Abstract:This paper is concerned with the global dynamics of a continuous planar piecewise linear differential system with three zones, where the dynamic of the one of the exterior linear zones is saddle and the remaining one is anti-saddle. We give all global phase portraits in the Poincaré disc and the complete bifurcation diagram including scabbard bifurcation curves, homoclinic bifurcation curves and double limit cycle bifurcation curve. Its application in a second-order memristor oscillator is shown. Finally, some… Show more
“…So all discussions for system (1.1) were restricted in the region G 1 . When d c ≤ 0, global phase portraits in the Poincaré disc and bifurcation diagrams of system (1.1) in the region G 1 were presented [21]. Therefore, in this study we continue to explore global dynamics of system (1.1) in the region G 1 when d c > 0.…”
Section: Introductionmentioning
confidence: 94%
“…Hence, the vector field (F (x) − y, g(x)) of system (5.29) is rotated about t c [22,Definition 1.6] or [38,Definition 3.3]. From [21,Lemma 5.3], it follows that the manifolds W + N and W − N of the saddle point N l of system (5.29) rotate clockwise when t c increases and t l , d c , d l , α are fixed, where W + N is the stable manifold of the right-hand side of N l and W − N is the unstable manifold of the right-hand side of N l . This indicates that system (5.29) exhibits at most one homoclinic loop.…”
Section: Ejde-2023/83mentioning
confidence: 99%
“…However, the unstable homoclinic loop breaks when t c = φ(α) ± ε, even ε > 0 is sufficiently small. According to [21,Lemma 5.3], the manifolds W + E l and W − E l rotate clockwise when t c increases and t r , t l , d r , d c , d l , α are fixed. When t c = φ(α) − ε and t c = φ(α) + ε, the relative locations of the manifolds W + E l and W − E l are depicted in Figure 17(a) and (c), respectively.…”
Section: Ejde-2023/83mentioning
confidence: 99%
“…Considerable attention has been devoted to characterizing global dynamics of system (1.1) [6,7,9,10,17,20,24,25,26,27,29]. Jia-Su-Chen [21] once investigated global dynamics of system (1.1) in the region:…”
This article concerns the global dynamics of a continuous planar piecewise linear differential system with three zones. We give global phase portraits in the Poincare disc and classify bifurcation diagrams under certain parametric conditions, when the dynamics of central linear zone is anti-saddle. Rich dynamical behaviors are demonstrated, from which we observe homoclinic loops appearing in three linear zones and limit cycles occurring in three linear zones which surround a node or node-focus.
For more information see https://ejde.math.txstate.edu/Volumes/2023/83/abstr.html
“…So all discussions for system (1.1) were restricted in the region G 1 . When d c ≤ 0, global phase portraits in the Poincaré disc and bifurcation diagrams of system (1.1) in the region G 1 were presented [21]. Therefore, in this study we continue to explore global dynamics of system (1.1) in the region G 1 when d c > 0.…”
Section: Introductionmentioning
confidence: 94%
“…Hence, the vector field (F (x) − y, g(x)) of system (5.29) is rotated about t c [22,Definition 1.6] or [38,Definition 3.3]. From [21,Lemma 5.3], it follows that the manifolds W + N and W − N of the saddle point N l of system (5.29) rotate clockwise when t c increases and t l , d c , d l , α are fixed, where W + N is the stable manifold of the right-hand side of N l and W − N is the unstable manifold of the right-hand side of N l . This indicates that system (5.29) exhibits at most one homoclinic loop.…”
Section: Ejde-2023/83mentioning
confidence: 99%
“…However, the unstable homoclinic loop breaks when t c = φ(α) ± ε, even ε > 0 is sufficiently small. According to [21,Lemma 5.3], the manifolds W + E l and W − E l rotate clockwise when t c increases and t r , t l , d r , d c , d l , α are fixed. When t c = φ(α) − ε and t c = φ(α) + ε, the relative locations of the manifolds W + E l and W − E l are depicted in Figure 17(a) and (c), respectively.…”
Section: Ejde-2023/83mentioning
confidence: 99%
“…Considerable attention has been devoted to characterizing global dynamics of system (1.1) [6,7,9,10,17,20,24,25,26,27,29]. Jia-Su-Chen [21] once investigated global dynamics of system (1.1) in the region:…”
This article concerns the global dynamics of a continuous planar piecewise linear differential system with three zones. We give global phase portraits in the Poincare disc and classify bifurcation diagrams under certain parametric conditions, when the dynamics of central linear zone is anti-saddle. Rich dynamical behaviors are demonstrated, from which we observe homoclinic loops appearing in three linear zones and limit cycles occurring in three linear zones which surround a node or node-focus.
For more information see https://ejde.math.txstate.edu/Volumes/2023/83/abstr.html
“…[9,12,21,25,28,34,41,45,46], H.C. [14,23,24] and I.C. [22,25,26,44] and the other control [1,3,10,18,40,42]. Nevertheless, in this manuscript, we design a SIR epidemic system to address the D.T.C.…”
This paper investigates the global dynamic behavior and bifurcations of a classical nonlinear transmission SIR epidemic model with discontinuous threshold strategy. Different from previous results, we not only consider the general nonlinear transmission, but also adopt the discontinuity control. First, the positivity and boundedness of the model are given. Second, by employing Lyapunov LaSalle approach and using Green Theorem, we perform the globally stable the three types of equilibria of the system. We analytically show the orbit can tend to the disease-free equilibrium point, the endemic equilibrium point or the sliding equilibrium point in discontinuous surfaces of the system. In addition, we also analyze the sliding bifurcations of the model when consider the special transmission. Finally, some numerical simulations are worked out to confirm the results obtained in this paper.
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