可应用于控制系统分析与设计的一种图示法

(一)限于实数值的复变数多项式的图示以往数学教科书中实变数 x 的多项式R_r=f(x)≡a_0x~n+a_1x~(n-1)+…+a_(n-1)x+a_n(1)在(x,R)平面中的图线不能对于每一个实数R_r 都有 n 个交点.因此不能在图上显示"n 次 ...     

一个新的运动稳定性判据

1.引言运动稳定性的判据有很多种,例如Routh-Hurwitz准则、Nyquist准则、谢绪恺判据等。不过,这些判据都需要知道线性系统的特征多项式,而由线性方程组的系数矩阵计算特征多项式需要大量的计算工作。李森林给出了一个利用系数矩阵判别系统稳定的充分条件,使用这个条件需要计算n个n-1阶行列式和一个n阶行列式。由于这个条件仅仅是充分的,因此,当计算结果满足这个条件时是能说明问题的;如果不满足这一条件,计算结果便毫无用处。尽管如此,在参考文献[4]中仍认为此法“比用其他方法来判定要简单得多(尤其当n很大时),所以在实际工作中可     

关于均匀变形问题的一种解答方法——讨论一个弹性力学习题的解

徐芝纶编《弹性力学》上册(1979)有这样一个习题(见该书习题 S—2):设某一物体发生如下的位移u=a_0 a_1x a_2y a_3zv=b_0 b_1x b_2y b_3zw=c_0 c_1x c_2y c_3z试证明:各个形变分量在物体内为常量(即所谓均匀变形);在变形以后,物体内的平面保持为平面,直线保持为直线,平行面保持平行,平行线保持平行,正平行     

关于均匀变形问题的一种解答方法——讨论一个弹性力学习题的解

徐芝纶编《弹性力学》上册(1979)有这样一个习题(见该书习题 S-2):设某一物体发生如下的位移u=a_0+a_1x+a_2y+a_3zv=b_0+b_1x+b_2y+b_3zw=c_0+c_1x+c_2y+c_3z试证明:各个形变分量在物体内为常量(即所谓均匀变形);在变形以后,物体内的平面保持为平面,直线保持为直线,平行面保持平行,平行线保持平行,正平行 ...     

对《线性算子方程组一般解的代数构造》的补充说明

在[1]的引言中指出:“a_(ii)是作用于线性空间M上的线性算子,属于可交换环R,u_i∈M(i=1,2,…,N).本文考虑的线性算子都是R中的元素,并且假设对任一P∈R,若P≠0,则对线性空间Ⅳ中任一元素f恒有u∈M使PU=f”,因此使用文[1]中的结论除满足定理的条件外,还需满足引言中的条件,例如文中用到的算子都必须属于R.如果将R理解为由线性常系数偏微分算子构成的环,并且D_i/D_(i-1)等不是线性常系数偏微分     

NEWTON METHOD FOR SOLVING A CLASS OF SMOOTH CONVEX PROGRAMMING

1ConvexProgrammingandExactPenaltyFunction Weconsiderthefollowingconvexprogramming:(P)minf(x)s.t.x∈S={x∈Rn:gi(x)≤0,i=1,…,m}.SupposethatSisacompactset.ThusthereexistsalargeboundedboxX,suchthatS={x∈Rn:gi(x)≤0,i=1,…,m}intX.Assumethatf(x),gi(x),i=1,…,m     

Singular perturbation of nonlinear vector boundary value problem

In this paper we study the perturbed boundary value problem of the form dx/dt=f(x,y,t;ε), εdy/dt=g(x,y,t;ε), a_1(ε)x(0,ε)+a_2(ε)y(0,ε)=a(ε) b_1(ε)x(1,ε)+εb_2(ε)y(1,ε)=β(ε)in whichx,f,β∈E~m, y,g,a∈E~n, 0<ε(?)1and a_1(ε), a_2(ε), b_2(ε)and b_2(ε) are matrices of the appropriate size. Under the condition that g_y(t) is nonsingular and other suitable restrictions, the existence of the solution is proved, the asymptotic expansion of solution of order n is constructed, and the remainder term is estimated.     

EPSILON-ALGORITHM AND ETA-ALGORITHM OF GENERALIZED INVERSE FUNCTION-VALUED PAD APPROXIMANTS USING FOR SOLUTION OF INTEGRAL EQUATIONS

IntroductionLetf(x ,λ)beagivenpowerserieswithfunction_valuedcoefficients,i.e.,f(x ,λ) =c0 (x) +c1(x)λ+c2 (x)λ2 +… +cn(x)λn+… ,( 1 )wherecj(x)isarealorcomplexfunctionwithregardasxwhichisdefinedon (a ,b) .Supposethatf(x,λ)isanalyticasafunctionofλattheoriginλ=0 .ItisknownthatPad啨ａｐｐｒｏｘｉｍａｎｔｍｅｔｈｏｄｓａｒｅｕｓｅｄｆｏｒｏｂｔａｉｎｉｎｇｔｈｅｓｏｌｕｔｉｏｎｏｆａｗｋｗａｒｄｉｎｔｅｇｒａｌｅｑｕａｔｉｏｎｓ,andespeciallythosewhichpossessageneratingfunctionoftheform ( …     

食饵-捕食者相互作用系统的定性分析

本文运用Liapunov第二方法，研究了食饵-捕食者系统｛x^·=f(x)-φ(x)τ(y)y^·=-eh(y) kh(y)φ(z)正平衡点的稳定性，并利用Poincare-Bendixon环域定理及张芷芬唯一性定理，论证了在R2^ =｛(x,y):x>0,y>0｝内极限环的存在唯一性及其稳定性。     

运动稳定性基本定理的一个注记

在某些实际情况下,难以构造满足 Liapunov 稳定定理的正定函数 V(t,x)。本文定理给出的条件使函数V(t,x)及 V(t,x)均可以是变号函数,因此既不要求 V(t,x)为正定,也不要求 V(t,x)为常负。文末给出了应用本文定理的实例。     

On the existence of periodic solutions for nonlinear system with multiple delays

IntroductionInthispaper,westudyT_periodicsolutionsofthefollowingnonlinearsystemwithmultipledelays x(t) =f(t,x(t) ,x(t-τ1(t) ) ,… ,x(t -τm(t) ) ) ,(1 )wherex(t) ∈C(R ,R) ,fiscontinuous,f(t+T ,·) =f(t,·) ,τi(t) (i=1 ,2 ,… ,m)arecontinuousperiodicfunctionsofperiodT .AlemmaisintroducedfordiscussingtheexistenceofT_periodicsolutionofsystem (1 ) .LetXbeaBanachSpace ,considerthefollowingoperatorequation :Lx =λNx　　 (λ∈ [0 ,1 ] ) ,whereL :DomL∩X→Xisalinearoperator,λ∈ [0 ,1 ]isapa…     

Global linear and quadratic one-step smoothing newton method for vertical linear complementarity problems

IntroductionLetN ∈Rm0 ×n(m0 ≥n)beaverticalblockmatrixoftype(m1,… ,mn) ,q∈Rm0 beaconstantvectorpartitionedconformablywithN ,thatareN =N1Nn,　q =q1qn,　m0 = ni=1mi,whereNi ∈Rmi×n,qi ∈Rmi,i ∈I =1 ,… ,n .WeconsidertheverticallinearomplementarityproblemVLCP(N ,q)associatedwith (N ,q)offindingavectorx∈Rnsuchthatx≥ 0 ,　si(x) :=Nix+qi ≥ 0 ,　xi∏mij=1sij(x) =0　　 (i∈I) ,wherexi,sij(x)denotetheithcomponentofxandthejthcomponentofsi(x) ,respectively ;∏ mj=1ajdenotesa1…am.Iti…     

Bifurcations of travelling wave solutions for a coupled nonlinear wave system

Introduction FangShaomeiandGuoBoling[1]consideredthefollowingtimeperiodicproblemof dampedcouplednonlinearwaveequations:ut f(u)x-αuxx βuxxx 2vvx=G1(u,v) h1(x),vt-γvxx 2(uv)x g(v)x=G2(u,v) h2(x),(1)whereα,β,γareconstants,andγ>0,β≠0.Undertheperiodicboundaryconditions,the authorsobtainedtheuniqueexistenceofstrongsolutionsfortheabovesystem.InthispaperweshallconsiderbifurcationbehaviorofthetravellingwavesolutionsofEq.(1)inthecaseGi(u,v)≡0,hi(u,v)≡0(i=1,2).Letξ=x-ct,u=u(x-ct),where cis…     

有随机常系数的Rayleigh方程及其应用

本文研究具有随机系数的耳Rayleigh微分方程x ω~2x ∈(-αx βx~3)=0。作者提出一个方法,分析有随机常系数Rayleigh方程解过程x(t)的统计性质。文中给出的实例,表明用本文的方法分析乳钢机打滑对的自激振动是有效的。     

Asymptotic theory of initial value problems for nonlinear perturbed Klein-Gordon equations

Introduction InthispaperasymptotictheoryofthefollowinginitialvalueproblemforanonlinearKlein Gordonequationisconsidered.tt-Δ =εF(t,x,,ε),t>0,x∈R2,(0,x,ε)=0(x,ε),t(0,x,ε)=1(x,ε),x∈R2,(1)where(t,x)isarealvaluedunknownfunction,Δ=2i     

子波变换及其对湍流的应用(Ⅱ)

<正> 4 离散子波变换 4.1 子波标架 4.1.1 定义在某种意义上,分析(6)和综合(8)两个公式就好像函数在进行运算,其中,它构成L~2(R)的一个正交完全集:在这个基础上f(x)的分解的系数由(6)给出,而根据这些系数的f(x)的重构则由(8)给出.其实,对于连续的情形,函数的集是高度冗余的.是否有可能选取一个称为“子波标架(waVelet frame)”的一个子集F,使得会构成一个对于L~2(R)是几乎正交的完全集呢?回答是肯定的,不     

Extended graphical representation of polynomials with applications to cybernetics

In this paper,the polynomial of a complex variable s(≡x iy)with realcoefficients K=a_0s~n a_1s~(n-1) …… a_(n-1)s a_n.is graphically represented by three plane curves which are the projections of aspace curve on three coordinate planes of the coordinate system(x,iy.K)inwhich K is confined to be real.The projection on(x,iy)plane is just the rootlocus of the polynomial with K as a real parameter.It is remarkable thatthe equation of the root-locus is m-th degree in y~2,whether n=2m 1 orn=2m 2.In addition to the real curve K.=f(x)in the figure(K,x)thereexists another curve K.which is plotted by the real parts of all complexroots against K.The(K,x)curve is particularly important to determine theabsolute as well as the relative stable interval of K for linear systems.For cybernetics,the(K,iy)curve can be used to show the relation betweenthe nature frequency ω and the gain K.Such three figures are useful forstudying the theory of equation and cybernetics.     

CONCENTRATION OF COUPLED CUBIC NONLINEAR SCHRDINGER EQUATIONS

IntroductionThe following coupled cubic nonlinear Schr dinger equations inR2are considered:it-Δ=(||2-|ψ|2),t>0,x∈R2,iψt-Δψ=(-||2 |ψ|2)ψ,t>0,x∈R2,(1)where=(t,x):[0,T)×R2→C,ψ=ψ(t,x):[0,T)×R2→C,Δis the Laplaceoperator onR2.The e     

THE LINEARIZATION OF CERTAIN CLASS OF NONLINEAR SIMULTANEOUS EQUATION SET CONTAINING AMPLITUDE AND PHASE FREQUENCY CHARACTERISTICS AND APPLICATION

A class of complex function of rational fraction type G(jω)=[1 a_1jω a_2(jω)~2 … a_m(jω)~n]/[b_0 b_1jω b_2(jω)~2 … b_n(jω)~n ] is frequently used to describe the dyna-mical properties of systems.It is however quite difficult to es-tablish a mathematical model of this type on the basis of ampli-tude and phase frequency data collected from experiments conductedon the related physical system.Since the erection of mathematicalmodel G(jω)would involve the solution of a set of nonlinear si-multaneous equations|G(jω_i)|=g_i∠G (jω_i)=θ_i i=1, 2,…,r. with the unknown coefficients a_isand b_is(i=0,1,…,m,…,n)in G(jω).Up to now,these nonlinear equa-tions have been considered to be very difficult to solve directly.In spite of the fact there are special computer programmes in cer-tain software packages available to tackle this problem,it is byno means an easy task due to the complex procedures involved inpicking up a set of initial values that should be close enough tothe exact solutions.This paper     

Existence of solutions for parabolic type evolution differential inclusions and the property of the solution set

IntroductionInrecenttenyears,becauseoftheneedofthecontroltheoryandeconomics,thetheoryofdifferentialinclusionshasbeendevelopingfast,andsome~tresultSindifferenhalinclusionshavebeenobtained.Asystematicstudyondifferenhalinclusionscanbefoundin[l].Inordertosuitcontroltheory,thefollowingsendlineardifferentialinclusionswereconsideredin[2~4]:x'(t) Ax(t)6F(t,x(t)),a.e.teI,x(0)=xo'(l)xthereAgeneratesalinearsendgroup(compactorequicolltinuouS),XisasepotleBanachspaCe,I=[0,TiisanintervalofR,F:IxX~Zx\0i…