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Time-delay feedback control of nonlinear oscillators Viktor Urumov,  PMF, Skopje 30 juni 2010, Niš
Plan ,[object Object],[object Object],[object Object],[object Object],[object Object]
PMF, Skopje
Prose~na golemina na  evropski oddel za fizika (2009) ,[object Object],[object Object],[object Object],[object Object],[object Object]
Current programme – part 1 (semesters 1-4) ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Current programme - part 2 (semesters 5-8,  physics teachers branch )   ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Nonlinear oscillator
The Lorenz system Chaotic attractor of the unperturbed system ( F(t)=0 ) E. N. Lorenz, “ Deterministic nonperiodic flow ,” J. Atmos. Sci.  20  (1963) 130. Fixed points:   C 0  (0,0,0) C ±  (±8.485, ±8.485,27) Eigenvalues:  (C 0 ) = {-22.83, 11.83, -2.67}  (C±) = {-13.85, 0.09+10.19i, 0.09-10.19i}
van der Pol oscillator
Limit cycle
Rössler oscillator with harmonic forcing
Historical example from Biology The glowworms ... Represent another shew, which settle on some Trees, like a fiery cloud, with this surprising circumstance, that a whole swarm of these insects, having taken possession of one Tree, and spread themselves over its branches, sometimes hide their Light all at once, and a moment after make it appear again with the utmost regularity and exactness … Engelbert Kaempfer description from his trip in Siam (1680)
 
 
Further examples  ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Further examples 2  ,[object Object],[object Object],[object Object],[object Object],[object Object]
Modelot na Kuramoto                                                  
Parametar na poredok i  sinhronizacija
Re{enie na modelot na Kuramoto (1975) re{enija i
 
 
INTRODUCTION -  THE PYRAGAS CONTROL METHOD - Time-delayed feedback control (TDFC) - Time-delayed autosynchronization (TDAS) K. Pyragas, Phys. Lett. A  170  (1992) 421
Applications ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Pyragas control force: VARIABLE DELAY FEEDBACK CONTROL OF USS VDFC force: - saw tooth wave:  - sine wave:  - random wave:  -  noninvasive for USS and periodic orbits   -  piezoelements, noise   A. Gjurchinovski and V. Urumov – Europhys. Lett.  84 , 40013 (2008)
VARIABLE DELAY FEEDBACK CONTROL OF USS
THE MECHANISM OF VDFC
DELAY MODULATIONS
THE MECHANISM OF VDFC
THE MECHANISM OF VDFC 2D UNSTABLE FOCUS WITH A DIAGONAL COUPLING original system : comparison system :   –  sufficiently  large Characteristic equation of the comparison system (2D focus):
THE MECHANISM OF VDFC TDAS VDFC VDFC VDFC
THE MECHANISM OF VDFC The effect of including variable delay into TDAS for small   ,[object Object],[object Object],CONCLUSION:  the stability domain will expand in all directions within the half-space  K > K 0 , as soon as    is increased from zero, independent of  the precise way in which the delay is varied
THE MECHANISM OF VDFC 2D unstable focus with  and    Pyragas  Increase of the stability  domain for small    (brown)  (green)  (yellow)
THE MECHANISM OF VDFC     diagrams for a saw tooth wave modulation ( T 0 =1)
THE MECHANISM OF VDFC
THE MECHANISM OF VDFC Stability analysis for the Lorenz system (saw tooth wave) C +  (8.485, 8.485,27) C 0  (0,0,0) C -  (-8.485, -8.485,27)  10, r   28, b   8/3
THE MECHANISM OF VDFC
THE MECHANISM OF VDFC The Rössler system  (sawtooth wave) O.E. Rössler, Phys. Lett. A  57 , 397 (1976). Fixed points:   C 1  (0.007,-0.035,0.035) C 2  (5.693, -28.465,28.465) Eigenvalues:  (C 1 ) = {-5.687,0.097+0.995i,0.097-0.995i}  (C 2 ) = {0.192,-0.00000459+5.428i, -0.00000459-5.428i}  0  0.5  1  2
STABILIZATION OF UPO BY VDFC ,[object Object],[object Object],[object Object],[object Object],[object Object],+ T(t) T 0 2T 0 t     T(t) T 0 2T 0 t     K(t) K/2 K t    
STABILIZATION OF UPO BY VDFC ,[object Object],Rössler   T 0 =5.88 ,[object Object],[object Object],[object Object],F(t)=K [y(t-T 0 )-y(t)] F(t)=K [y(t-T(t))-y(t)] F(t)=K(t) [y(t-T 0 )-y(t)] F(t)=K(t) [y(t-T(t))-y(t)]
STABILIZATION OF UPO BY VDFC Rössler   T 0 =11.75 Rössler   T 0 =17.5
STABILIZATION OF UPO BY VDFC ,[object Object],K periodically varied between K and K/4 (Rössler,  T 0 =17.5 ) ,[object Object],F(t)=K(t) Sin [y(t-T(t))-y(t)]
STABILIZATION OF UPO BY VDFC Rössler  T 0 =5.88 VDFC (square wave)    = T 0    = 2T 0    = T 0 /2
STABILITY ANALYSIS - RDDE Retarded delay-differential equations ,[object Object],[object Object],[object Object],T. Erneux,  Applied Delay Differential Equations  (Springer, New York, 2009)
Retarded delay-differential equations General scalar RDDE system: T 1   ≥ 0   – constant delay time F   – arbitrary nonlinear function of the state variable  x Linearized system around the fixed point  x * : DELAY-DIFFERENTIAL EQUATIONS Characteristic equation for the stability of steady state  x *  of the free-running system: A. Gjurchinovski and V. Urumov – Phys. Rev. E  81 , 016209 (2010)
STABILITY ANALYSIS - RDDE Retarded delay-differential equations Controlled RDDE system: u(t)  – Pyragas-type feedback force with a variable time delay   K   – feedback gain (strength of the feedback) T 2   – nominal delay value f   –  periodic function with zero mean  –   amplitude of the modulation  –   frequency of the modulation
STABILITY ANALYSIS - RDDE Stability of the unperturbed system
STABILITY ANALYSIS - RDDE Stability under variable-delay feedback control Limitation of the VDFC for RDDE systems: ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
STABILITY ANALYSIS - RDDE Representation of the control boundaries parametrized by    = Im(  ) ( K , T 2 )  plane:
EXAMPLES AND SIMULATIONS Mackey-Glass system ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
EXAMPLES AND SIMULATIONS Mackey-Glass system (without control) ,[object Object],[object Object],[object Object],[object Object]
EXAMPLES AND SIMULATIONS Mackey-Glass system (VDFC) ,[object Object],[object Object],[object Object],[object Object],T 1  = 23
EXAMPLES AND SIMULATIONS Mackey-Glass system (VDFC) ,[object Object],[object Object],[object Object],[object Object],T 1  = 23
EXAMPLES AND SIMULATIONS Mackey-Glass system (VDFC) ,[object Object],[object Object],[object Object],[object Object],K  = 0.5
EXAMPLES AND SIMULATIONS Mackey-Glass system (VDFC) T 1  = 23,  T 2  = 18,  K  = 2,    = 2,    = 5  saw  sin  sqr
EXAMPLES AND SIMULATIONS Mackey-Glass system (VDFC)
EXAMPLES AND SIMULATIONS Mackey-Glass system (VDFC)
EXAMPLES AND SIMULATIONS Ikeda system ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
EXAMPLES AND SIMULATIONS Sprott system ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
FRACTIONAL DIFFERENTIAL EQUATIONS Fractional R ö ssler system Caputo fractional-order derivative:
FRACTIONAL DIFFERENTIAL EQUATIONS Fractional R ö ssler system
FRACTIONAL DIFFERENTIAL EQUATIONS Fractional R ö ssler system -  stability diagrams Time-delayed feedback control Variable delay feedback control (sine-wave,   =1,   =10) Time-delayed feedback control Variable delay feedback control (sine-wave,   =1,   =10) Time-delayed feedback control Variable delay feedback control (sine-wave,   =1,   =10) Time-delayed feedback control
Desynchronisation in systems of coupled oscillators Hindmarsh - Rose oscillators Mean field Global coupling Delayed feedback control M. Rosenblum and A. Pikovsky, Phys. Rev. Lett.  92 , 114102; Phys. Rev. E  70 , 041904 (2004)
Desynchronisation in systems of coupled oscillators Feedback switched on at  t=5000 System of  1000  H-R oscillators  = const =72.5 K=0.0036 K mf =0.08
Desynchronisation in systems of coupled oscillators Time-delayed feedback control Variable delay feedback control (sine-wave,   =40,   =10) Suppression coefficient X – Mean field in the  absence  of feedback X f  – Mean field in the  presence  of feedback T=145  – average period of the mean field in the  absence  of feedback
CONCLUSIONS AND FUTURE PROSPECTS ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
SCI  publikacii od balkanski gradovi  2006-2010   IT, GR, DE, FR, US 7 7 22 147 162 348 Tirana DE, US, FR, IT 72 241 953 760 6826 8964 Sofija DE, BG, US, SRB, IT 15 22 58 520 628 1257 Skopje DE, CRO, US, SRB, SLO 3 9 48 192 565 824 Saraevo SRB, DE, IT, FR, RU 5 13 54 287 363 Podgorica GR, US, UK, DE 25 71 175 162 1354 1858 Nikozija US, DE, IT, UK, FR 87 358 1129 733 7957 10482 Qubqana US, DE, RU, PL 6 23 120 123 768 1044 Ki{inev US, DE, UK, IT, FR 703 443 1031 2772 15135 20627 Istanbul US, DE, IT, FR, SLO 194 373 936 1252 6590 9576 Zagreb FR, DE, US, IT, UK 32 205 1523 1312 8184 11413 Bukure{t DE, US, IT, UK, FR 112 242 860 1669 7287 10348 Belgrad US, UK, DE, FR, IT 1032 1592 1751 4996 16700 26880 Atina glavna sorabotka pisma revijalni zbornici apstrakti statii vkupno
SCI  publikacii od Skopje 1993-2009 (Sv. Kiril i Metodij)

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Viktor Urumov - Time-delay feedback control of nonlinear oscillators

  • 1. Time-delay feedback control of nonlinear oscillators Viktor Urumov,  PMF, Skopje 30 juni 2010, Niš
  • 2.
  • 4.
  • 5.
  • 6.
  • 8. The Lorenz system Chaotic attractor of the unperturbed system ( F(t)=0 ) E. N. Lorenz, “ Deterministic nonperiodic flow ,” J. Atmos. Sci. 20 (1963) 130. Fixed points: C 0 (0,0,0) C ± (±8.485, ±8.485,27) Eigenvalues:  (C 0 ) = {-22.83, 11.83, -2.67}  (C±) = {-13.85, 0.09+10.19i, 0.09-10.19i}
  • 9. van der Pol oscillator
  • 11. Rössler oscillator with harmonic forcing
  • 12. Historical example from Biology The glowworms ... Represent another shew, which settle on some Trees, like a fiery cloud, with this surprising circumstance, that a whole swarm of these insects, having taken possession of one Tree, and spread themselves over its branches, sometimes hide their Light all at once, and a moment after make it appear again with the utmost regularity and exactness … Engelbert Kaempfer description from his trip in Siam (1680)
  • 13.  
  • 14.  
  • 15.
  • 16.
  • 17. Modelot na Kuramoto                                                  
  • 18. Parametar na poredok i sinhronizacija
  • 19. Re{enie na modelot na Kuramoto (1975) re{enija i
  • 20.  
  • 21.  
  • 22. INTRODUCTION - THE PYRAGAS CONTROL METHOD - Time-delayed feedback control (TDFC) - Time-delayed autosynchronization (TDAS) K. Pyragas, Phys. Lett. A 170 (1992) 421
  • 23.
  • 24. Pyragas control force: VARIABLE DELAY FEEDBACK CONTROL OF USS VDFC force: - saw tooth wave: - sine wave: - random wave: - noninvasive for USS and periodic orbits - piezoelements, noise A. Gjurchinovski and V. Urumov – Europhys. Lett. 84 , 40013 (2008)
  • 25. VARIABLE DELAY FEEDBACK CONTROL OF USS
  • 29. THE MECHANISM OF VDFC 2D UNSTABLE FOCUS WITH A DIAGONAL COUPLING original system : comparison system :  – sufficiently large Characteristic equation of the comparison system (2D focus):
  • 30. THE MECHANISM OF VDFC TDAS VDFC VDFC VDFC
  • 31.
  • 32. THE MECHANISM OF VDFC 2D unstable focus with  and    Pyragas  Increase of the stability domain for small   (brown)  (green)  (yellow)
  • 33. THE MECHANISM OF VDFC     diagrams for a saw tooth wave modulation ( T 0 =1)
  • 35. THE MECHANISM OF VDFC Stability analysis for the Lorenz system (saw tooth wave) C + (8.485, 8.485,27) C 0 (0,0,0) C - (-8.485, -8.485,27)  10, r  28, b  8/3
  • 37. THE MECHANISM OF VDFC The Rössler system (sawtooth wave) O.E. Rössler, Phys. Lett. A 57 , 397 (1976). Fixed points: C 1 (0.007,-0.035,0.035) C 2 (5.693, -28.465,28.465) Eigenvalues:  (C 1 ) = {-5.687,0.097+0.995i,0.097-0.995i}  (C 2 ) = {0.192,-0.00000459+5.428i, -0.00000459-5.428i}  0  0.5  1  2
  • 38.
  • 39.
  • 40. STABILIZATION OF UPO BY VDFC Rössler T 0 =11.75 Rössler T 0 =17.5
  • 41.
  • 42. STABILIZATION OF UPO BY VDFC Rössler T 0 =5.88 VDFC (square wave)  = T 0  = 2T 0  = T 0 /2
  • 43.
  • 44. Retarded delay-differential equations General scalar RDDE system: T 1 ≥ 0 – constant delay time F – arbitrary nonlinear function of the state variable x Linearized system around the fixed point x * : DELAY-DIFFERENTIAL EQUATIONS Characteristic equation for the stability of steady state x * of the free-running system: A. Gjurchinovski and V. Urumov – Phys. Rev. E 81 , 016209 (2010)
  • 45. STABILITY ANALYSIS - RDDE Retarded delay-differential equations Controlled RDDE system: u(t) – Pyragas-type feedback force with a variable time delay K – feedback gain (strength of the feedback) T 2 – nominal delay value f – periodic function with zero mean  – amplitude of the modulation  – frequency of the modulation
  • 46. STABILITY ANALYSIS - RDDE Stability of the unperturbed system
  • 47.
  • 48. STABILITY ANALYSIS - RDDE Representation of the control boundaries parametrized by  = Im(  ) ( K , T 2 ) plane:
  • 49.
  • 50.
  • 51.
  • 52.
  • 53.
  • 54. EXAMPLES AND SIMULATIONS Mackey-Glass system (VDFC) T 1 = 23, T 2 = 18, K = 2,  = 2,  = 5 saw sin sqr
  • 55. EXAMPLES AND SIMULATIONS Mackey-Glass system (VDFC)
  • 56. EXAMPLES AND SIMULATIONS Mackey-Glass system (VDFC)
  • 57.
  • 58.
  • 59. FRACTIONAL DIFFERENTIAL EQUATIONS Fractional R ö ssler system Caputo fractional-order derivative:
  • 60. FRACTIONAL DIFFERENTIAL EQUATIONS Fractional R ö ssler system
  • 61. FRACTIONAL DIFFERENTIAL EQUATIONS Fractional R ö ssler system - stability diagrams Time-delayed feedback control Variable delay feedback control (sine-wave,  =1,  =10) Time-delayed feedback control Variable delay feedback control (sine-wave,  =1,  =10) Time-delayed feedback control Variable delay feedback control (sine-wave,  =1,  =10) Time-delayed feedback control
  • 62. Desynchronisation in systems of coupled oscillators Hindmarsh - Rose oscillators Mean field Global coupling Delayed feedback control M. Rosenblum and A. Pikovsky, Phys. Rev. Lett. 92 , 114102; Phys. Rev. E 70 , 041904 (2004)
  • 63. Desynchronisation in systems of coupled oscillators Feedback switched on at t=5000 System of 1000 H-R oscillators  = const =72.5 K=0.0036 K mf =0.08
  • 64. Desynchronisation in systems of coupled oscillators Time-delayed feedback control Variable delay feedback control (sine-wave,  =40,  =10) Suppression coefficient X – Mean field in the absence of feedback X f – Mean field in the presence of feedback T=145 – average period of the mean field in the absence of feedback
  • 65.
  • 66. SCI publikacii od balkanski gradovi 2006-2010 IT, GR, DE, FR, US 7 7 22 147 162 348 Tirana DE, US, FR, IT 72 241 953 760 6826 8964 Sofija DE, BG, US, SRB, IT 15 22 58 520 628 1257 Skopje DE, CRO, US, SRB, SLO 3 9 48 192 565 824 Saraevo SRB, DE, IT, FR, RU 5 13 54 287 363 Podgorica GR, US, UK, DE 25 71 175 162 1354 1858 Nikozija US, DE, IT, UK, FR 87 358 1129 733 7957 10482 Qubqana US, DE, RU, PL 6 23 120 123 768 1044 Ki{inev US, DE, UK, IT, FR 703 443 1031 2772 15135 20627 Istanbul US, DE, IT, FR, SLO 194 373 936 1252 6590 9576 Zagreb FR, DE, US, IT, UK 32 205 1523 1312 8184 11413 Bukure{t DE, US, IT, UK, FR 112 242 860 1669 7287 10348 Belgrad US, UK, DE, FR, IT 1032 1592 1751 4996 16700 26880 Atina glavna sorabotka pisma revijalni zbornici apstrakti statii vkupno
  • 67. SCI publikacii od Skopje 1993-2009 (Sv. Kiril i Metodij)