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Limit Cycles of Differential Equations

Colin Christopher Chengzhi Li

Resumen/Descripción – provisto por la editorial

No disponible.

Palabras clave – provistas por la editorial

Ordinary Differential Equations; Dynamical Systems and Ergodic Theory

Disponibilidad
Institución detectada Año de publicación Navegá Descargá Solicitá
No detectada 2007 SpringerLink

Información

Tipo de recurso:

libros

ISBN impreso

978-3-7643-8409-8

ISBN electrónico

978-3-7643-8410-4

Editor responsable

Springer Nature

País de edición

Reino Unido

Fecha de publicación

Información sobre derechos de publicación

© Birkhäuser Verlag 2007

Cobertura temática

Tabla de contenidos

Hilbert’s 16th Problem and Its Weak Form

Colin Christopher; Chengzhi Li

Consider the planar differential systems where and are real polynomials in and the maximum degree of and is . The second half of the famous Hilbert’s 16th problem, proposed in 1900, can be stated as follows (see [70]):

Part II - Abelian Integrals and Applications to the Weak Hilbert’s 16th Problem | Pp. 95-109

Abelian Integrals and Limit Cycles

Colin Christopher; Chengzhi Li

In this chapter we will explain the relation between the number of zeros of the Abelian integrals and the number of limit cycles of the corresponding planar polynomial differential systems.

Part II - Abelian Integrals and Applications to the Weak Hilbert’s 16th Problem | Pp. 111-126

Estimate of the Number of Zeros of Abelian Integrals

Colin Christopher; Chengzhi Li

To study the weak Hilbert’s 16th problem by using Abelian integrals, it is crucial to estimate the number of zeros of the Abelian integral. In this chapter, we introduce several methods to study the number of zeros of the Abelian integral () given in (1.10), which is related to the codimension 2 Bogdanov-Takens bifurcation problem, as we explained in subsection 1.2.2.

Part II - Abelian Integrals and Applications to the Weak Hilbert’s 16th Problem | Pp. 127-142

A Unified Proof of the Weak Hilbert’s 16th Problem for n=2

Colin Christopher; Chengzhi Li

As we explained in Subsection 1.2.1, any cubic generic Hamiltonian, with at least one period annulus contained in its level curves, can be transformed into the normal form where are parameters lying in the open region Figure 1 (in Subsection 1.2.1) shows all five possible phase portraits of in the generic cases. Here is the Hamiltonian vector field corresponding to , i.e., The vector field has a center at the origin in the ()-plane, and the continuous family of ovals, surrounding the center, is The oval shrinks to the center as → 0, and the oval terminates at the saddle loop of the saddle point (1, 0) when → 1/6.

Part II - Abelian Integrals and Applications to the Weak Hilbert’s 16th Problem | Pp. 143-158