关于一个平面二次系统极限环的唯一性

<正> 我们这里研究平面二次系统容易知道方程（1）当δ=0时不存在闭轨与奇闭轨线，事实上只要引进变数变换d而且1+by=0是无切直线,因此当δ=0时(1)无闭轨与奇闭轨.因为(1)对于参数δ构成旋转向量场,因而我们知道(1)当δa(b+2l)≤0时在原点附近不存在极限环,而当δa(b+2l)>0且|δ|《1时在原点附近存在极限环,本文证明了(1)的极限环是唯一的.     

一类三次系统的广义相伴系统的定性分析

研究了一类三次多项式微分系统=-y+δx+lx~2+mxy+bxy~2+ax~3,=x的广义相伴系统=-y+δx+lx~2+mxy+bxy~2+ax~3,=x(y),对原点O进行了中心-焦点判定.利用旋转向量场的理论得出了系统不存在极限环的充分条件,利用Hopf分支问题的Lyapunov第二方法得到了该系统极限环存在性的若干充分条件,最后利用Coppel的唯一性定理得到了极限环唯一性的充分条件.     

二次系统的椭圆分界线环

多项式系统存在极限环的准确的参数区间的研究是一个较困难的课题。主要的困难是,在旋转向量场中,当极限环随参数的单调变化而扩大,最后变成分界线环而消失时,所对应的这个准确参数值,只有在所对应的分界线环是代数曲线,且找到这个代数曲线的方程后才能得到。除此之外,找不到一个更为有效的方法。这样就大大地限制了对极限环     

判别二次系统有界分界线环的例子

设二次系统x=-y+δx+lx~2+mxy+ny~2,y=x(1+ax+by),在O(0,0)外围存在一个极限环,它随δ按适当方向单调变化而扩大.如果它最后变成了有限分界线环,那末如何判别此分界线环的类型.对于一般的二次系统,这是一个极困难的问题.但     

极限环和拟旋转向量场

本文定义了平面上的拟旋转向量场,研究在拟旋转向量场中极限环随参数的变化情况,证明它具有和旋转向量场完全族类似的性质.     

Ⅲa＝0（－1＜n＜0，0＜l＜1）类二次系统存在极限环的充要条件

本文利用旋转向量场理论得到了系统ｘ＝－ｙ＋δｘ＋ｌｘ２＋ｍｘｙ＋ｎｙ２，ｙ＝ｘ（１＋ｙ），｛（－１＜ｎ＜０，０＜ｌ＜１）存在极限环的充要条件．     

方程(dy)/(dx)=(sumq_(ij)x~iy~j from 0≤i+j≤2)/(sum p_(ij)x~iy~j from 0≤i+j≤2)所定义的积分曲线的定性研究(Ⅵ):Ⅰ类方程的极限环

继【2],考察最一般的I类方程注劣.,二,二,_,、d,_,—~一y十心x十lx’十xy十n犷~尸Lx,夕),一~x~夕气x,y)‘dt----一dt一在其中不”‘+·>0,方程(‘,有两个有限远奇点:“(0,。,为焦点,“(”,劲(l)为鞍点,由旋转向量场的理论[a.4]得知,当d由。变为负值时,0由不稳定焦点变为稳定,在它附近产生一个不稳定极限环,且随d减小而单调地扩大.〔l]首先证明了:当l~o时,此极限环最后遇鞍点N而消失.在这一过程,没有其它极限环产生.【2」则证明了。~0或l一41,一。时极限环的唯一性.本文将证明,当,)21>0,l,)丝时,(l)的极 l6限环最多也只有一个.与此同时,还…     

微分方程组=a+sum from ((i+j)=2) (a_(ij)x~iy~j),=b+sum from ((i+j)=2) (b_(ij)x~iy~j)的极限环存在的分歧值与代数奇异环

§1 引言 董金柱最先研究如下的二次系统[1]: (?)=α+sum from i+j=2 (α_(ij)x~iy~i,(?)=b+sum from i+j=2 (b_(ij)x~iy~i) (E) 的极限环的个数问题,他指出(E)可以至少存在两个极限环,且这两个极限环的位置分布在两个奇点周围。文[2]中证明了(E)至多存在两个极限环。本文将应用旋转向量场理论,研究当旋转参数α=时极限环变为奇异环的分歧值。从而得出一些情况下(E)恰存在两个极限环的充要条件。依据[2],研究(E)的极限环,只要研究如下系统就行了:     

旋转向量场中闭轨线的方程

<正> G.F.D.Duff于1953年首次展开了旋转向量场的理论.后来G.Seifert改进了Duff的工作.本文主要在于建立旋转向量场中闭轨线的方程,并初步用它来计算含小参数的范德坡方程的极限环,这种方法较简便,且对旋转向量场中的合小参数的不少方程同样有效.我们采用 Seifert 关于旋转向量场的定义和术语.考察方程组     

一类五次平面向量场的极限环

本文利用分支方法和微分方程定性分析理论研究了一类Z_2旋转不变的五次平面向量场的极限环的个数和分布,发现该五次多项式系统中至少存在25个极限环,同时发现所研究五次系统出现的25个极限环具有四种不同的分布．由此可推出五次多项式平面微分方程的Hilbert数日(5)≥25=5~2,所得结果有助于弱的Hilbert问题的进一步研究．     

Bifurcation and Isochronicity at Infinity in a Class of Cubic Polynomial Vector Fields

In this paper, we study the appearance of limit cycles from the equator and isochronicity of infinity in polynomial vector fields with no singular points at infinity. We give a recursive formula to compute the singular point quantities of a class of cubic polynomial systems, which is used to calculate the first seven singular point quantities. Further, we prove that such a cubic vector field can have maximal seven limit cycles in the neighborhood of infinity. We actually and construct a system that has seven limit cycles. The positions of these limit cycles can be given exactly without constructing the Poincare cycle fields. The technique employed in this work is essentially different from the previously widely used ones. Finally, the isochronous center conditions at infinity are given.     

Bifurcations of limit cycles in a Z 4-equivariant quintic planar vector field

In this paper, a Z4-equivariant quintic planar vector field is studied. The Hopf bifurcation method and polycycle bifurcation method are combined to study the limit cycles bifurcated from the compounded cycle with 4 hyperbolic saddle points. It is found that this special quintic planar polynomial system has at least four large limit cycles which surround all singular points. By applying the double homoclinic loops bifurcation method and Hopf bifurcation method, we conclude that 28 limit cycles with two different configurations exist in this special planar polynomial system. The results acquired in this paper are useful for studying the weakened 16th Hilbert＇s Problem.     

Quantities at infinity in translational polynomial vector fields

In this paper, we study quantities at infinity and the appearance of limit cycles from the equator in polynomial vector fields with no singular points at infinity. We start by proving the algebraic equivalence of the corresponding quantities at infinity (also focal values at infinity) for the system and its translational system, then we obtain that the maximum number of limit cycles that can appear at infinity is invariant for the systems by translational transformation. Finally, we compute the singular point quantities of a class of cubic polynomial system and its translational system, reach with relative ease expressions of the first five quantities at infinity of the two systems, then we prove that the two cubic vector fields perturbed identically can have five limit cycles simultaneously in the neighborhood of infinity and construct two systems that allow the appearance of five limit cycles respectively. The positions of these limit cycles can be pointed out exactly without constructing Poincaré cycle fields. The technique employed in this work is essentially different from more usual ones, The calculation can be readily done with using computer symbol operation system such as Mathematics.     

Configurations of limit cycles and planar polynomial vector fields

We show that every finite configuration of disjoint simple closed curves of the plane is topologically realizable as the set of limit cycles of a polynomial vector field. Moreover, the realization can be made by algebraic limit cycles, and we provide an explicit polynomial vector field exhibiting any given finite configuration of limit cycles.     

Homoclinic,heteroclinic and periodic orbits of singularly perturbed systems

The main aims of this paper are to study the persistence of homoclinic and heteroclinic orbits of the reduced systems on normally hyperbolic critical manifolds, and also the limit cycle bifurcations either from the homoclinic loop of the reduced systems or from a family of periodic orbits of the layer systems. For the persistence of homoclinic and heteroclinic orbits, and the limit cycles bifurcating from a homolinic loop of the reduced systems, we provide a new and readily detectable method to characterize them compared with the usual Melnikov method when the reduced system forms a generalized rotated vector field. To determine the limit cycles bifurcating from the families of periodic orbits of the layer systems, we apply the averaging methods.We also provide two four-dimensional singularly perturbed differential systems, which have either heteroclinic or homoclinic orbits located on the slow manifolds and also three limit cycles bifurcating from the periodic orbits of the layer system.     

Center conditions and bifurcation of limit cycles at degenerate singular points in a quintic polynomial differential system

The center problem and bifurcation of limit cycles for degenerate singular points are far to be solved in general. In this paper, we study center conditions and bifurcation of limit cycles at the degenerate singular point in a class of quintic polynomial vector field with a small parameter and eight normal parameters. We deduce a recursion formula for singular point quantities at the degenerate singular points in this system and reach with relative ease an expression of the first five quantities at the degenerate singular point. The center conditions for the degenerate singular point of this system are derived. Consequently, we construct a quintic system, which can bifurcates 5 limit cycles in the neighborhood of the degenerate singular point. The positions of these limit cycles can be pointed out exactly without constructing Poincaré cycle fields. The technique employed in this work is essentially different from more usual ones. The recursion formula we present in this paper for the calculation of singular point quantities at degenerate singular point is linear and then avoids complex integrating operations.     

Estimating the number of limit cycles in polynomials systems

We describe a method based on algorithms of computational algebra for obtaining an upper bound for the number of limit cycles bifurcating from a center or a focus of polynomial vector field. We apply it to a cubic system depending on six parameters and prove that in the generic case at most six limit cycles can bifurcate from any center or focus at the origin of the system.     

Wintner-Perko termination principle,parameters rotating a field,and limit-cycle problem

In this paper, limit cycles of polynomial dynamical systems are studied. For the global analysis of bifurcations of limit cycles, we use the Wintner-Perko termination principle. Monotone families of limit cycles and rotated vector fields and limit-cycle problems for quadratic systems are also discussed.Translated from Sovremennaya Matematika i Ee Prilozheniya (Contemporary Mathematics and Its Applications), Vol. 7, Suzdal Conference-1, 2003.This revised version was published online in April 2005 with a corrected cover date.     

The applied geometry of a general Liénard polynomial system

In this work, applying a canonical system with field rotation parameters and using geometric properties of the spirals filling the interior and exterior domains of limit cycles, we solve the limit cycle problem for a general Liénard polynomial system with an arbitrary (but finite) number of singular points.     

Note on a paper of J. Llibre and G. Rodríguez concerning algebraic limit cycles

In a recent paper of Llibre and Rodríguez (J. Differential Equations 198 (2004) 374-380) it is proved that every configuration of cycles in the plane is realizable (up to homeomorphism) by a polynomial vector field of degree at most 2(n+r)-1, where n is the number of cycles and r the number of primary cycles (a cycle C is primary if there are no other cycles contained in the bounded region limited by C). In this letter we prove the same theorem by using an easier construction but with a greater polynomial bound (the vector field we construct has degree at most 4n-1). By using the same technique we also construct R³ polynomial vector fields realizing (up to homeomorphism) any configuration of limit cycles which can be linked and knotted in R³. This answers a question of R. Sverdlove.