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

        ?

        GLOBAL EXISTENCE OF CLASSICAL SOLUTIONS TO THE HYPERBOLIC GEOMETRY FLOW WITH TIME-DEPENDENT DISSIPATION?

        2018-07-23 08:41:10DexingKONG孔德興
        關(guān)鍵詞:劉琦德興

        Dexing KONG(孔德興)

        School of Mathematical Sciences,Zhejiang University,Hangzhou 310027,China

        E-mail:dkong@zju.edu.cn

        Qi LIU(劉琦)?

        Department of Applied Mathematics,College of Science,Zhongyuan University of Technology,Zhengzhou 450007,China

        E-mail:21106052@zju.edu.cn

        Abstract In this article,we investigate the hyperbolic geometry flow with time-dependent dissipation on Riemann surface.On the basis of the energy method,for 0<λ≤1,μ>λ+1,we show that there exists a global solution gijto the hyperbolic geometry flow with time-dependent dissipation with asymptotic flat initial Riemann surfaces.Moreover,we prove that the scalar curvature R(t,x)of the solution metric gijremains uniformly bounded.

        Key words Hyperbolic geometry flow;time-dependent damping;classical solution;energy method;global existence

        1 Introduction

        Let M be an n-dimensional complete manifold with Riemannian metric gij.The following general version of hyperbolic geometry flow

        was introduced by Kong and Liu in[4],where Rijis the Ricci curvature tensor of metric gijand Fijare some smooth functions of g andThe most important three cases are so-called standard hyperbolic geometry flow[5,6],the Einstein’s hyperbolic geometry flow[8],and the dissipative hyperbolic geometry flow[1,10].

        In this article,we are concerned with the hyperbolic geometry flow with time-dependent dissipation

        with the initial metric on a Riemann surface

        where u0(x1,x2)>0 is a smooth function.

        In fact,on a surface,the metric can always be written(at least locally)in the following form

        where u(t,x1,x2)>0 is a smooth function.Therefore,we have

        Thus,equation(1.2)becomes

        Denote

        then,equation(1.6)becomes

        Forμ=0,(1.2)is the standard hyperbolic geometry flow.In this case,Kong,Liu,and Xu[6]investigate the solution of equation(1.2)in one space dimension.They prove that the solution can exist for all time by choosing a suitable initial velocity.On the other hand,if the initial velocity tensor does not satisfy the condition presented in[6],the solution blows up at a finite time.Later,Kong,Liu,and Wang[5]consider the Cauchy problem for the hyperbolic geometry flow in two space variables with asymptotic flat initial Riemann surfaces,and give a lower bound of the life-span of classical solutions to the hyperbolic geometry flow.

        Forμ>0,λ=0,(1.2)is the dissipative hyperbolic geometry flow.Liu[10]studies the solution of equation(1.2)in one space dimension and gains the similar results with Kong,Liu,and Xu[6].Kong,Liu,and Song[7]shown(1.2)that admits a global existence and established the asymptotic behavior of classical solutions to the dissipative hyperbolic geometry flow in two space variables.

        Forμ >0 and λ >0,it is natural to ask:does the smooth solution of(1.2)blows up in finite time or does it exist globally?

        In this article,we are interested in the hyperbolic geometry flow(1.2)with time-dependent dissipation in two space variables,that is,we consider the Cauchy problem for equation(1.8)with the following initial data

        Throughout this article,we denote the general constants by C.[1,+∞],denotes the usual Sobolev space with its norm

        We also always denote?k= ?xkand ?kl= ?xkxl.

        The main results of this article can be described as follows.

        Theorem 1.1Let 0< λ ≤ 1 and μ > λ+1.Suppose thatandis sufficiently small.Then,there exists a unique,global,classical solution of(1.8)–(1.9)satisfying

        Theorem 1.2Under the assumptions mentioned in Theorem 1.1,the Cauchy problem(1.8)-(1.9)has a unique classical solution for all time;moreover,the scalar curvature R(t,x)corresponding to the solution metric gijremains uniformly bounded,that is,

        where M is a positive constant,depending on the Hsnorm of φ0(x)and the Hs?1norm of φ1(x),but independent of t and x.

        Remark 1.3Our main result,Theorem 1.1,gives a global existence of the classical solution of Cauchy problem(1.8)–(1.9).The theorem shows that,under suitable assumptions,the smooth evolution of asymptotic flat initial Riemann surfaces under the dissipative flow(1.2)exists globally on[0,+∞).

        Remark 1.4Our main result,Theorem 1.1,gives a global existence of the classical solution of Cauchy problem(1.8)–(1.9)for 0< λ ≤ 1,μ> λ+1,while for the case 0<λ ≤ 1,μ≤λ+1,we have no idea to prove the global existence or blow up of the classical solution of the Cauchy problem.This implies that the relatively “l(fā)arge” dissipation has contribution to existence of the global solution,but for the relatively “small” dissipation,it is still unknown.

        Set s≥4.Define

        Moreover,we assume that for any t≥0,

        where K>0 is a suitably large constant.By Sobolev inequality,we have

        Because(1.8)implies

        we have

        Let us indicate the proofs of Theorem 1.1.As in[2,11],in the following sections,we will eventually show thatwhenis assumed for some suitably large constant K>0 and small ε>0.Based on this and a continuous induction argument,the global existence of φ and then the main Theorem 1.1 are established for 0<λ≤1,μ>λ+1.

        The rest of the article is arranged as follows.In Section 2,we will obtain the elementary estimate to the solution of(1.8)by using energy method.In Section 3,the estimates to higher derivatives will be considered,under which we show the global existence to the solution of the Cauchy problem(1.8)–(1.9),and prove the boundness of scalar curvature R(t,x)corresponding to the solution metric,that is,Theorem 1.1 and Theorem 1.2.

        2 Elementary Energy Estimates

        The equation(1.8)can be rewritten as

        On one hand,multiplying(2.1)by m(1+t)2λφt,we have

        where m>0 will be determined later.Integrating it over R2×[0,t]yields

        On the other hand,multiplying(2.1)by(1+t)λφ,we have

        Integrating it over R2×[0,t]yields

        For λ=1,combining(2.3)and(2.5),we obtain

        As μ >2,then letμ =2+4δ,where δ>0.Using Cauchy-Schwartz inequality,we have

        in the left hand of(2.6)are all positive.Therefore,

        For 0<λ<1,combining(2.3)and(2.5),we obtain

        Becauseμ > λ+1,then letμ = λ+1+4δ,where δ>0.Using inequality(2.7),and choosingit is easy to show that the coefficients in the left hand of(2.9)are all positive.Therefore,

        It follows from(2.8)and(2.10)that

        where

        and

        Because

        thus,

        Now,we consider I2.

        Thus,

        By combining the above estimates,we get

        Thus,

        provided ε small enough.

        3 Estimates on Higher Derivatives

        The estimate as(2.19)can also be obtained for higher derivatives.In fact,by multiplying(2.1)bywe have

        Integrating it over R2×[0,t]yields

        where

        Because

        we have the followings:

        First

        thus,

        Next,we consider I12,

        thus,

        For I13,we have

        thus,by(3.6),(3.8),and(3.9),we obtain

        Now,we consider I2.

        Thus,

        By combining the above estimates,we get

        Summing k from 1 to 2,we have

        provided ε small enough.

        Combining(2.19)and(3.14)gives

        Moreover,we can prove that for any positive number m,

        Therefore,

        Choosing K>0 large and ε small,by Gronwall’s inequality,one get,for any t ≥ 0,

        Thus,on the basis of the above discussion,we prove the main theorem 1.1 by the assumption that E(t)≤ K2ε2and a continuous induction argument.

        We finally estimate the scalar curvature R(t,x).By the definition,we have

        Noting(1.7),we obtain from(3.19)

        Using(1.14),we have

        where 0< λ ≤ 1,M is a positive constant,depending on the Hsnorm of φ0(x)and the Hs?1norm of φ1(x),but independent of t and x.Thus,this prove Theorem 1.2.

        猜你喜歡
        劉琦德興
        From decoupled integrable models tocoupled ones via a deformation algorithm*
        咕咕叫的肚皮
        初心引航,構(gòu)建“雙減”新樣態(tài)
        大戰(zhàn)章魚博士
        麥香——一『廳級農(nóng)民』趙德興
        江西銅業(yè)集團(tuán)(德興)鑄造有限公司
        江西銅業(yè)集團(tuán)(德興)實(shí)業(yè)有限公司
        江西銅業(yè)集團(tuán)(德興)鑄造有限公司
        DFT study of solvation of Li+/Na+in fluoroethylene carbonate/vinylene carbonate/ethylene sulfite solvents for lithium/sodium-based battery?
        一壟地
        金山(2017年9期)2017-09-23 19:54:19
        中文字幕乱码免费视频| 极品粉嫩小仙女高潮喷水操av | 亚洲av无码国产综合专区| 国产欧美日韩一区二区三区在线| 国产精品白浆一区二区免费看| 日韩在线精品视频免费| 国内自拍速发福利免费在线观看| 在线天堂www中文| 人妻夜夜爽天天爽三区麻豆AV网站| 国产 在线播放无码不卡| 亚洲本色精品一区二区久久 | 日韩av一区二区蜜桃| 风情韵味人妻hd| 久久久久久久女国产乱让韩| 美女窝人体色www网站| 亚洲免费在线视频播放| 国产日韩av在线播放| 色av综合av综合无码网站| 青青青草国产熟女大香蕉| 国语对白精品在线观看| 中文字幕乱码熟妇五十中出 | 天天插天天干天天操| 亚洲精品美女中文字幕久久| 国产精品186在线观看在线播放| 免费看久久妇女高潮a| 深夜福利国产| 国产在线观看视频一区二区三区| 国色天香精品一卡2卡3卡4| 欧美第五页| 亚洲av精品一区二区| 亚洲最新无码中文字幕久久| 精品人妻人人做人人爽夜夜爽| 精品久久杨幂国产杨幂| av在线免费观看麻豆| 亚洲日韩av无码一区二区三区人 | 99国产精品视频无码免费 | 日本一区二区三区四区啪啪啪| 男女啪动最猛动态图| h在线国产| av男人的天堂第三区| 一本色道久久88加勒比—综合 |