Abstract
The present study deals with the basins of the equilibrium points embedded within the normal forms of Bogdanov–Takens bifurcation with delayed feedback control. It is numerically shown that the unstable periodic orbit that coexists with the equilibrium point stabilized by delayed feedback control is associated with the basin of the stabilized point. The relation between the periodic orbit and the basin indicates that for enlarging the basin, a homoclinic bifurcation for the orbit and a saddle point can provide useful information for the design of delayed feedback controllers. These results are experimentally confirmed in a real direct-current bus circuit that has dynamics similar to that of the normal form .
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The data in this work are available from the authors on reasonable request.
Notes
See Subsect. 2.2 for more details.
The states \( {\varvec{x}}_0 \) are set in \( 50 \times 50 \) grids with \( x_1(0) \in [x_{1l}^* - 3, x_{1l}^* + 3] \) and \( x_2(0) \in [x_{2l}^* - 3, x_{2l}^* + 3] \). A light-blue (red) dot is plotted if the trajectory starting from the dot converges (does not converge) to \( [x_{1l}^*, x_{2l}^*]^\text {T}\). The criterion for the convergence is given by the inequality \( \left| [x_1(1000)-x_{1l}^*, x_2(1000)-x_{2l}^*]^\text {T}\right| < 0.01 \).
r is numerically obtained as \((\text {number of light-blue dots})/2500\).
The stability region shown in Fig. 1 has three stable sets. The present paper deals with the largest set.
The numerical procedure used for calculating the index is the same as that for Fig. 6. The states \( {\varvec{x}}_0 \) are set in \( 50 \times 50 \) grids with \( x_{1}(0) \in [0.1, 1.2] \) and \( x_{2}(0) \in [0.1, 10] \).
Note that safe operation does not include the following case: the voltage \( v_\text {P}(t) \) converges to the equilibrium point but touches the edges.
We implemented one bipolar power supply by connecting the constant-voltage (CV) output terminal and the CV load terminal of a power supply (GPP-4323G, TEXIO). The other bipolar power supply was realized by combining the CV output (PW24-1.5AQ, TEXIO) and the CV load (PLZ164W, KIKUSUI).
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Acknowledgements
This study was supported in part by JSPS KAKENHI (18H03306 and 21H03513).
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This paper is a substantially extended version of a conference paper presented at the SICE Annual Conference 2018 [1].
Appendices
Appendix A: Solutions of time-delayed dynamical systems
This appendix gives a brief explanation of the solutions of autonomous time-delayed dynamical systems. For simplicity, we consider a time-delayed system with single scalar variable \( x \in {\mathbb {R}} \) and a single constant delay \( \tau \ge 0 \),
The dynamics depends on both the current state x(t) and the previous state \(x(t-\tau )\). Therefore, a time function,
is required as an initial condition for the time development of time-delayed system (19).
Appendix B: Saddle-node bifurcation of UPOs in a DC bus circuit with DFC
This appendix explains the bifurcation scenario that includes the saddle-node bifurcation of UPOs described by the gray lines in Fig. 9. With an increase in k from 0 for a fixed delay time \( \tau \in [6.52, 10.00] \), a pair of UPOs appear at the saddle-node bifurcation curve. As an example, the bifurcation scenario with a fixed \( \tau = 8.0 \) is shown in Fig. 15. The top panel shows an enlarged view of the bifurcation curves in Fig. 9; the bottom panel shows a bifurcation diagram for \( x_1 \). The red symbols \( \text {HP}_\text {sub} \), HC, and SN denote the bifurcation points of the Hopf bifurcation of equilibrium point \( [x_{1+}^*, x_{2+}^*]^\text {T}\), the homoclinic bifurcation of a UPO, and the saddle-node bifurcation of UPOs, respectively.
We now review the bifurcation scenario in Fig. 15 with an increase in k from 0. The unstable equilibrium point \( [x_{1+}^*, x_{2+}^*]^\text {T}\) is stabilized and UPO 1 appears via a subcritical Hopf bifurcation at \( k \approx 0.07 \) (\( \text {HP}_\text {sub} \)). With a further increase in k, UPO 1 enlarges and then disappears via the homoclinic bifurcation at \( k \approx 0.18 \) (HC). At \( k \approx 0.25 \), UPO 2 and UPO 3 are created by the saddle-node bifurcation (SN). The equilibrium point \( [x_{1+}^*, x_{2+}^*]^\text {T}\) becomes unstable and UPO 2 disappears via a subcritical Hopf bifurcation at \( k \approx 0.35 \) (\( \text {HP}_\text {sub} \)).
Appendix C: Procedure for setting initial functions
This appendix describes an experimental procedure for setting three restricted initial functions. The implementation of the CPL and the delay unit can be found in our previous study [42]. Figure 16 shows a DC bus circuit with a delayed feedback controller.
Two bipolar power suppliesFootnote 8, which can output both positive and negative currents, are used for voltage E and initial voltage \( v_\text {0} \). The power supply that supplies \( v_\text {0} \) is connected to the DC bus line by a switch. This switch is paired with another switch; they open and close at the same time. The lower switch is connected to a 5-V power supply. The delay unit detects whether the switch is open or closed. The delay unit is implemented using a peripheral interface controller (PIC: PIC18F2550-I/SP, Microchip Technology). The unit was modified from a previous one [42] to read the switch’s open/close status and to handle a voltage range of \( v_\text {P} \in [6.0, 20.0]\ \text {V}\). The output voltage \( v_\text {out}(t) \) of the delay unit can be adjusted in accordance with programs implemented in PIC.
The experimental procedure used for setting the initial functions is as follows. First, set \( v_\text {0} \) to a voltage in voltage set (18) and close the switches. Second, after a sufficient amount of time, open the switches at \( t = 0 \). Third, set the output voltage \( v_\text {out}(t) \) to
where \( v^*_\text {P} = {12.0}\ \text {V} \) corresponds to the equilibrium point (i.e., the operating point) of \( v_\text {P} (t) \). We can easily see that \( v_\text {out}(t) \) in Eqs. (21) and (22) realizes the initial functions \( {\varvec{\varPhi }}_1(t)\) and \( {\varvec{\varPhi }}_2(t)\), respectively. \( v_\text {out}(t) \) in Eq. (23) realizes \( {\varvec{\varPhi }}_3(t)\) in a shifted time scale. That is, the DC bus system starts with initial point \( v_\text {out}(0) = v_\text {0} \) and runs without control (i.e., \( i_\text {u} = 0 \)) from \( t = 0 \) to \( t = \varGamma \); DFC works from \( t = \varGamma \).
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Yoshida, K., Konishi, K. & Hara, N. Basins and bifurcations of a delayed feedback control system and its experimental verification for a DC bus circuit. Nonlinear Dyn 106, 2363–2376 (2021). https://doi.org/10.1007/s11071-021-06902-5
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DOI: https://doi.org/10.1007/s11071-021-06902-5