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

        ?

        Non-local Boundary Value Problem for the Third Order Mixed Type Equation in Double-connected Domain

        2014-05-04 00:28:06ABDULLAYEVKh

        ABDULLAYEV O.Kh

        National University of Uzbekistan,Tahskent 700-174,Uzbekistan.

        Received 7 March 2014;Accepted 31 August 2014

        Non-local Boundary Value Problem for the Third Order Mixed Type Equation in Double-connected Domain

        ABDULLAYEV O.Kh?

        National University of Uzbekistan,Tahskent 700-174,Uzbekistan.

        Received 7 March 2014;Accepted 31 August 2014

        .In the present paper an existence and uniqueness of solution of the nonlocal boundary value problem for the third order loaded elliptic-hyperbolic type equation in double-connected domain have been investigated.At the proof of unequivocal solvability of the investigated problem,the extremum principle for the mixed type equations and method of integral equations have been used.

        Loaded equation;elliptic-hyperbolic type;double-connected domain;an extremum principle;existence of solution;uniqueness of solution;method of integral equations.

        1 Introduction

        Boundary value problems(BVP)for mixed type equations have numerous applications in physics,biology and in other material sciences.F.I.Frankl[1]found critical applications of the problem Tricomi and others related problems in transonic gas dynamics. In the works by A.V.Bitsadze[2],the analogue of problem Tricomi for the first time is formulated and investigated in double-connected domain for the equations of the mixed type,whichwas newdirectionofthetheorypartial differential equations.Afterthiswork various problems for the equation of the mixed elliptic-hyperbolic type of the second order in double connected domain were investigated.For example,we note works by M. S.Salahitdinov and A.K.Urinov[3],B.Islomov and O.Kh.Abdullaev[4]and etc.

        We as well note that with intensive research on problem of optimal control of the agroeconomical system,regulating thelabel ofgroundwatersand soilmoisture,it hasbecome necessary to investigate a new class of equations called“LOADED EQUATIONS”.Such equations were investigated in first in the works of N.N.Nazarov and N.Kochin, but they didn’t use the term“LOADED EQUATIONS”.For the first time was given the most general definition of a LOADED EQUATIONS and various loaded equations are classified in detail by A.M.Nakhushev[5].After this work has appeared very interesting results of the theory of boundary value problems for the loaded equations parabolic, parabolic-hyperbolic and elliptic-hyperbolic types.We note works of:A.M.Nakhushev[6],K.B.Sabitov and E.R.Melisheva[7],E.R.Melisheva[8]and O.Kh.Abdullaev[9],[10].

        Local and non-local problems for the third order loaded equations elliptic-hyperbolic type in double-connected domains as well were not investigated.

        In the present paper,the uniqueness and the existence of the solution of non-local boundary value problem for the third order loaded equation of elliptic-hyperbolic type in double-connected domain was proved.

        2 The statement of the problem

        Consider the equation

        in double-connected domain ?,bounded with two lines:

        We will introduce designations:

        Problem I.To find a function u(x,y)with the following properties:

        1)u(x,y)∈C(?);

        3)u(x,y)satisfies gluing conditions on lines of changing type:

        4)u(x,y)satisfies boundary conditions:

        and

        Theorem 2.1.If conditions(2.8)-(2.12)and

        are satisfied,than the solution of the Problem I exists and unique.

        Proof.Note,that at the proof of the theorem the following lemma is important:

        Lemma 2.1.Any regular solution of the Eq.(2.1)at the xy6=0,x+y6=±q can be represented in the form of[11]:

        where z(x,y)is regular solution of the equation

        Without restricting generality it is possible to assume the following conditions

        Based on(2.14)and(2.15)considering(2.16),theProblem Iwill be reduced to theProblem I*:To find a solution of the Eq.(2.15)in the domain of ?,satisfying conditions:

        Note that the solution of the Eq.(2.15)in hyperbolic domain looks like[10]:

        Owing to(2.23)we will receive,that the solution of the Cauchy problem for the Eq.(2.15) satisfying conditions:

        in the domain of Δ2,has a form:

        From here,by virtue,(2.21)we obtain:

        Further,owing to(2.20)from(2.26)is found:

        Hence:

        From(2.28)and(2.27)we will receive a functional relation between τ1(y)and ν1(y)from

        From the solution of problem Cauchy for the Eq.(2.15)satisfying conditions z(x,0)= τ2(x),zy(x,0)=ν2(x)in the domain of Δ1,and with the account of conditions(2.20)and (2.22),we will obtain a functional relation between τ2(x)and ν2(x):

        and we will find

        3 The uniqueness of solution of the problem I?.

        It is known that,if the homogeneous problem has only trivial solution then a solution of the accordingly non-uniform problem will be unique.

        We will assume that bj(x)≡μj(t)≡0 then from(2.29)-(2.32)accordingly we will receive:

        Note that an extremum principle for the hyperbolic equations[12]will be applicable to the investigated problem if ω1(y)≡0,and it is obtained from(3.2),at τ1(y)≡0,i..at first it is required to prove that τ1(y)≡0.

        Let the function τ1(y)reach a positive maximum(a negative minimum)in some point of y0∈A2B2,then from(3.2)based on(2.13)we obtain

        To conclude that if bj(x)≡μj(t)≡0 and a1(y)>1/2,then we have ω1(y)≡0,i.e. an extremum principle for the hyperbolic equations became applicable to investigated problem I?.

        The following principle of the extremum is acceptable:

        Proof.Lemma 3.2 will be proved similarly as the Lemma 3.1.

        Thus,the solution of homogeneous problem I*is identically equal to zero in the domain of ?.The uniqueness of solution of theProblemI?is proved.Therefore,by virtue of Lemma 2.1 we will conclude that the solution of theProblem Iis unique,too.

        4 The existence of solution of the problem I.

        where G(ξ,η;x,y)is the Green function of the problem N for the Laplace equation in the domain ?0,which looks like[3]:

        and

        Further,after differentiating(4.3)by x and(4.4)by y,we will get

        where

        It is easy to see that

        As well,from(2.30)and(2.31)accordingly we can get:

        where|M(t,y,λ)|6const,and

        where

        Note that the unequivocal solvability of the system integral Eqs.(4.9)follows from the uniqueness of solution of the Problem I and from the theory integral equations[14].

        Theorem 2.1 is proved.

        [1]Frankl F.I.,Selected Works of the Gas Dynamics.M.1973.(In Russian)

        [2]Bitsadze.A.V.,To the Problem of the Mixed Type Equations.Trudi.Instit.Matem.AN SSSR., 1953.(In Russian)

        [3]Salakhitdinov M.S.,Urinov A.K.,Problems for the general Lavrentyev-Bitsadze equation in doubly connected domain.Izv.N Uz SSR ser.fiz-mat.nauk.,6(1990),29-36.(In Russian)

        [4]Islomov B.,Abdullaev O.Kh.,Boundary value problem of type of the problem Bitsadze for the equation of the elliptic-hyperbolic type of the third order in double-connected domain. Dokl.Adigskoy AN.,7(1)(2004),42-47.(In Russian)

        [5]Nakhushev A.M.,Loaded equations and their applications.Differe.Equa.,19(1)(1983),74-81.

        [6]Nakhushev A.M.,N-the Darboux problem for the degenerate loaded integral differential equation of the second order.Differe.Uravn.,12(1)(1976),103-108.

        [7]Sabitov K.B.,Melisheva E.P.,The Dirichlet problem for the loaded mixed type equations in a rectangularity domain.Russi.Math.,57(2013),53-65.

        [8]Melisheva E.P.,The Dirichlet problem for the loaded equations of the Lavrentyev-Bitsadze. Vestnik SamGU.,6(80)(2010).(In Russian)

        [9]Abdullayev O.Kh.,About uniqueness of solution of the boundary value problem for the loaded equation of the elliptic-hyperbolic type in double-connected domain.Doklady A.N. RUz.,3(2011),7-11.(In Russian)

        [10]Abdullayev O.Kh.,Boundary value problem for the loaded equation of the elliptic-hyperbolic type in doubly connected domain.Vestnik.KRAUNS.Russian.Phyz-Math-science,1(8) (2014),33-48.(In Russian)

        [11]Salakhitdinov M.S.,Mixed-Compound Type Equations.Fan.1974.(In Russian)

        [12]Agmon S.,Nirenberg L.,Protter M.H.,A maximum principle for a class of hyperbolic equation and application to equations elliptic-hyperbolic type.Comm.Pure Appl.Math.,1(1953), 455-470.

        [13]Bitsadze A.V.,Differential Equations of Mixed Type.Mac.Millan.Co.,New York.1964.

        [14]Muskheleshvili N.I.,Physics,Singular Integral Equations:Boundary Problems of Function Theory and Their Application to Mathematical Physics,Dover Publications,2008.

        ?Corresponding author.Email addresses:obidjon.mth@gmail.com(O.Kh.Abdullayev)

        10.4208/jpde.v27.n4.1 December 2014

        AMS Subject Classifications:35M10

        Chinese Library Classifications:O175.2

        亚洲精品视频在线一区二区| 国产成人综合久久久久久| 亚欧免费视频一区二区三区| 国产一级自拍av播放| 久久国产精品亚洲va麻豆| 一区二区无码精油按摩| 亚洲一区二区免费日韩| 国产精品久久久黄色片| 国产精品毛片va一区二区三区| 久久只精品99品免费久23| 久久久国产一区二区三区四区小说| 69av在线视频| av大片网站在线观看| 国产一区二区三区十八区| 丰满少妇人妻久久久久久| 最新亚洲人成网站在线观看| 三级特黄60分钟在线观看| 亚洲熟妇网| 国产av一区麻豆精品久久| 久久亚洲av成人无码国产最大| 中文字幕一区二区三区乱码| 亚洲AV无码乱码1区久久| 久久国产女同一区二区| 亚洲最大成人网站| 人妻av中文字幕无码专区| 国产成人免费高清激情明星 | 2022AV一区在线| 中文字幕乱码亚洲一区二区三区| 国产午夜成人av在线播放| 亚洲h视频| 日本二区三区视频免费观看| 亚洲熟妇自偷自拍另类| 人人妻人人妻人人片av| 亚洲AV成人无码久久精品老人| 亚洲电影中文字幕| 丰满人妻一区二区三区52| 色偷偷色噜噜狠狠网站30根| 亚洲va中文字幕无码毛片| 亚洲手机国产精品| 亚洲成人免费久久av| 国产欧美日韩一区二区加勒比|