Limit Cycles of Planar Piecewise Differential Systems with Linear Hamiltonian Saddles

We provide the maximum number of limit cycles for continuous and discontinuous planar piecewise differential systems formed by linear Hamiltonian saddles and separated either by one or two parallel straight lines. We show that when these piecewise differential systems are either continuous or discon...

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Main Authors: Jaume Llibre, Claudia Valls
Format: Article
Language:English
Published: MDPI AG 2021-06-01
Series:Symmetry
Subjects:
Online Access:https://www.mdpi.com/2073-8994/13/7/1128
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spelling doaj-08ef24d7030448efa89d054f8d97dcbf2021-07-23T14:08:58ZengMDPI AGSymmetry2073-89942021-06-01131128112810.3390/sym13071128Limit Cycles of Planar Piecewise Differential Systems with Linear Hamiltonian SaddlesJaume Llibre0Claudia Valls1Departament de Matemàtiques, Universitat Autònoma de Barcelona, 08193 Barcelona, SpainDepartamento de Matemática, Instituto Superior Técnico, Universidade de Lisboa, Av. Rovisco Pais, 1049-001 Lisboa, PortugalWe provide the maximum number of limit cycles for continuous and discontinuous planar piecewise differential systems formed by linear Hamiltonian saddles and separated either by one or two parallel straight lines. We show that when these piecewise differential systems are either continuous or discontinuous and are separated by one straight line, or are continuous and are separated by two parallel straight lines, they do not have limit cycles. On the other hand, when these systems are discontinuous and separated by two parallel straight lines, we prove that the maximum number of limit cycles that they can have is one and that this maximum is reached by providing an example of such a system with one limit cycle. When the line of discontinuity of the piecewise differential system is formed by one straight line, the symmetry of the problem allows to take this straight line without loss of generality as the line <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>x</mi><mo>=</mo><mn>0</mn></mrow></semantics></math></inline-formula>. Similarly, when the line of discontinuity of the piecewise differential system is formed by two parallel straight lines due to the symmetry of the problem, we can assume without loss of generality that these two straight lines are <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>x</mi><mo>=</mo><mo>±</mo><mn>1</mn></mrow></semantics></math></inline-formula>.https://www.mdpi.com/2073-8994/13/7/1128crossing limit cycleslinear Hamiltonian saddlescontinuous piecewise linear differential systemsdiscontinuous piecewise differential systems
collection DOAJ
language English
format Article
sources DOAJ
author Jaume Llibre
Claudia Valls
spellingShingle Jaume Llibre
Claudia Valls
Limit Cycles of Planar Piecewise Differential Systems with Linear Hamiltonian Saddles
Symmetry
crossing limit cycles
linear Hamiltonian saddles
continuous piecewise linear differential systems
discontinuous piecewise differential systems
author_facet Jaume Llibre
Claudia Valls
author_sort Jaume Llibre
title Limit Cycles of Planar Piecewise Differential Systems with Linear Hamiltonian Saddles
title_short Limit Cycles of Planar Piecewise Differential Systems with Linear Hamiltonian Saddles
title_full Limit Cycles of Planar Piecewise Differential Systems with Linear Hamiltonian Saddles
title_fullStr Limit Cycles of Planar Piecewise Differential Systems with Linear Hamiltonian Saddles
title_full_unstemmed Limit Cycles of Planar Piecewise Differential Systems with Linear Hamiltonian Saddles
title_sort limit cycles of planar piecewise differential systems with linear hamiltonian saddles
publisher MDPI AG
series Symmetry
issn 2073-8994
publishDate 2021-06-01
description We provide the maximum number of limit cycles for continuous and discontinuous planar piecewise differential systems formed by linear Hamiltonian saddles and separated either by one or two parallel straight lines. We show that when these piecewise differential systems are either continuous or discontinuous and are separated by one straight line, or are continuous and are separated by two parallel straight lines, they do not have limit cycles. On the other hand, when these systems are discontinuous and separated by two parallel straight lines, we prove that the maximum number of limit cycles that they can have is one and that this maximum is reached by providing an example of such a system with one limit cycle. When the line of discontinuity of the piecewise differential system is formed by one straight line, the symmetry of the problem allows to take this straight line without loss of generality as the line <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>x</mi><mo>=</mo><mn>0</mn></mrow></semantics></math></inline-formula>. Similarly, when the line of discontinuity of the piecewise differential system is formed by two parallel straight lines due to the symmetry of the problem, we can assume without loss of generality that these two straight lines are <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>x</mi><mo>=</mo><mo>±</mo><mn>1</mn></mrow></semantics></math></inline-formula>.
topic crossing limit cycles
linear Hamiltonian saddles
continuous piecewise linear differential systems
discontinuous piecewise differential systems
url https://www.mdpi.com/2073-8994/13/7/1128
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