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        Periodic Solutions for Some Second Order Systems with Gyroscopic Forces

        2016-06-05 15:00:58MENGFengjuan
        關(guān)鍵詞:系統(tǒng)

        MENG Fengjuan

        Periodic Solutions for Some Second Order Systems with Gyroscopic Forces

        MENG Fengjuan

        (School of Mathematics and Physics,Jiangsu University of Technology,Changzhou 213001,Jiangsu)

        In this paper,the periodic solutions for second order non-autonomous differential systems with gyroscopic forces are investigated,by applying the least action principle and minimax methods,some existence results of periodic solutions are obtained.

        periodic solution;critical point;variational method

        1 Introduction

        In this paper,we are concerned with the existence of periodic solutions for the following second order system:

        where T>0,A is a real antisymmetry constant matrix and F:[0,T]×RN→R satisfies the following assumption:

        (H)F(t,x)is measurable in t for each x∈RNand continuously differentiable in x for a.e.t∈[0,T],and there exist a∈C(R+,R+),b∈L1([0,T]; R+)such that

        for all x∈RNand a.e.t∈[0,T].

        The term A u(t)means that the system has a gyroscopic force(see[1]).For more background,see[2-4]and the references therein.System(1)was mentioned by Ekeland[5]as possible extensions of his basic examples by modern variational methods,but without concrete work.

        For the case of A=0,system(1)reduces to the following second order Hamiltonian system

        The existence of periodic solutions for(2)was first considered by Berger and Schechter in[6]under the coercive condition.From then on,problem(2)has been extensively studied,many solvability conditions are obtained,such as:the coercivity condition;the convexity conditions;the sublinear nonlinearity conditions;the subquadratic potential conditions;the superquadratic potential conditions;the periodicity conditions and the even type potential condition(See[7-8]and the references therein).

        For the case of system(1),in[9-10],the authors have studied the existence of periodic solutions under superquadratic potential conditions and the subconvex condition respectively;in[11-14],Han etc.have investigated the existence of periodic solutions under the sublinear nonlinearity.

        where 0≤α<1 and f,g∈L1([0,T];R+).

        In this paper,we will consider the case of α=1.Furthermore,we will weak the Ahmad-Lazer-Paul condition

        where β is a constant,which has been extensivelyused in the literature.Our main results complete and develop some known results.

        2 Preliminaries

        We first introduce some notations,inequalities and variational structure of(1),which will be used in our main results.={u:[0,T]→RN|u is absolutely continuous,

        with the norm

        for all u∈H1T.

        one has Sobolev’s inequality

        and Wirtinger’s inequality

        for all u∈H1T(see Proposition 1.3 in[7]),where

        Lemma 2.1[11-12]Define the corresponding functional φ onby

        It follows from the assumption(H)that φ is continuously differentiable and the solutions of problem(1) corresponding to the critical points of φ.Moreover,one has

        3 Main results

        For convenience,we denote various positive constants as Ci,i=1,2,….Now we give our main results.

        Theorem 3.1 Suppose that F(t,u)satisfies condition(H).Moreover,we have the following assumptions: (i)‖A‖where‖A‖ i s the norm of A as a linear operator from RNto RN;

        (ii)there exist f,g∈L1([0,T];R+)withsuch that

        f

        or all x∈RNand a.e.t∈[0,T];

        (iii)

        Then problem(1)has at least one solution which minimizes φ on

        then a>0.It follows from(ii)and Sobolev’s inequality and Young inequality that

        as‖u‖→∞ by(iii)and

        By Theorem 1.1 and Corollary 1.1 in[7],the proof is completed.

        Remark 3.2 In[12],Han proved the corresponding results when F(t,x)is sublinear growth,i.e.(3)holds.Theorem 3.1 is a complementary and development of this result corresponding to α=1.

        Corollary 3.3 Suppose that A=0 and F(t,u) satisfies condition(H)and(ii),(iii)in Theorem 3.1,then problem(2)has at least one solution which minimizes φ on

        Remark 3.4 Corollary 3.3 improves Corollary 3 in[15].Instead of(iii),Corollary 3 in[15]requires Ahmad-Lazer-Paul condition

        It is easy to see that(iii)in Theorem 3.1 is weaker that(7).

        Theorem 3.5 Suppose that F(t,u)satisfies condition(H),and(i)in Theorem 3.1 holds.Moreover,assume F satisfies

        (iv)there exist h,k∈L1([0,T];R+)with‖A‖)such that for every ε>0 there exists C(ε)

        for all x∈RNand a.e.t∈[0,T];

        (v)

        where M will be specialized in the proof.Then problem(1)has at least one solution in H1T.

        Proof We will accomplish the proof by three steps.

        Step 1 First,we prove that φ satisfies the(PS) condition.Assume that{un}is a(PS)sequence for φ,that is{φ(un)}is bounded and φ'(un)→0 as n→∞.In a similar way to(6),we have

        for large n.It follows from Wirtinger’s inequality that

        for all n,thus we can get

        Similar to(6),we can estimate

        Combining with(8)and Young inequality,we can estimate

        It follows from the boundedness of φ(un)and(8) and(9),we have

        for all large n.From(v),by choosing ε small enough such that M >C11ε,combining with(10),we can deduce that{珔un}is bounded.Hence{un}is bounded in H1Tby(8).In a way similar to the proof of Proposition 4.1 in[7],see also the proof of Theorem 2.1 in[12],we conclude that the(PS)condition is satisfied.

        In fact,similar to(6),we have

        Step 3 By(v),we can easily find thatx)dt→+∞ as|x|→∞ for all x∈RN.Hence we can obtain that

        Combining with step 1 to 3,by applying the Saddle Point Theorem 4.6 in[16],the proof is completed.

        Remark 3.6 In[12],Han proved the corresponding results when F(t,x)is sublinear growth,i.e.(3)holds.Theorem 3.5 is a complementary and development of this result corresponding to α=1.

        Corollary 3.7 Suppose that F(t,u)satisfies condition(A)and(iv),(v)in Theorem 3.5,then problem(2)has at least one solution which minimizes φ on

        Remark 3.8 Under conditions(3)and(4),in[17],Tang proved the problem(2)has at least one solution in Theorem 1 and Theorem 2.Our Corollary 3.3 and Corollary 3.7 is a complementary and development of Theorem 1 and Theorem 2 in[17]respectively.

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        [17]TANG C L.Periodic solutions for nonautonomous second order systems with sublinear nonlinearity[J].Proc Am Math Soc,1998,126:3263-3270.

        [18]居加敏,王智勇.一類帶阻尼項(xiàng)的次二次二階Hamilton系統(tǒng)的周期解[J].四川師范大學(xué)學(xué)報(bào)(自然科學(xué)版),2015,38(3):329-332.

        [19]葉一蔚.具有變號(hào)位勢(shì)的二階Hamilton系統(tǒng)周期解的存在性定理[J].四川師范大學(xué)學(xué)報(bào)(自然科學(xué)版),2013,36(3): 337-341.

        [20]賀鐵山,陳文革,雷友發(fā).二階離散Hamiltonian系統(tǒng)的多重變號(hào)周期解[J].四川師范大學(xué)學(xué)報(bào)(自然科學(xué)版),2010,33(4):462-466.

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        帶gyroscopic項(xiàng)的二階系統(tǒng)周期解的存在性

        孟鳳娟

        (江蘇理工學(xué)院數(shù)理學(xué)院,江蘇常州213001)

        利用臨界點(diǎn)理論中的極小作用原理和極小極大方法,研究了帶有g(shù)yroscopic項(xiàng)的二階非自治微分系統(tǒng)周期解的存在性,得到了一些新的可解條件,推廣和改進(jìn)了已有的結(jié)果.

        周期解;臨界點(diǎn);變分方法

        O175

        A

        1001-8395(2016)05-0643-06

        2015-07-27

        國(guó)家自然科學(xué)基金(11526100)、江蘇省高校自然科學(xué)基金(15KJB110005)和江蘇省青藍(lán)工程作者簡(jiǎn)介:孟鳳娟(1982—),女,副教授,主要從事非線性泛函分析的研究,E-mail:fjmeng@jsut.edu.cn

        10.3969/j.issn.1001-8395.2016.05.005

        (編輯 周 俊)

        date:2015-07-27

        s:This work was supported by NSFC Grant(11401459),Natural Science Fund For Colleges and Universities in Jiangsu Province (15KJB110005)and Qinglan Project of Jiangsu Province

        2010 MSC:34C25;58E05;58K05

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