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

        ?

        A m,p-Laplacian Parabolic Equation with Nonlinear Absorption and Boundary Flux

        2020-07-28 01:13:16LIUBingchen劉丙辰ZHANGChangcheng張長城WANGLu王璐
        應用數學 2020年3期
        關鍵詞:王璐長城

        LIU Bingchen(劉丙辰),ZHANG Changcheng(張長城),WANG Lu(王璐)

        (Department of Appiled Mathematics,China University of Petroleum,Qingdao 266580,China)

        Abstract: In this paper,we deal with a m,p-Laplacian equation of parabolic type in with inner absorption term (?λuκ) and nonlinear boundary flux uq.If q q?,both global solutions and blow-up solutions could exist depending on the choosing of initial data.In the balanced case q = q?,the size of the coefficient of the absorption term plays a fundamental role in distinguishing global solutions from blow-up solutions.All solutions exist globally for κ ≤1.If 1 <κ m(p?1)+p,there exist both global and blow-up solutions.

        Key words: m,p-Laplacian parabolic equation;Fujita-type blow-up;Global existence

        1.Introduction

        In this paper,we consider am,p-Laplacian equation of parabolic type The nonlinear diffusion equations (1.1) can be used to describe the nonstationary flow in a porous medium of fluids with a power dependence of the tangential stress on the velocity of displacement under polytropic conditions.

        The equation (1.1) without absorption,subject to nonlinear boundary flux (1.2),has been studied by WANG,et al.in[6](i.e.,λ=0).It was proved that the blow-up phenomena are caused by the nonlinear boundary flux and the Fujita exponent is denoted byqc:=(m+1)(p?1).The results are obtained as follows.

        (i) If 0≤q ≤q0:=(m+1)(p?1)/p,the solution is global;

        (ii) Ifq0

        (iii) Ifq >qc,both global solutions and blow-up solutions could exist.

        Recently,JIN,et al.[3]considered the parabolic equation ofp-Laplacian type,

        subject to the nonlinear boundarywhere constantsp>2,κ,q,λ>0.The critical Fujita absorption exponent has been firstly introduced in the critical case,which can be seen from the results:

        (i) Ifq

        (ii) Ifq >q?,then there exist both global solutions and blow-up solutions;

        (iii) Ifq=q?withλlarge,then all solutions exist globally;

        (iv) Letq=q?withλsmall.

        Ifκ ≤1,all solutions exist globally.

        If 1<κ<2p?1,the solutions blow up under any nontrivial nonnegative initial data.

        Ifκ >2p?1,there could be both global solutions and blow-up solutions for small and large initial data,respectively.

        The other works about the parabolic equations ofp-Laplacian type can be found in[1-2,4-5,8-10] and the papers cited there.

        To our knowledge,the system (1.1)-(1.3) has not been considered before.In this paper,we want to determine the critical Fujita absorption exponent for suchm,p-Laplacian equation(1.1)with absorption and boundary flux,and study how the absorption affects the global and blow-up solutions,inspired by [3,6].Moreover,we try to obtain the quantitative description about the coefficientλof the absorption term in distinguishing the existence of global solutions from blow-up solutions.

        The main results will be given in the next section.We also give some remarks about the influence of coefficients,the absorption and the boundary flux on the existence of global solutions and blow-up solutions of system (1.1)-(1.3).The proof of the main results can be found in Sections 3-6,respectively.

        2.Main Results and Remarks

        For convenience,we denote a positive constant It can be found thatq?= (m+1)(p?1)/pforκ <1 andq?= (κ+m)(p?1)/pforκ ≥1,respectively.The main results are as follows.

        Theorem 2.1(i) Ifq

        (ii) Ifq >q?,then both global solutions and blow-up solutions could exist.

        (iii) Letq=q?.If one of the following conditions holds,then all solutions exist globally.

        ? κ ≤1;

        ?1<κ

        where positive constantsr:=p/[m(p?1)?κ] andMsatisfies that

        for any compactly supportedu0(x);

        ? κ>m(p?1) andλ>(κ+m)(p?1)/p;

        ? κ=m(p?1) andλ>mp(p?1);

        (iv) Letq=q?.

        ?If 1<κ

        where constantsr,C,A,α,β,σsatisfy that for smallσ ∈(0,1) and large constantC,

        ?Ifm(p?1)≤κ

        ?Ifκ>m(p?1)+p,global solutions exist for small initial data while blow-up solutions exist for large initial data,respectively.

        Remark 2.1The results in Theoreom 2.1 are compatible with the ones of [3] if takingm=1.

        Remark 2.2There is a Fujita-type blow-up result in the exponent region

        which is equivalent to{(p?1)(m+1)

        Remark 2.3The results in Theoreom 2.1 show that the existence of global and blow-up solutions was influenced not only by the exponentsp,q,mbut also by the coefficient of the absorption term in the equation (1.1).Ifq q?,both global solutions and blow-up solutions exist depending on the choosing of initial data.The balanced caseq=q?is more interesting.The size of the coefficient of the absorption term plays a fundamental role in distinguishing global solutions from non-global solutions.In fact,forq=(κ+m)(p?1)/p,

        ?1<κ

        ? 1<κ

        ? m(p?1) ≤κ max{(κ+m)(p?1)/p,mp(p?1)}: global existence.

        ? m(p?1)≤κ

        3.Proof of Theorem 2.1 (i)

        wheneverMis large enough.We conclude that ˉuis a global super-solution to system (1.1)-(1.3) by using the comparison principle.

        4.Proof of Theorem 2.1 (ii)

        Next consider the caseq >q?.

        Proof of Theorem 2.1 (ii)Define

        Thenis a subsolution whenever the functionhsatisfies the inequalities

        and

        5.Proof of Theorem 2.1 (iii)

        6.Proof of Theorem 2.1 (iv)

        At the last section,we pay attention to the more interesting balanced caseq=q?.

        Proof of Theorem 2.1 (iv)Ifκ ≤1,thenq?= (m+1)(p?1)/p,and the solution always exists globally for anyλ ≥0 by the arguments for (i).Hence,it suffices to consider the caseκ>1,that is.Takeuas that for (ii) with

        we see that the above inequalities are ensured by

        Forλ<1,there exists some positive constantσ ∈(0,1)such thatλ ≤1?σ,and thus(6.2)is true.Furthermore,a direct calculation yields that(6.3)holds for appropriately large constantC.In addition,for anyu0(x)≠ 0,we haveprovided thatTis large enough,which means thatis a blow-up sub-solution according to the comparison principle.

        Finally,ifκ >m(p?1)+p,that is,q >(m+1)(p?1),it is known from [6] that the problem (1.1)-(1.3) withλ=0 admits global solutions for small initial data,and so does(1.1)-(1.3) withλ>0 according to the comparison principle.

        猜你喜歡
        王璐長城
        Wave nature of Rosensweig instability
        Static-to-kinematic modeling and experimental validation of tendon-driven quasi continuum manipulators with nonconstant subsegment stiffness
        “海上長城”豐盈關
        華人時刊(2023年9期)2023-06-20 08:31:10
        Bandgap evolution of Mg3N2 under pressure:Experimental and theoretical studies
        交互式教學在英語專業(yè)閱讀課改中的應用研究
        在地下挖一座“竊聽長城”(下)
        在地下挖一座“竊聽長城”(上)
        Improved Fibroblast Adhesion and Proliferation by Controlling Multi-level Structure of Polycaprolactone Microfiber
        守護長城
        直徑不超過2的無爪圖的2—因子
        91人妻无码成人精品一区91| 久久亚洲精品成人av无码网站 | 亚洲精品国产二区在线观看| 亚洲一区二区在线观看网址| 99精品国产一区二区三区| 久青草国产在线观看| 日本二区视频在线观看| av黄色在线免费观看| 久久精品无码av| 亚洲综合色秘密影院秘密影院| av资源在线永久免费观看 | 久久精品亚洲国产成人av| 亚洲亚色中文字幕剧情| 国产免费av片在线观看| 精品人妻中文av一区二区三区| 久久狠狠髙潮曰十八女人| 天天做天天爱夜夜夜爽毛片 | 99久久久无码国产精品性| 国产av人人夜夜澡人人爽| 最新在线观看精品国产福利片| av毛片亚洲高清一区二区| 中文字幕在线日亚州9 | 亚洲日韩av一区二区三区中文 | av在线一区二区精品| 人人做人人爽人人爱| 色妺妺在线视频| 国产男女猛烈无遮挡免费视频网址 | 午夜少妇高潮免费视频| 成人影片麻豆国产影片免费观看| 日韩免费无码一区二区三区| 精品无吗国产一区二区三区av| 蜜桃视频在线在线观看| 亚洲中文字幕一区精品自拍| 巨大欧美黑人xxxxbbbb| 久久国产精品国产精品久久 | 国产69精品久久久久777| 在线免费毛片| 人妻av中文字幕精品久久| 亚洲av无码无线在线观看| 国产成人无码精品午夜福利a| 亚洲区精品久久一区二区三区女同|