Catálogo de publicaciones - libros
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
2007
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