擬周期平面振子平衡點的穩(wěn)定性

邢秀梅,任秀芳

(1.伊犁師范學院 數(shù)學與統(tǒng)計學院,新疆 伊寧 835000;2.南京農(nóng)業(yè)大學 理學院數(shù)學系,南京 210095)

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擬周期平面振子平衡點的穩(wěn)定性

邢秀梅1,任秀芳2

(1.伊犁師范學院 數(shù)學與統(tǒng)計學院,新疆 伊寧 835000;2.南京農(nóng)業(yè)大學 理學院數(shù)學系,南京 210095)

利用主積分方法,將周期系統(tǒng)平衡點的穩(wěn)定性判據(jù)推廣到擬周期情形,即證明擬周期二階微分方程x″+h(t)x′+a(t)x2n+1+e(t,x)=0(n≥1)平衡點x=x′=0的穩(wěn)定性,其中h(t),a(t),e(t,x)是擬周期系數(shù),其頻率向量滿足Diophantine條件,且在x=x′=0附近,|e(t,x)|=O(x2n+2).結(jié)果表明,具有變號阻尼項擬周期振子的平衡點在一定條件下具有穩(wěn)定性.

擬周期;Diophantine條件;平衡點穩(wěn)定性

0 引 言

近年來,對擬周期微分方程的研究受到人們廣泛關注.關于周期微分方程平衡點穩(wěn)定性的研究已有許多結(jié)果[1-9].儲繼峰等[1]考慮具有一個半自由度的阻尼震蕩系統(tǒng)：

(1)

(2)

本文將劉期懷等[2]的相關結(jié)果推廣到擬周期微分方程：即在方程(2)中,要求e(t,x)在x=0附近滿足|e(t,x)|=O(x2n+2),h(t),a(t),e(t,x)關于t,x是實解析的,并且關于t是擬周期函數(shù),相應的頻率向量(ω1,ω2,…,ωm)滿足Diophantine條件：即存在常數(shù)γ>0和τ>m-1,使得對一切k=(k1,k2,…,km)≠0,都有

(3)

其中|k|=|k1|+|k2|+…+|km|.

1)方程(2)的平衡點x=x′=0是穩(wěn)定的;

1 典則變換

(4)

相應的Hamiltonian函數(shù)為

(5)

(6)

(7)

(8)

考慮輔助系統(tǒng)

(9)

令c=|[c]|[b]n+1.記(C(t),S(t))是方程(9)的滿足初始條件(C(0),S(0))=(1,0)的周期解.令T>0為其最小正周期,則這些函數(shù)滿足下列條件:

(10)

2 不穩(wěn)定性的證明

1)首先,引進典則變換:

則Hamiltonian函數(shù)(8)變?yōu)?/p>

(11)

其次,定義一個與時間相關的典則變換:

其中

(12)

它關于t是擬周期的.則變換后的Hamiltonian函數(shù)(11)具有如下形式:

其中

(13)

令

(14)

利用式(12)和2β>1,得

(15)

2)不穩(wěn)定性的證明.考慮關于變量λ,φ的動力系統(tǒng)

(16)

首先,證明存在一個φ*和0<υ<1,使得ψ(φ*)=0,并且當|φ-φ*|≤υ時,下述結(jié)論成立:

(17)

事實上,由式(10)有

并且

記m=min{|ψ(φ*+υ)|,|ψ(φ*-υ)|}.對于系統(tǒng)(16),存在常數(shù)r0>0,使得當|λ|≤r0時,下述不等式成立：

(19)

其次,定義角形區(qū)域Sε={(λ,φ)||λ|≤ε,|φ-φ*|≤υ},則必存在一點(λ0,φ0)∈Sε和某一時刻t*<0,使得λ(t*,λ0,ψ0)≥r0.

事實上,否則方程(16)的負向解屬于集合

(20)

3 穩(wěn)定性的證明

1)由于[c]>0,所以典則變換Φ1將Hamiltonian函數(shù)(8)變?yōu)?/p>

(21)

其中：

顯然f1(t,θ)關于t的均值為零、關于θ是1周期的.

2)利用典則變換Φ2,使變換后的Hamiltonian函數(shù)(21)具有如下形式:

其中

(22)

(23)

(24)

(25)

可得

(26)

對于固定的t,解λ,φ在每一時刻t關于φ0連續(xù),相應的積分曲線形成了t軸的管狀領域.由解的存在唯一性知,該管狀內(nèi)出發(fā)的解永遠位于管狀領域內(nèi).由于該管狀領域大小由ε控制,而且ε可任意小,因此得到系統(tǒng)(23)的不動點λ=0是穩(wěn)定的.

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(責任編輯：趙立芹)

StabilityoftheEquilibriumofQuasi-periodicPlanarOscillator

XING Xiumei1,REN Xiufang2

(1.SchoolofMathematicsandStatistics,YiliNormalUniversity,Yining835000,XinjiangUygurAutonomousRegion,China;2.DepartmentofMathematics,CollegeofScience,NanjingAgriculturalUniversity,Nanjing210095,China)

We generalized the stability criteria for the equilibrium of the periodic system to those for that of quasi-periodic system,applying the method of main integration.Concretely,we showed the stability for the equilibriumx=x′=0 of the quasi-periodic second order differential equationx″+h(t)x′+a(t)x2n+1+e(t,x)=0,n≥1,whereh(t),a(t),e(t,x)are quasi-periodic coefficients,whose frequency vectors meet the requirements proposed by Diophantine.And moreover,|e(t,x)|=O(x2n+2)nearx=x′=0.The results we obtained also imply that,under some conditions,the equilibrium of the quasi-periodic oscillator with damping changing sign can still be stable.

quasi-periodic;Diophantine condition;stability of the equilibrium

10.13413/j.cnki.jdxblxb.2015.03.07

2014-10-27.< class="emphasis_bold">網(wǎng)絡出版時間

時間：2015-02-11.

邢秀梅(1973—),女,漢族,博士,講師,從事Hamiltonian系統(tǒng)的研究,E-mail:xingxm09@163.com.通信作者:任秀芳(1982—),女,漢族,博士,講師,從事擬周期動力系統(tǒng)的研究,E-mail:xiufangren@gmail.com.

國家自然科學基金(批準號:21364016)、新疆維吾爾自治區(qū)自然科學基金(批準號:20122111328)和新疆維吾爾自治區(qū)重點學科項目(批準號:2012ZDXK13).

http://www.cnki.net/kcms/detail/22.1340.O.20150211.1126.001.html.

O175.13

：A

：1671-5489(2015)03-0383-06