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Journal of Pure and Applied Mathematics

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Yaméogo Pierre Claver*, Alex Vuginshteyn, Guido Fuortes and Abdo Miled Abou Jaoude
 
Bircham International University, United States, Email: claver.yams1@gmail.com
 
*Correspondence: Yaméogo Pierre Claver, Bircham International University, United States, Email: claver.yams1@gmail.com

Received: 03-Sep-2024, Manuscript No. puljpam-24-7285; Editor assigned: 05-Sep-2024, Pre QC No. puljpam-24-7285(PQ); Accepted Date: Sep 25, 2024; Reviewed: 08-Sep-2024 QC No. puljpam-24-7285(Q); Revised: 13-Sep-2024, Manuscript No. puljpam-24-7285(R); Published: 30-Sep-2024, DOI: 10.37532/2752- 8081.24.8(5).01-03

Citation: Claver YP, Vuginshteyn A, Fuortes G, et al. Specific case of an internal control-external control (bounded domain). J Pure Appl Math.2024; 8(5):1-3

This open-access article is distributed under the terms of the Creative Commons Attribution Non-Commercial License (CC BY-NC) (http://creativecommons.org/licenses/by-nc/4.0/), which permits reuse, distribution and reproduction of the article, provided that the original work is properly cited and the reuse is restricted to noncommercial purposes. For commercial reuse, contact reprints@pulsus.com

Abstract

We try to study the controllability of bounded domain Ω consisting of several heated materials. For this, we will use the functional (μ), whichoptimizes the cost. The objective is to bring the excess heat inside the domain and also on the border of the domain and it’s this excess heat that is a function called control.

Key Words

Prime numbers; Prime conjecture; Graphs; Twin prime conjecture; Sequential prime product

Introduction

Let Ω be a bounded domain made up of heated materials, we give ourselves the conductivity (x) at the point x ∈ Ω the heat source ƒ in L2(Ω) in the temperature TD imposed on ΓD by the system, the flux PN imposed on TN. Let’s consider the following problem:

equation

Problem

Let yD be a given temperature.

How to act on the system (S) so that y is close enough to yD?

Idea

It is a question of bringing a surplus of heat u so that y is as close as possible to yD [1-5]. This excess heat is a function called control [1-5]. To leave a good choice of u, we must optimize the cost, which reflects what we want to achieve and the means at our disposal. What amounts to considering the functional J(u) defined by:

equation

Where g is a definite function of Ω a value in â?. (y-yD) makes is possible to minimize the difference between y and yD, ∈ being very small serves not only to prove the existence and uniqueness of the solution but also to minimize the cost.

Problem

Is there Å« ∈ u such that

equation

1. u is in the set of admissible controls,

2. Å« is the optimal control

3. y= y(Å«) is the optimal state

The function J is the objective function

However, there are two types of controls:

1. Internal control,

2. Border control

NB: we advise you to look at the course material on control for detailed proof.

Internal control

It is a question of bringing the excess heat inside the domain. Let us consider the following example of control:

Let ƒ in L2(Ω), yD belonging to L2(Ω) and u be a nonempty closed convex set of L2(Ω) . Let u∈, (u) be the solution of the following equation.

equation

Let’s pose

equation

So we get the following problem:

equation

Resolution

equation

For any Z in L2(Ω),we know the problem below

equation

Has a unique solution in H10Ω, therefore is the unique solution of problem (11).

We define the following operation:

equation

Were Z is the solution of equation (4). A thus defined is linear and continuous.

We have

L2(Ω),

By replacing (u) by its value in (2), we get:

equation

Where

equation

And equation is a constant.

Minimizing the functional J amounts to minimizing the functional J1.

We put

equation

1. a is bilinear,continous,coercive and symmetric,

2. l is continous linear,

3. u a nonempty closed convex set of L2(Ω),

By stampacchia’s theorem, there exists a unique Å« in u solution.

The solution Å« is characterized by:

equation

Having obtained the existence and uniqueness of the solution, we are interested in giving the characteristics of Å«. To do this, we introduce the optimality system. By interpreting, the reaction

equation

The Conjoint state equation is the solution of the following problem:

equation

We therefore have

equation

We get the following optimality system:

equation

Particular case

equation

In the case of shareholder internal Control, we have

equation

Border control

This is to bring the excess heat to the Boundary of the domain.

Consider

The following boundary control example

Let ƒ in L2(Ω), yD belong to L2(Ω), g a function of L2(T) and u nonempty closed convex of L2(T). Let u∈ u, y(u) be a solution of the following equation:

equation

We pose:

equation

Resolution

Simplification

By setting:

equation

Where y1(u) is the solution of the problem:

equation

And z belongs to H10(Ω) solution de :

equation

System S1 becomes

equation

We pose:

equation

Where

equation

Transposition formula

We associate to (S2) the following transposition equation:

equation

Let ƒ be a function of L2(Ω) ( ) admitting a unique solution, we get from ( )

equation

Considering the following problem:

equation

l is linear and continuous application on L2(Ω) by riesz’s theorem, there exists a unique y L2(Ω) such that

equation

We define the operator

equation

Replacing

equation

In J(u), We have:

equation

With

equation

We pose

equation

Conclusion

In short, to solve the problem we must optimize the cost according to the goal we are looking for and taking into account the means at our disposal. But the case here requires a good mastery of the solutions of optimal control and some demonstrations to prove the existence, uniqueness and stability of solutions. Also, we give some extensions to our investigation.

References

 
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Citations : 83

Journal of Pure and Applied Mathematics received 83 citations as per Google Scholar report

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