亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        Regional gradient observability for semilinear hyperbolic system s:HUM approach

        2018-04-04 03:49:22AdilKHAZARIAliBOUTOULOUTImadELHARRAKI
        Control Theory and Technology 2018年1期

        Adil KHAZARI,Ali BOUTOULOUT,Imad EL HARRAKI

        1.Sidi Moham ed Ben Abdellah University,école Nationale de Commerce et de gestion,Fez,Morocco;

        2.TSI Team,MACS Laboratory,Faculty of Sciences,Mou lay Ism ail University,Meknes,Morocco;

        3.école nationale supérieure des mines de Rabat,Rabat,Morocco

        1 Introduction

        Observability represents one of the major concepts of modern control system theory.It was introduced by R.Kalman in 1960.Roughly speaking,observability is concerned with whether without knowing the initial state,one can determine the state of a system given the input and the output.The study of this kind of problem has become fairly common,and is now an established area of research with a long list of publications.

        Hyperbolic problem s are one of the problem s which undergoes a detailed investigation,due to the many problem s which rely on this theory.Hyperbolic equations describe various time dependent models of many physical,chemical and biological phenomena so the study of such equations is of substantial contemporary interest.

        Modeling any real problem involves approximations.When we model a phenomena,we must make compromises.We attem pt to retain essential factors while keeping within bounds of mathematical tractability.All real problem s are nonlinear,often strongly nonlinear.But in a mathematics point of view we do liniarize them.In this paper we are interested to study the regional observability of semilinear hyperbolic problem s which are linear problems containing a nonlinear term(see[1,2]).

        Analysis and control theory are known as as et of technical reasoning and mathematical tools in the service of system s for both a better understanding of its functioning and decision-making.To do this,there must bean accurate description of the system,which requires a fairly detailed know ledge of its various components,their behavior and their interactions.This description may be represented as partial differential equations(PDEs).Exploration and research on the analysis of distributed system sand their control were mainly focused on the global domain of the evolution of system(see[3,4]and[5]).However,many real problem s can’t be formulated in all the domain of development,but only in a sub-region of global area,called regional context(see[2,6]and[7]).

        Specifically,the regional observability concept concerns the actual identification of the trajectory based on the information collected on the system which is equivalent to solve an inverse problem(see[8]).The study of this concept becomes more com p lex in the case of infinite dimension spaces.The general approach to reconstruct the initial state is to leave the system in free evolution for a tim e interval[0,T]during which the performances are measured with sensors.For example,the problem of detecting a polluted area in the ocean caused by a sinking oil ship or knowing the region of a pipe leak both problem s are observability problems where we need to reconstruct just the gradient initial conditions without the know ledge of initial conditions(see[9,10]and[11]).

        This work focuses on the study of regional observability of a very important class of distributed system s,which is a class of semilinear system s,since they are intermediate between linear system s and the nonlinear ones(see[12]).In fact,m any real problems are modeled by using nonlinear systems,of either the parabolic type(such as the heat equation)or the hyperbolic type(such as the w ave equation).We extend the concept of regional observability of the gradient for linear system s to a class of semilinear hyperbolic system s.This work is discussed in the parabolic case(see[9]).To rebuild the gradient of the initial state in a subregion ω of the evolution domain Ω,we combine the so called Hilbert uniqueness method(see)with a fixed point technique(see[11])for the reconstruction of the flow of initial conditions.This technique was used in[13]for the exact distributed controllability for the semilinear wave equation.The author generalized the theorem s of exact controllability for the linear wave equation with a distributed control to the semilinear case,showing that,given T large enough,for every initial state in a sufficiently small neigh bour hood of the origin in a certain function space,there exists a distributed control,supported on a part of a domain,driving the system to rest.This approach also provides a numerical algorithm tested on a simulation example.

        2 Regional observability of the gradient

        Let Ω be an open bounded subset of Rn(n=1,2,3).For T>0,we denote Q=Ω×]0,T[,Σ=?Ω×]0,T[and we consider the follow ing hyperbolic system:

        where A is an elliptic and a second order operator,system(1)is augmented with the output function given by

        augmented with the output function

        Let us consider a basis of eigenfunctions of the operator A,denoted Φmj,with eigenvalues associated are λmwith multiplicity rm.

        We can write for any(y1,y2)∈F,

        then the output equation can be expressed by

        Consider the operatorˉ?given by the formula

        w here

        For ω ? Ω a nonempty open subregion of Ω with positive Lebesgue measure,letbe the restriction operator defined by

        where

        De finition1System is said to be gradient observable or G-observable in ω if we can reconstruct the gradient of the initial condition in a subregion ω of Ω.

        In what follow s,we say that a system is G-observable in ω.

        We consider the following semilinear system:

        augmented with the output function

        where N is a nonlinear operator as sum ed to be locally Lipschitzian.

        System(5)is equivalent to the follow ing system

        System(7)is increased by the output function

        System(7)has a unique solution that can be expressed in the m ild sense as follow s(see[15]):

        Problem(*)Given the semilinear system(5)and(6)on]0,T[,is it possible to reconstructwhich is the gradient of the initial condition of(5)on ω?

        3 HUM app roach

        In this section,we give an approach that allows the reconstruction of the initial gradient of the state and speed in ω.This approach is an extension of HUM method developed by Lions[15],and does not take into account what m ay be the residual part in the subregion Ωω.

        We consider system(5)augmented with the output function(6)and we assume that system(5)is observed by means of internal zone sensor(D,f)with D?Ω is the support of the sensor and f∈L2(D)defined his space repartition.

        The problem of regional gradient observability of(5)and(6)is the possibility to reconstruct the component

        Let us consider

        which can be decomposed as follow s:

        and

        System(12)has a unique solution

        We define the mapping

        which in ducesasem i-norm on G,with=(??0,??1),if the linear system(12)is weakly G-observable in ω,the semi-norm define a norm on G we also denote by G the completion of G.

        We define the auxiliary system by

        The resolution to(15)provides

        Consider the operator

        where

        We decompose as follow s:ˉψ=ψ0+ψ1,w here ψ0is a solution to the problem

        and ψ1is a solution to

        then

        w here

        and

        with

        If the linear part of system(5)is weakly G-observable,then Λ is invertible,and finally

        Considering the following system:

        We have the following result.

        Proposition 1If the linear part(1)of system(5)is weakly G-observable in ω and N satisfies that?c > 0 such as ‖N(x)‖≤ c‖x‖,then(20)admits a unique fixed point corresponding to the gradient of the initial conditions to be observed in the subregion ω.

        ProofWe show the proposition in two steps:first the operator M is com pact;second ly:we apply the theorem of the fixed point of Schauder,to prove that the operator Mhas a fixed point that corresponds to the gradients of the initial conditions to observe in the region ω.

        ?Let p> 0 and Bp=B(0,p)×B(0,p),and we have

        We have ψ1(·)is a solution to(17),then we obtain

        Without loss of generality we assume that rm=1,then we obtain:

        or we have

        Then

        with t? τ=t′.

        By the continuity of the gradient we have

        where c1is the constant of continuity.

        In the other hand,ψ0(·)solution to(16)then

        By the continuity of the gradient we have

        As well,we obtain that θ(·)is a solution to(13),then

        We have ?1is a solution to(12)then

        Then we obtain

        App lying Gronwall’s theorem for the function θ(·)we have

        Therefore,using Gronwall’s theorem for the function ψ1(·)we have

        For 0<t1<T and 0<t2<T,we obtain

        Thus,we see that M:Bp→G?is com pact.

        ?M enforces the ball Bpin itself.If the linear part(1)of system(5)is weakly G-observable in ω,then Λ?1P is bounded,

        Then with the Schauder theorem the operator Madmits a unique fixed point and the gradient of the initial condition to be observed in ω is given by□

        We have the follow ing algorithm:

        Algorithm

        Step 1The initial conditionsthe region ω,the domain D,the function of distribution f and the accuracy threshold ε.

        Step 2Repeat

        ?Solving(13)and obtain θk.

        Step 3The restriction ofto ω corresponds to the gradientto be reconstructed in ω.

        4 Simulation results

        Here we present a numerical example illustrating the algorithm based to HUM m ethod.The obtained results are related to the considered subregion and the sensor location.

        ExampleConsider the monodimensional semilinear system in Ω=]0,1[,

        For the simulations in the zonal case,we assume that in this case the sensor is located in an internal zone D=]0.6,0.7[,T=2,

        Using the obtained algorithm,for ω=]0.35,0.65[,we have Figs.1 and 2.

        Fig.1 The exact state gradient and estim ated state gradientin ω.

        Fig.2 T he exact speed gradientand estimated speed gradient in ω.

        The reconstruction is observed with error equals to

        For ω = Ω,we have Figs.3 and 4.

        The reconstruction is observed with error equals to

        Here we study numerically the dependence of the gradient reconstruction error with respect to the subregion area of ω,we have Table 1.

        Fig.3 The exact state gradientand estim ated state gradient in Ω.

        Fig.4 The exact speed gradientand estimated speed gradientin Ω.

        Table 1 The reconstruction error with respect to the subregion area.

        5 Conclusions

        The regional gradient observability for hyperbolic semilinear systems is considered.The regional gradient observability of linear systems was explored to solve the problem s related to the semilinear ones which constitutes a natural extension.We explored Hilbert Uniqueness reconstruction approach combined with the fixed point techniques.This leads to an algorithm which is numerically implemented.Many questions remain open,such as the case of the regional gradient observability of semilinear system s using sectorial approach[17]and the case of the regional gradient of the boundary observability of hyperbolic system s[18].The questions are still under consideration and the results will appear in a future paper.

        [1]D. Henry. Geometric Theory of Semilinear Parabolic Systems.Berlin: Springer, 1981.

        [2] I. El Harraki, A. Boutoulout. Gradient controllability for hyperbolicsystems. Information Sciences Letters – An International Journal,2014, 3(1): 11 – 19.

        [3] I. Lasiecka, R. Triggiani. Exact controllability of semilinear abstractsystems with applications to waves and plates boundary controlproblems. Applied Mathematics and Optimization, 1991, 23(2):109 – 154.

        [4]H. Zhou. Approximate controllability for a class of semilinearabstract equations. SIAM Journal on Control and Optimization,1983, 21(4): 551 – 555.

        [5]E. Zuazua. Exact controllability for the semilinear wave equations.Journal de Mathe′matiques Pures et Applique′es, 1990, 59(1): 1 –31.

        [6]I.El Harraki,A.Boutoulout.A notes on the boundary gradient controllability for hyperbolic system s:approaches and simulations.International Review of Automatic Control,2015,8(3):170–179.

        [7] E.Zerrik,R.Larhrissi,H.Bourray.An output controllability problem for sem ilinear distributed hyperbolic system s.International Journal of Applied Mathematics Computer Science,2007,17(4):437–448.

        [8]K.Ram dani,M.Tucsnak,G.Weiss.Recovering the initial state of an infinite-dimensional system using observers.Automatica,2010,46(10):1616–1625.

        [9] A.Boutoulout,H.Bourray,F.Z.El Alaoui.Regional gradient observability fordistributed sem ilinearparabolic system s.Journal of dynamical and Control System s,2012,18(2):159–179.

        [10]A.Boutoulout,H.Bourray,A.Khazari.Gradient observability for hyperbolic system.International Review of Automatic Control,2013,6:247–263.

        [11]E.Zeidler.Nonlinear Functional Analysis and Its Applications II/A:Linear Monotone Operators.New York:Springer,1990.

        [12]R.C.Baker,B.Charlie.Nonlinear unstable system s.International Journal of Control,1989,23(4):123–145.

        [13]W.Liu.Exact distributed controllability for the sem ilinear wave equation.Portugaliae Mathem atica,2000,57(4):494–508.

        [14]A. Pazy. Semigroups of Linear Operators and Applications to PartialDifferential Equations.New York: Springer, 1990.

        [15]J. L. Lions. Contr? olabilit′e Exacte, Perturbations et Stabilisation deSyste`mes Distribue′s. Paris: Masson, 1988.

        [16]J.L.Lions,E.Magenes.Problèm es Aux Limites Non Homogè Nes et Applications.Paris:Dunod,1968.

        [17]A.Khazari,A.Boutoulout.Gradient observability for sem ilinear hyperbolic system s:sectorial approach.Intelligent Control and Automation,2014,5(3):170–181.

        [18]A.Khazari,A.Boutoulout.Flux reconstruction for hyperbolic system s:sensors and sim ulations.Evolution Equations and Control Theory,2015,4(2):177–192.

        亚欧视频无码在线观看| 少妇被爽到高潮喷水久久欧美精品| 色欲av伊人久久大香线蕉影院| 一本久道综合在线无码人妻 | 日本边添边摸边做边爱的网站| 亚洲另类激情综合偷自拍图 | 亚洲色成人www永久在线观看| 成人黄色网址| 国产精品公开免费视频| 国产精品伦人视频免费看| av男人操美女一区二区三区| 中文字幕亚洲精品专区| 国产精品久久久福利| 免费毛片a线观看| 蜜臀aⅴ国产精品久久久国产老师 国产精品久久婷婷六月丁香 | 亚洲精品乱码久久久久蜜桃| 丰满人妻一区二区三区视频53| 人妻少妇av无码一区二区| 亚洲av美女在线播放啊| 国产一区,二区,三区免费视频| 狠狠综合久久av一区二区三区| 91精品国产综合久久熟女| 久久久久久亚洲av成人无码国产| 国产色a在线观看| 中文字幕一区二区人妻出轨| 女同国产日韩精品在线| 亚洲av激情一区二区| 大陆国产乱人伦| 熟妇丰满多毛的大隂户| 99精品国产在热久久国产乱| 色哟哟av网站在线观看| 在线亚洲妇色中文色综合| 精品人妻一区二区三区浪人在线| 777国产偷窥盗摄精品品在线| 亚洲色偷拍区另类无码专区| 欧美日韩国产成人综合在线影院| 青青草视频在线你懂的| 国产亚洲熟妇在线视频| 久久人妻无码一区二区| 台湾佬综合网| 青青草视频华人绿色在线|