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        Local Regularity for a 1D Compressible Viscous Micropolar Fluid Model with Non-homogeneous Temperature Boundary

        2014-07-24 15:29:28SUNLinlinLIANGTiewangZHANGJianpeng

        SUN Lin-lin,LIANG Tie-wang,ZHANG Jian-peng

        (1.College of Science,Donghua University,Shanghai 201620,China;2.Department of Infomation and Arts Design,Henan Forestry Vocational College,Luoyang 471002,China)

        Local Regularity for a 1D Compressible Viscous Micropolar Fluid Model with Non-homogeneous Temperature Boundary

        SUN Lin-lin1,LIANG Tie-wang2,ZHANG Jian-peng1

        (1.College of Science,Donghua University,Shanghai 201620,China;2.Department of Infomation and Arts Design,Henan Forestry Vocational College,Luoyang 471002,China)

        In this paper,we discuss the local existence of Hi(i=2,4)solutions for a 1D compressible viscous micropolar fluid model with non-homogeneous temperature boundary. The proof is based on the local existence of solutions in[1].

        compressible Navier-Stokes equations;micropolar fl uid;the initial boundary value problem;non-homogeneous temperature boundary

        §1. Introduction

        The present paper is concerned with the local existence of Hi(i=2,4)solutions to the system of one-dimensionalcompressible viscous micropolar fluid modelwith non-homogeneous temperature boundary.This system is a kind of viscous compressible Navier-Stokes equations describing the motion of a heat-conducting micropolar fluid,which belongs to a class of fluids with nonsymmetric stress tensor called polar fluids.Precisely in the Lagrangian coordinate, such a system can be written as follows

        where for(x,t)∈[0,1]×[0,T](T>0)is the Lagrangian mass coordinate and

        denote stress,heat flux,pressure and internal energy,respectively and A>0 is a constant.In addition,

        denotes the density of the fluid.Meanwhile,we consider(1.1)~(1.5)subject to the following initial conditions

        and the following boundary conditions

        whereη0(x),v0(x),w0(x),θ0(x)are given functions.We also assume as in Nermina Mujakovic’s article

        where m>0 is a constant.

        The research of1Dcompressible Navier-Stokes system has obtained a great ofresults.Specifically,the crucialpoint to the research is that in 1D case under the Lagrangian coordinate,the specific volumeηcan be represented by other unknown variables,and the positive upper and lower bounds can be derived in the respective initialboundary problems.[2-4]have studied the Cauchy problem.As the domain is unbounded and the Poincar′e inequality is not available,the authors discussed it in small initial data condition.There are also a lot of works concerning the initial boundary problems(see,e.g.,[5-24]).They have obtained many results concerning the global existence,regularity and asymptotic behavior.Qin[2223]also obtained a series of properties about the exponential stability and attractors of the system.Recently,Mujakovi′c has studied the non-homogeneous boundary value problems,such as velocity boundary v,momentum w and temperatureθare non-homogeneous(see,e.g.,[1,25]).Actually,this paper is based on the local existence results in Mujakovi′c[1]and improves his result.

        In this paper,constants Ci(i=1,2,3,4)denote the universal constants depending on the Hi[0,1](i=1,2,3,4)spatial norms of(η0(x),v0(x),w0(x),θ0(x))and Wi,∞[0,T](i= 1,2,3,4)spatialnorms of(u0(t),u1(t)).

        Now,we state our main results in this paper

        Theorem 1 If(1.10)~(1.11)are satisfied,(η0(x),v0(x),w0(x),θ0(x))∈H2[0,1]and (u0(t),u1(t))∈W2,∞[0,T],then there exists a time 0≤T0≤T,such that problem(1.1)~(1.9) admits a H2-local solution(η(t,x),v(t,x),w(t,x),θ(t,x))∈L∞([0,T0),H2[0,1])and the following estimates hold for any t∈[0,T0),

        Theorem 2 If(1.10)~(1.11)are satisfied,(η0(x),v0(x),w0(x),θ0(x))∈H4[0,1]and (u0(t),u1(t))∈W3,∞[0,T],then there exists a time 0≤T0≤T,such that problem(1.1)~(1.9) admits a H4-local solution(η(t,x),v(t,x),w(t,x),θ(t,x))∈L∞([0,T0),H4[0,1])and the following estimates hold for any t∈[0,T0],

        We organize the paper as follows:Section 2 is asserted for the proof of Theorem 1 and Section 3 is arranged as for the proof of Theorems 2.

        §2. Local Existence in H2

        Lemma 2.1 Under the assumptions of Theorem 1.1,there exists a time 0≤T0≤T, such that for all t∈[0,T0),there holds

        Proof We can easily get(2.1)~(2.5)from Theorem 2.1 and Lemma 5.2 in[1].

        Lemma 2.2 The following estimate holds for all t∈[0,T0),

        Proof By Lemma 2.1 and the following inequalities

        and also from(1.1),

        we can get estimate(2.6).The proof is complete.

        Lemma 2.3 For all t∈[0,T0),there holds

        Proof Differentiating(1.2)with respect t,multiplying the resulting equation by vt,using Lemma 2.1,we deduce that

        Also from(1.2),using Lemma 2.1,the interpolation inequality and Young’s inequality,we have for anyε>0,

        which gives forε>0 smallenough,

        Similarly,we derive from(1.3)forε>0 smallenough,

        which gives

        Meanwhile,we can deduce from(1.3)forε>0 smallenough,

        which gives

        Similarly,we derive from(1.4)forε>0 small enough,

        which gives

        From(1.4),we can obtain,

        which gives for anyε>0,

        From Lemma 2.1 and(2.12),(2.15),we arrive

        As we know

        as(u0(t),u1(t))∈W2,∞[0,T]and‖θx‖L∞≤C1(‖θx‖1/2‖θxx‖1/2+‖θx‖),then we know that

        Thus the estimate(2.11)follow from(2.12),(2.14),(2.15),(2.17),(2.19),(2.23)and(2.26). The proof is complete.

        Lemma 2.4 For all t∈[0,T0),there holds

        Proof Diff erentiating(1.2)with respect to x,multiplying the resulting equation byηxx/η and using(1.1)(ηtxx=vxxx),we can see that for anyε>0

        which,combined with Lemma 2.1~Lemma 2.3,gives

        Differentiating(1.2)~(1.4)with respect to x respectively,using Lamma 2.1~Lemma 2.3,we can see that

        which gives(2.28).The proof is complete.

        Proof of Theorem 1 By Lemma 2.1~Lemma 2.4,we have proved the local existence of H2-solution of problem(1.1)~(1.9).

        §3. Local Existence in H4

        Lemma 3.1 Under the assumptions of Theorem 2,then for all t∈[0,T0),where T0is defined in Lemma 2.1,there holds

        whereεis a suffi ciently smallpositive constant.

        Proof We easily infer from(1.2)and Lemma 2.1~Lemma 2.4 that

        Diff erentiating(1.2)with respect to x and utilizing Lemma 2.1~Lemma 2.4,we have

        or

        Diff erentiating(1.2)with respect to x twice,using Lemma 2.1~Lemma 2.4 and the interpolation inequalities,we have

        or

        In the same manner,we deduce from(1.3)and(1.4)that

        or

        and

        or

        Diff erentiating(1.2)with respect to t and utilizing Lemma 2.1~Lemma 2.4,we deduce that

        which,together with(3.7),(3.9)and(3.14),implies

        Analogously,we derive from(1.3)~(1.4)and Lemma 2.1~Lemma 2.4 that

        which,combined with(3.11)~(3.14),(3.17)~(3.18)and(3.7),give

        Hence we obtain(3.1)~(3.2).

        Now diff erentiating(1.2)with respect to t twice,multiplying the resulting equation by vttin L2(?)and using(1.1)and Lemma 2.1~Lemma 2.4,we deduce

        which,along with(3.24),implies

        Thus estimate(3.3)follows from Lemma 2.1~Lemma 2.4,(3.2)and(3.28). Analogously,we obtain from(1.3)that

        which,integrated over(0,t),t∈[0,T0),implies

        Hence(3.4)follows.

        In the same way,we can obtain from(1.4)

        which implies

        i.e.,

        where

        As we know

        For estimating‖θxxt(t)‖2,we diff erentiate(1.4)with t and use Lemma 2.1~Lemma 2.4,to obtain that for anyε>0,

        So we get

        We also easily know that for anyε>0,

        By Lemma 2.1~Lemma 2.4,and the interpolation inequalities,we derive

        We can get

        Thus from(3.42)~(3.44)and Lemma 2.1~Lemma 2.4,it follows for anyε>0,

        As the interpolation inequality,we know that

        By(3.40)~(3.41),(3.46)~(3.47)and taking the supremum on the right-hand side of(3.43), we can obtain(3.5).The proof is complete.

        Lemma 3.2 For all t∈[0,T0),there holds for anyε>0,

        Proof See,e.g.,Lemma 2.5,[22]and(3.48)can be obtained immediately.

        Differentiating(1.3)with respect to x and t,multiplying the resulting equation by wtxin L2(?)and integrating by parts,we infer from(1.3)

        Differentiating(1.3)with respect to t and both to x and t respectively,we can see

        Hence it follows from(3.52)~(3.53)

        which leads to(3.49).

        Analogously,we also deduce from(1.4)and(3.52)

        and differentiating(1.4)with respect to t and x,we can see

        which,combined with Lemma 2.1~Lemma 2.4,(3.49)and the Young’s inequality,implies estimate(3.50).The proof is now complete.

        Lemma 3.3 For all t∈[0,T0),there holds

        Proof Adding up(3.3),(3.5),(3.48)and(3.50)and takingεsuffi ciently small,also utilizing the fact based on(3.48)

        we can immediately obtain(3.57).The proof ends here.

        Lemma 3.4 For all t∈[0,T0),there holds:

        Proof See,e.g.[24],Lemma 4.3.

        Lemma 3.5 For all t∈[0,T0),there holds:

        Proof Using(1.1),Lemma 2.1~Lemma 2.4 and Lemma 3.1~Lemma 3.4,we can derive estimates(3.61)~(3.62).The proof is complete.

        Proof of Theorem 2 By Lemma 3.1~Lemma 3.5,we have proved the local existence of H4-solution of problem(1.1)~(1.9).

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        tion:35Q30,35M33

        1002–0462(2014)01–0129–13

        Chin.Quart.J.of Math. 2014,29(1):129—141

        date:2013-06-28

        Supported by the NNSF of China(11271066);Supported by the grant of Shanghai Education Commission(13ZZ048)

        Biography:SUN Lin-lin(1989-),male,native of Zhoukou,Henan,a master candidate of Donghua University, engages in applied partial diff erential equations.

        CLC number:O175.29 Document code:A

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