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Period-doubling bifurcation

In dynamical systems theory, a period-doubling bifurcation occurs when a slight change in a system's parameters causes a new periodic trajectory to emerge from an existing periodic trajectory—the new one having double the period of the original. With the doubled period, it takes twice as long (or, in a discrete dynamical system, twice as many iterations) for the numerical values visited by the system to repeat themselves.

A period-halving bifurcation occurs when a system switches to a new behavior with half the period of the original system.

A period-doubling cascade is an infinite sequence of period-doubling bifurcations. Such cascades are a common route by which dynamical systems develop chaos.[1] In hydrodynamics, they are one of the possible routes to turbulence.[2]

Period-halving bifurcations (L) leading to order, followed by period-doubling bifurcations (R) leading to chaos.

Examples edit

 
Bifurcation diagram for the logistic map. It shows the attractor values, like   and  , as a function of the parameter  .

Logistic map edit

The logistic map is

 

where   is a function of the (discrete) time  .[3] The parameter   is assumed to lie in the interval  , in which case   is bounded on  .

For   between 1 and 3,   converges to the stable fixed point  . Then, for   between 3 and 3.44949,   converges to a permanent oscillation between two values   and   that depend on  . As   grows larger, oscillations between 4 values, then 8, 16, 32, etc. appear. These period doublings culminate at  , beyond which more complex regimes appear. As   increases, there are some intervals where most starting values will converge to one or a small number of stable oscillations, such as near  .

In the interval where the period is   for some positive integer  , not all the points actually have period  . These are single points, rather than intervals. These points are said to be in unstable orbits, since nearby points do not approach the same orbit as them.

Quadratic map edit

Real version of complex quadratic map is related with real slice of the Mandelbrot set.

Kuramoto–Sivashinsky equation edit

 
Period doubling in the Kuramoto–Sivashinsky equation with periodic boundary conditions. The curves depict solutions of the Kuramoto–Sivashinsky equation projected onto the energy phase plane (E, dE/dt), where E is the L2-norm of the solution. For ν = 0.056, there exists a periodic orbit with period T ≈ 1.1759. Near ν ≈ 0.0558, this solution splits into 2 orbits, which further separate as ν is decreased. Exactly at the transitional value of ν, the new orbit (red-dashed) has double the period of the original. (However, as ν increases further, the ratio of periods deviates from exactly 2.)

The Kuramoto–Sivashinsky equation is an example of a spatiotemporally continuous dynamical system that exhibits period doubling. It is one of the most well-studied nonlinear partial differential equations, originally introduced as a model of flame front propagation.[4]

The one-dimensional Kuramoto–Sivashinsky equation is

 

A common choice for boundary conditions is spatial periodicity:  .

For large values of  ,   evolves toward steady (time-independent) solutions or simple periodic orbits. As   is decreased, the dynamics eventually develops chaos. The transition from order to chaos occurs via a cascade of period-doubling bifurcations,[5][6] one of which is illustrated in the figure.

Logistic map for a modified Phillips curve edit

Consider the following logistical map for a modified Phillips curve:

 

 

 

 

where :

  •   is the actual inflation
  •   is the expected inflation,
  • u is the level of unemployment,
  •   is the money supply growth rate.

Keeping   and varying  , the system undergoes period-doubling bifurcations and ultimately becomes chaotic.[citation needed]

Experimental observation edit

Period doubling has been observed in a number of experimental systems.[7] There is also experimental evidence of period-doubling cascades. For example, sequences of 4 period doublings have been observed in the dynamics of convection rolls in water and mercury.[8][9] Similarly, 4-5 doublings have been observed in certain nonlinear electronic circuits.[10][11][12] However, the experimental precision required to detect the ith doubling event in a cascade increases exponentially with i, making it difficult to observe more than 5 doubling events in a cascade.[13]

See also edit

Notes edit

  1. ^ Alligood (1996) et al., p. 532
  2. ^ Thorne, Kip S.; Blandford, Roger D. (2017). Modern Classical Physics: Optics, Fluids, Plasmas, Elasticity, Relativity, and Statistical Physics. Princeton University Press. pp. 825–834. ISBN 9780691159027.
  3. ^ Strogatz (2015), pp. 360–373
  4. ^ Kalogirou, A.; Keaveny, E. E.; Papageorgiou, D. T. (2015). "An in-depth numerical study of the two-dimensional Kuramoto–Sivashinsky equation". Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences. 471 (2179): 20140932. Bibcode:2015RSPSA.47140932K. doi:10.1098/rspa.2014.0932. ISSN 1364-5021. PMC 4528647. PMID 26345218.
  5. ^ Smyrlis, Y. S.; Papageorgiou, D. T. (1991). "Predicting chaos for infinite dimensional dynamical systems: the Kuramoto-Sivashinsky equation, a case study". Proceedings of the National Academy of Sciences. 88 (24): 11129–11132. Bibcode:1991PNAS...8811129S. doi:10.1073/pnas.88.24.11129. ISSN 0027-8424. PMC 53087. PMID 11607246.
  6. ^ Papageorgiou, D.T.; Smyrlis, Y.S. (1991), "The route to chaos for the Kuramoto-Sivashinsky equation", Theoretical and Computational Fluid Dynamics, 3 (1): 15–42, Bibcode:1991ThCFD...3...15P, doi:10.1007/BF00271514, hdl:2060/19910004329, ISSN 1432-2250, S2CID 116955014
  7. ^ see Strogatz (2015) for a review
  8. ^ Giglio, Marzio; Musazzi, Sergio; Perini, Umberto (1981). "Transition to Chaotic Behavior via a Reproducible Sequence of Period-Doubling Bifurcations". Physical Review Letters. 47 (4): 243–246. Bibcode:1981PhRvL..47..243G. doi:10.1103/PhysRevLett.47.243. ISSN 0031-9007.
  9. ^ Libchaber, A.; Laroche, C.; Fauve, S. (1982). "Period doubling cascade in mercury, a quantitative measurement" (PDF). Journal de Physique Lettres. 43 (7): 211–216. doi:10.1051/jphyslet:01982004307021100. ISSN 0302-072X.
  10. ^ Linsay, Paul S. (1981). "Period Doubling and Chaotic Behavior in a Driven Anharmonic Oscillator". Physical Review Letters. 47 (19): 1349–1352. Bibcode:1981PhRvL..47.1349L. doi:10.1103/PhysRevLett.47.1349. ISSN 0031-9007.
  11. ^ Testa, James; Pérez, José; Jeffries, Carson (1982). "Evidence for Universal Chaotic Behavior of a Driven Nonlinear Oscillator". Physical Review Letters. 48 (11): 714–717. Bibcode:1982PhRvL..48..714T. doi:10.1103/PhysRevLett.48.714. ISSN 0031-9007.
  12. ^ Arecchi, F. T.; Lisi, F. (1982). "Hopping Mechanism Generating1fNoise in Nonlinear Systems". Physical Review Letters. 49 (2): 94–98. Bibcode:1982PhRvL..49...94A. doi:10.1103/PhysRevLett.49.94. ISSN 0031-9007.
  13. ^ Strogatz (2015), pp. 360–373

References edit

  • Alligood, Kathleen T.; Sauer, Tim; Yorke, James (1996). Chaos: An Introduction to Dynamical Systems. Textbooks in Mathematical Sciences. Springer-Verlag New York. doi:10.1007/0-387-22492-0_3. ISBN 978-0-387-94677-1. ISSN 1431-9381.
  • Giglio, Marzio; Musazzi, Sergio; Perini, Umberto (1981). "Transition to Chaotic Behavior via a Reproducible Sequence of Period-Doubling Bifurcations". Physical Review Letters. 47 (4): 243–246. Bibcode:1981PhRvL..47..243G. doi:10.1103/PhysRevLett.47.243. ISSN 0031-9007.
  • Kalogirou, A.; Keaveny, E. E.; Papageorgiou, D. T. (2015). "An in-depth numerical study of the two-dimensional Kuramoto–Sivashinsky equation". Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences. 471 (2179): 20140932. Bibcode:2015RSPSA.47140932K. doi:10.1098/rspa.2014.0932. ISSN 1364-5021. PMC 4528647. PMID 26345218.
  • Kuznetsov, Yuri A. (2004). Elements of Applied Bifurcation Theory. Applied Mathematical Sciences. Vol. 112 (3rd ed.). Springer-Verlag. ISBN 0-387-21906-4. Zbl 1082.37002.
  • Libchaber, A.; Laroche, C.; Fauve, S. (1982). "Period doubling cascade in mercury, a quantitative measurement" (PDF). Journal de Physique Lettres. 43 (7): 211–216. doi:10.1051/jphyslet:01982004307021100. ISSN 0302-072X.
  • Papageorgiou, D.T.; Smyrlis, Y.S. (1991), "The route to chaos for the Kuramoto-Sivashinsky equation", Theoret. Comput. Fluid Dynamics, 3 (1): 15–42, Bibcode:1991ThCFD...3...15P, doi:10.1007/BF00271514, hdl:2060/19910004329, ISSN 1432-2250, S2CID 116955014
  • Smyrlis, Y. S.; Papageorgiou, D. T. (1991). "Predicting chaos for infinite dimensional dynamical systems: the Kuramoto-Sivashinsky equation, a case study". Proceedings of the National Academy of Sciences. 88 (24): 11129–11132. Bibcode:1991PNAS...8811129S. doi:10.1073/pnas.88.24.11129. ISSN 0027-8424. PMC 53087. PMID 11607246.
  • Strogatz, Steven (2015). Nonlinear Dynamics and Chaos: With applications to Physics, Biology, Chemistry and Engineering (2nd ed.). CRC Press. ISBN 978-0813349107.
  • Cheung, P. Y.; Wong, A. Y. (1987). "Chaotic behavior and period doubling in plasmas". Physical Review Letters. 59 (5): 551–554. Bibcode:1987PhRvL..59..551C. doi:10.1103/PhysRevLett.59.551. ISSN 0031-9007. PMID 10035803.

External links edit

  • Connecting period-doubling cascades to chaos

period, doubling, bifurcation, dynamical, systems, theory, period, doubling, bifurcation, occurs, when, slight, change, system, parameters, causes, periodic, trajectory, emerge, from, existing, periodic, trajectory, having, double, period, original, with, doub. In dynamical systems theory a period doubling bifurcation occurs when a slight change in a system s parameters causes a new periodic trajectory to emerge from an existing periodic trajectory the new one having double the period of the original With the doubled period it takes twice as long or in a discrete dynamical system twice as many iterations for the numerical values visited by the system to repeat themselves A period halving bifurcation occurs when a system switches to a new behavior with half the period of the original system A period doubling cascade is an infinite sequence of period doubling bifurcations Such cascades are a common route by which dynamical systems develop chaos 1 In hydrodynamics they are one of the possible routes to turbulence 2 Period halving bifurcations L leading to order followed by period doubling bifurcations R leading to chaos Contents 1 Examples 1 1 Logistic map 1 2 Quadratic map 1 3 Kuramoto Sivashinsky equation 1 4 Logistic map for a modified Phillips curve 2 Experimental observation 3 See also 4 Notes 5 References 6 External linksExamples edit nbsp Bifurcation diagram for the logistic map It shows the attractor values like x displaystyle x nbsp and x displaystyle x nbsp as a function of the parameter r displaystyle r nbsp Logistic map edit The logistic map is x n 1 r x n 1 x n displaystyle x n 1 rx n 1 x n nbsp where x n displaystyle x n nbsp is a function of the discrete time n 0 1 2 displaystyle n 0 1 2 ldots nbsp 3 The parameter r displaystyle r nbsp is assumed to lie in the interval 0 4 displaystyle 0 4 nbsp in which case x n displaystyle x n nbsp is bounded on 0 1 displaystyle 0 1 nbsp For r displaystyle r nbsp between 1 and 3 x n displaystyle x n nbsp converges to the stable fixed point x r 1 r displaystyle x r 1 r nbsp Then for r displaystyle r nbsp between 3 and 3 44949 x n displaystyle x n nbsp converges to a permanent oscillation between two values x displaystyle x nbsp and x displaystyle x nbsp that depend on r displaystyle r nbsp As r displaystyle r nbsp grows larger oscillations between 4 values then 8 16 32 etc appear These period doublings culminate at r 3 56995 displaystyle r approx 3 56995 nbsp beyond which more complex regimes appear As r displaystyle r nbsp increases there are some intervals where most starting values will converge to one or a small number of stable oscillations such as near r 3 83 displaystyle r 3 83 nbsp In the interval where the period is 2 n displaystyle 2 n nbsp for some positive integer n displaystyle n nbsp not all the points actually have period 2 n displaystyle 2 n nbsp These are single points rather than intervals These points are said to be in unstable orbits since nearby points do not approach the same orbit as them Quadratic map edit Real version of complex quadratic map is related with real slice of the Mandelbrot set nbsp Period doubling cascade in an exponential mapping of the Mandelbrot set nbsp 1D version with an exponential mapping nbsp period doubling bifurcation Kuramoto Sivashinsky equation edit nbsp Period doubling in the Kuramoto Sivashinsky equation with periodic boundary conditions The curves depict solutions of the Kuramoto Sivashinsky equation projected onto the energy phase plane E dE dt where E is the L2 norm of the solution For n 0 056 there exists a periodic orbit with period T 1 1759 Near n 0 0558 this solution splits into 2 orbits which further separate as n is decreased Exactly at the transitional value of n the new orbit red dashed has double the period of the original However as n increases further the ratio of periods deviates from exactly 2 The Kuramoto Sivashinsky equation is an example of a spatiotemporally continuous dynamical system that exhibits period doubling It is one of the most well studied nonlinear partial differential equations originally introduced as a model of flame front propagation 4 The one dimensional Kuramoto Sivashinsky equation is u t u u x u x x n u x x x x 0 displaystyle u t uu x u xx nu u xxxx 0 nbsp A common choice for boundary conditions is spatial periodicity u x 2 p t u x t displaystyle u x 2 pi t u x t nbsp For large values of n displaystyle nu nbsp u x t displaystyle u x t nbsp evolves toward steady time independent solutions or simple periodic orbits As n displaystyle nu nbsp is decreased the dynamics eventually develops chaos The transition from order to chaos occurs via a cascade of period doubling bifurcations 5 6 one of which is illustrated in the figure Logistic map for a modified Phillips curve edit Consider the following logistical map for a modified Phillips curve p t f u t b p t e displaystyle pi t f u t b pi t e nbsp p t 1 p t e c p t p t e displaystyle pi t 1 pi t e c pi t pi t e nbsp f u b 1 b 2 e u displaystyle f u beta 1 beta 2 e u nbsp b gt 0 0 c 1 d f d u lt 0 displaystyle b gt 0 0 leq c leq 1 frac df du lt 0 nbsp where p displaystyle pi nbsp is the actual inflation p e displaystyle pi e nbsp is the expected inflation u is the level of unemployment m p displaystyle m pi nbsp is the money supply growth rate Keeping b 1 2 5 b 2 20 c 0 75 displaystyle beta 1 2 5 beta 2 20 c 0 75 nbsp and varying b displaystyle b nbsp the system undergoes period doubling bifurcations and ultimately becomes chaotic citation needed Experimental observation editPeriod doubling has been observed in a number of experimental systems 7 There is also experimental evidence of period doubling cascades For example sequences of 4 period doublings have been observed in the dynamics of convection rolls in water and mercury 8 9 Similarly 4 5 doublings have been observed in certain nonlinear electronic circuits 10 11 12 However the experimental precision required to detect the ith doubling event in a cascade increases exponentially with i making it difficult to observe more than 5 doubling events in a cascade 13 See also editList of chaotic maps Complex quadratic map Feigenbaum constants Universality dynamical systems Sharkovskii s theoremNotes edit Alligood 1996 et al p 532 Thorne Kip S Blandford Roger D 2017 Modern Classical Physics Optics Fluids Plasmas Elasticity Relativity and Statistical Physics Princeton University Press pp 825 834 ISBN 9780691159027 Strogatz 2015 pp 360 373 Kalogirou A Keaveny E E Papageorgiou D T 2015 An in depth numerical study of the two dimensional Kuramoto Sivashinsky equation Proceedings of the Royal Society A Mathematical Physical and Engineering Sciences 471 2179 20140932 Bibcode 2015RSPSA 47140932K doi 10 1098 rspa 2014 0932 ISSN 1364 5021 PMC 4528647 PMID 26345218 Smyrlis Y S Papageorgiou D T 1991 Predicting chaos for infinite dimensional dynamical systems the Kuramoto Sivashinsky equation a case study Proceedings of the National Academy of Sciences 88 24 11129 11132 Bibcode 1991PNAS 8811129S doi 10 1073 pnas 88 24 11129 ISSN 0027 8424 PMC 53087 PMID 11607246 Papageorgiou D T Smyrlis Y S 1991 The route to chaos for the Kuramoto Sivashinsky equation Theoretical and Computational Fluid Dynamics 3 1 15 42 Bibcode 1991ThCFD 3 15P doi 10 1007 BF00271514 hdl 2060 19910004329 ISSN 1432 2250 S2CID 116955014 see Strogatz 2015 for a review Giglio Marzio Musazzi Sergio Perini Umberto 1981 Transition to Chaotic Behavior via a Reproducible Sequence of Period Doubling Bifurcations Physical Review Letters 47 4 243 246 Bibcode 1981PhRvL 47 243G doi 10 1103 PhysRevLett 47 243 ISSN 0031 9007 Libchaber A Laroche C Fauve S 1982 Period doubling cascade in mercury a quantitative measurement PDF Journal de Physique Lettres 43 7 211 216 doi 10 1051 jphyslet 01982004307021100 ISSN 0302 072X Linsay Paul S 1981 Period Doubling and Chaotic Behavior in a Driven Anharmonic Oscillator Physical Review Letters 47 19 1349 1352 Bibcode 1981PhRvL 47 1349L doi 10 1103 PhysRevLett 47 1349 ISSN 0031 9007 Testa James Perez Jose Jeffries Carson 1982 Evidence for Universal Chaotic Behavior of a Driven Nonlinear Oscillator Physical Review Letters 48 11 714 717 Bibcode 1982PhRvL 48 714T doi 10 1103 PhysRevLett 48 714 ISSN 0031 9007 Arecchi F T Lisi F 1982 Hopping Mechanism Generating1fNoise in Nonlinear Systems Physical Review Letters 49 2 94 98 Bibcode 1982PhRvL 49 94A doi 10 1103 PhysRevLett 49 94 ISSN 0031 9007 Strogatz 2015 pp 360 373References editAlligood Kathleen T Sauer Tim Yorke James 1996 Chaos An Introduction to Dynamical Systems Textbooks in Mathematical Sciences Springer Verlag New York doi 10 1007 0 387 22492 0 3 ISBN 978 0 387 94677 1 ISSN 1431 9381 Giglio Marzio Musazzi Sergio Perini Umberto 1981 Transition to Chaotic Behavior via a Reproducible Sequence of Period Doubling Bifurcations Physical Review Letters 47 4 243 246 Bibcode 1981PhRvL 47 243G doi 10 1103 PhysRevLett 47 243 ISSN 0031 9007 Kalogirou A Keaveny E E Papageorgiou D T 2015 An in depth numerical study of the two dimensional Kuramoto Sivashinsky equation Proceedings of the Royal Society A Mathematical Physical and Engineering Sciences 471 2179 20140932 Bibcode 2015RSPSA 47140932K doi 10 1098 rspa 2014 0932 ISSN 1364 5021 PMC 4528647 PMID 26345218 Kuznetsov Yuri A 2004 Elements of Applied Bifurcation Theory Applied Mathematical Sciences Vol 112 3rd ed Springer Verlag ISBN 0 387 21906 4 Zbl 1082 37002 Libchaber A Laroche C Fauve S 1982 Period doubling cascade in mercury a quantitative measurement PDF Journal de Physique Lettres 43 7 211 216 doi 10 1051 jphyslet 01982004307021100 ISSN 0302 072X Papageorgiou D T Smyrlis Y S 1991 The route to chaos for the Kuramoto Sivashinsky equation Theoret Comput Fluid Dynamics 3 1 15 42 Bibcode 1991ThCFD 3 15P doi 10 1007 BF00271514 hdl 2060 19910004329 ISSN 1432 2250 S2CID 116955014 Smyrlis Y S Papageorgiou D T 1991 Predicting chaos for infinite dimensional dynamical systems the Kuramoto Sivashinsky equation a case study Proceedings of the National Academy of Sciences 88 24 11129 11132 Bibcode 1991PNAS 8811129S doi 10 1073 pnas 88 24 11129 ISSN 0027 8424 PMC 53087 PMID 11607246 Strogatz Steven 2015 Nonlinear Dynamics and Chaos With applications to Physics Biology Chemistry and Engineering 2nd ed CRC Press ISBN 978 0813349107 Cheung P Y Wong A Y 1987 Chaotic behavior and period doubling in plasmas Physical Review Letters 59 5 551 554 Bibcode 1987PhRvL 59 551C doi 10 1103 PhysRevLett 59 551 ISSN 0031 9007 PMID 10035803 External links editConnecting period doubling cascades to chaos Retrieved from https en wikipedia org w index php title Period doubling bifurcation amp oldid 1221894499, wikipedia, wiki, book, books, library,

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