ \int_{0}^{m}\frac{\partial^{2} w_{i}}{\partial t^{2}} \frac{\partial v(x,t)}{\partial x_{i}} dt+ \int_{0}^{m}w_{i} \frac{\partial }{\partial x_{i}}( \frac{\partial^{2} v}{\partial t^{2}}) dt\right]dx\\\\ + \int_{0}^{m}\lambda d Qdt.\\ \end{align}$

(6.8)

□

Theorem 6.1. Consider the set $U_{p}$ , of partial admissible control defined as (5.1) and $u = u (Q)$ is its associate solution of (2.2), then the solution of (6.1) is

$\begin{equation} Q_{\varepsilon}(t) = max(-p,min( \frac{-1}{\lambda}\widetilde{P}_{\theta}(u_{t})(\widetilde{P}_{\theta} Div(w)),p)), \end{equation}$

(6.9)

where $Div(w) = \sum\limits_{i = 1}^{n}\frac{\partial w_{i}}{\partial x_{i}}$ .

Proof. Let $d \in U_{p}$ and $Q + k d \in U_{p}$ for $k > 0$ . The cost $C_{\lambda}$ at its minimum $Q$ , verifies

$\begin{equation} 0 \leq \lim\limits_{k\longrightarrow 0} \frac{C_{\lambda}(Q+k d)-C_{\lambda}(Q)}{k}. \end{equation}$

(6.10)

From Lemma 6.1, substituting $\frac{\partial^{2} v}{\partial t^{2}}$ , by its value in system (4.1), we deduce that

$\begin{align} 0 \leq \lim\limits_{k\longrightarrow 0} \frac{C_{\lambda}(Q+k d)-C_{\lambda}(Q)}{k}\\ = \sum\limits_{i = 1}^{n}\int_\theta \widetilde{P}^*_{\theta}\widetilde{P}_{\theta}\left[\int_{0}^{m} \frac{\partial v}{\partial x_{i}}\frac{\partial^{2} w_{i} }{\partial t^{2}}dt+ \int_{0}^{m}(-\Delta^{2} \frac{\partial v}{\partial x_{i}}+Q(t) \frac{\partial }{\partial x_{i}}(v_{t}) + d(t)\frac{\partial }{ \partial x_{i}}(u_{t}))w_{i} dt\right]dx\\ + \int_{0}^{m}\lambda d Q dt, \end{align}$

(6.11)

and system (6.3) gives

$\begin{align} 0 \leq \sum\limits_{i = 1}^{n} \int_\theta \widetilde{P}^*_{\theta}\widetilde{P}_{\theta}\left[\int_{0}^{m} \frac{\partial v}{\partial x_{i}}(\frac{\partial^{2} w_{i} }{\partial t^{2}}-\Delta^{2} w_{i}-Q(t) (w_{i})_{t})dt+d(t) \frac{\partial }{\partial x_{i}}(u_{t})w_{i} dt\right]dx+\int_{0}^{m}\lambda d Q dt.\\ \\ = \sum\limits_{i = 1}^{n} \int_\theta \widetilde{P}^*_{\theta}\widetilde{P}_{\theta} \int_{0}^{m} (h(t)u_{t})\frac{\partial w_{i}}{\partial x_{i}} dt+ \int_{0}^{m}\lambda d Q dt.\\ \\ = \int_{0}^{m} h(t)\int_\theta\left[ u_{t}\widetilde{P}^*_{\theta}\widetilde{P}_{\theta} \sum\limits_{i = 1}^{n}\frac{\partial w_{i}}{\partial x_{i}} + \lambda Q\right] dx dt, \end{align}$

(6.12)

which gives the optimal control

$\begin{equation} Q_{\varepsilon}(t) = max(-p,min( \frac{-1}{\lambda}\widetilde{P}_{\theta}(u_{t})(\widetilde{P}_{\theta} Div(w)),p)). \end{equation}$

(6.13)

□

7. Conclusions

This paper studied the optimal control problem governed by an infinite dimensional bilinear plate equation. The objective was to command the flow state of the bilinear plate equation to the desired flow using different types of bounded feedback. The problem flow optimal control governed by a bilinear plate equation was considered and solved in two cases using the adjoint method. The first case considered a spatiotemporal control function and looked to reach a flow target on the whole domain. The second case considered a time control function and looks to reach a prescribed target at a fixed final time. As an application, the partial flow control problem was established and solved using the proposed method. More applications can be examined, for example. the case of fractional hyperbolic systems.

Use of AI tools declaration

The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

Acknowledgments

This work was funded by the Deanship of Scientific Research at Jouf University under Grant Number (DSR2022-RG-0119).

Conflict of interest

The authors affirm that they have no conflicts of interest to disclose.

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