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Jordan & Smith Mathematical Techniques 4e Pdf

Mathematical constants related to chaotic behavior

Feigenbaum constant δ expresses the limit of the ratio of distances between consecutive bifurcation diagram on L i / L i + 1

In mathematics, specifically bifurcation theory, the Feigenbaum constants are two mathematical constants which both express ratios in a bifurcation diagram for a non-linear map. They are named after the physicist Mitchell J. Feigenbaum.

History [edit]

Feigenbaum originally related the first constant to the period-doubling bifurcations in the logistic map, but also showed it to hold for all one-dimensional maps with a single quadratic maximum. As a consequence of this generality, every chaotic system that corresponds to this description will bifurcate at the same rate. Feigenbaum made this discovery in 1975,[1] [2] and he officially published it in 1978.[3]

The first constant [edit]

The first Feigenbaum constant δ is the limiting ratio of each bifurcation interval to the next between every period doubling, of a one-parameter map

x i + 1 = f ( x i ) , {\displaystyle x_{i+1}=f(x_{i}),}

where f(x) is a function parameterized by the bifurcation parameter a .

It is given by the limit[4]

δ = lim n a n 1 a n 2 a n a n 1 = 4.669 201 609 , {\displaystyle \delta =\lim _{n\to \infty }{\frac {a_{n-1}-a_{n-2}}{a_{n}-a_{n-1}}}=4.669\,201\,609\,\ldots ,}

where an are discrete values of a at the n th period doubling.

Names [edit]

  • Feigenbaum bifurcation velocity
  • delta

Value [edit]

  • 30 decimal places : δ = 4.669201 609 102 990 671 853 203 820 466
  • (sequence A006890 in the OEIS)
  • A simple rational approximation is: 621 / 133 , which is correct to 5 significant values (when rounding). For more precision use 1228 / 263 , which is correct to 7 significant values.
  • Is approximately equal to 10( 1 / π − 1 ), with an error of 0.0015%

Illustration [edit]

Non-linear maps [edit]

To see how this number arises, consider the real one-parameter map

f ( x ) = a x 2 . {\displaystyle f(x)=a-x^{2}.}

Here a is the bifurcation parameter, x is the variable. The values of a for which the period doubles (e.g. the largest value for a with no period-2 orbit, or the largest a with no period-4 orbit), are a 1 , a 2 etc. These are tabulated below:[5]

n Period Bifurcation parameter ( an ) Ratio a n−1a n−2 / a n a n−1
1 2 0.75
2 4 1.25
3 8 1.3680989 4.2337
4 16 1.3940462 4.5515
5 32 1.3996312 4.6458
6 64 1.4008286 4.6639
7 128 1.4010853 4.6682
8 256 1.4011402 4.6689

The ratio in the last column converges to the first Feigenbaum constant. The same number arises for the logistic map

f ( x ) = a x ( 1 x ) {\displaystyle f(x)=ax(1-x)}

with real parameter a and variable x . Tabulating the bifurcation values again:[6]

n Period Bifurcation parameter ( an ) Ratio a n−1a n−2 / a n a n−1
1 2 3
2 4 3.4494897
3 8 3.5440903 4.7514
4 16 3.5644073 4.6562
5 32 3.5687594 4.6683
6 64 3.5696916 4.6686
7 128 3.5698913 4.6692
8 256 3.5699340 4.6694

Fractals [edit]

Self-similarity in the Mandelbrot set shown by zooming in on a round feature while panning in the negative- x direction. The display center pans from (−1, 0) to (−1.31, 0) while the view magnifies from 0.5 × 0.5 to 0.12 × 0.12 to approximate the Feigenbaum ratio.

In the case of the Mandelbrot set for complex quadratic polynomial

f ( z ) = z 2 + c {\displaystyle f(z)=z^{2}+c}

the Feigenbaum constant is the ratio between the diameters of successive circles on the real axis in the complex plane (see animation on the right).

n Period = 2 n Bifurcation parameter ( cn ) Ratio = c n 1 c n 2 c n c n 1 {\displaystyle ={\dfrac {c_{n-1}-c_{n-2}}{c_{n}-c_{n-1}}}}
1 2 −0.75
2 4 −1.25
3 8 −1.3680989 4.2337
4 16 −1.3940462 4.5515
5 32 −1.3996312 4.6458
6 64 −1.4008287 4.6639
7 128 −1.4010853 4.6682
8 256 −1.4011402 4.6689
9 512 −1.401151 982 029
10 1024 −1.401154 502 237
−1.401155 1890

Bifurcation parameter is a root point of period-2 n component. This series converges to the Feigenbaum point c = −1.401155...... The ratio in the last column converges to the first Feigenbaum constant.

Other maps also reproduce this ratio, in this sense the Feigenbaum constant in bifurcation theory is analogous to π in geometry and e in calculus.

The second constant [edit]

The second Feigenbaum constant or Feigenbaum's alpha constant (sequence A006891 in the OEIS),

α = 2.502 907 875 095 892 822 283 902 873 218... , {\displaystyle \alpha =2.502\,907\,875\,095\,892\,822\,283\,902\,873\,218...,}

is the ratio between the width of a tine and the width of one of its two subtines (except the tine closest to the fold). A negative sign is applied to α when the ratio between the lower subtine and the width of the tine is measured.[7]

These numbers apply to a large class of dynamical systems (for example, dripping faucets to population growth).[7]

A simple rational approximation is 13 / 11 × 17 / 11 × 37 / 27 = 8177 / 3267 .

Properties [edit]

Both numbers are believed to be transcendental, although they have not been proven to be so.[8] There is also no known proof that either constant is irrational.

The first proof of the universality of the Feigenbaum constants carried out by Oscar Lanford—with computer-assistance—in 1982[9] (with a small correction by Jean-Pierre Eckmann and Peter Wittwer of the University of Geneva in 1987[10]). Over the years, non-numerical methods were discovered for different parts of the proof, aiding Mikhail Lyubich in producing the first complete non-numerical proof.[11]

See also [edit]

  • Bifurcation diagram
  • Bifurcation theory
  • Cascading failure
  • Feigenbaum function
  • List of chaotic maps

Notes [edit]

  1. ^ Feigenbaum, M. J. (1976). "Universality in complex discrete dynamics" (PDF). Los Alamos Theoretical Division Annual Report 1975–1976.
  2. ^ Alligood, K. T.; Sauer, T. D.; Yorke, J. A. (1996). Chaos: An Introduction to Dynamical Systems. Springer. ISBN0-387-94677-2.
  3. ^ Feigenbaum, Mitchell J. (1978). "Quantitative universality for a class of nonlinear transformations". Journal of Statistical Physics. 19 (1): 25–52. doi:10.1007/BF01020332. S2CID 124498882.
  4. ^ Jordan, D. W.; Smith, P. (2007). Non-Linear Ordinary Differential Equations: Introduction for Scientists and Engineers (4th ed.). Oxford University Press. ISBN978-0-19-920825-8.
  5. ^ Alligood, p. 503.
  6. ^ Alligood, p. 504.
  7. ^ a b Strogatz, Steven H. (1994). Nonlinear Dynamics and Chaos. Studies in Nonlinearity. Perseus Books. ISBN978-0-7382-0453-6.
  8. ^ Briggs, Keith (1997). Feigenbaum scaling in discrete dynamical systems (PDF) (PhD thesis). University of Melbourne.
  9. ^ Lanford III, Oscar (1982). "A computer-assisted proof of the Feigenbaum conjectures". Bull. Amer. Math. Soc. 6 (3): 427–434. doi:10.1090/S0273-0979-1982-15008-X.
  10. ^ Eckmann, J. P.; Wittwer, P. (1987). "A complete proof of the Feigenbaum conjectures". Journal of Statistical Physics. 46 (3–4): 455. Bibcode:1987JSP....46..455E. doi:10.1007/BF01013368. S2CID 121353606.
  11. ^ Lyubich, Mikhail (1999). "Feigenbaum-Coullet-Tresser universality and Milnor's Hairiness Conjecture". Annals of Mathematics. 149 (2): 319–420. arXiv:math/9903201. Bibcode:1999math......3201L. doi:10.2307/120968. JSTOR 120968. S2CID 119594350.

References [edit]

  • Alligood, Kathleen T., Tim D. Sauer, James A. Yorke, Chaos: An Introduction to Dynamical Systems, Textbooks in mathematical sciences Springer, 1996, ISBN 978-0-38794-677-1
  • Briggs, Keith (July 1991). "A Precise Calculation of the Feigenbaum Constants" (PDF). Mathematics of Computation. 57 (195): 435–439. Bibcode:1991MaCom..57..435B. doi:10.1090/S0025-5718-1991-1079009-6.
  • Briggs, Keith (1997). Feigenbaum scaling in discrete dynamical systems (PDF) (PhD thesis). University of Melbourne.
  • Broadhurst, David (22 March 1999). "Feigenbaum constants to 1018 decimal places".
  • Weisstein, Eric W. "Feigenbaum Constant". MathWorld.

External links [edit]

  • Feigenbaum Constant – from Wolfram MathWorld
  • OEIS sequence A006890 (Decimal expansion of Feigenbaum bifurcation velocity)
OEIS sequence A006891 (Decimal expansion of Feigenbaum reduction parameter)
OEIS sequence A094078 (Decimal expansion of Pi + arctan(e^Pi))
  • Feigenbaum constant – PlanetMath
  • Moriarty, Philip; Bowley, Roger (2009). " δ – Feigenbaum Constant". Sixty Symbols. Brady Haran for the University of Nottingham.

Jordan & Smith Mathematical Techniques 4e Pdf

Source: https://en.wikipedia.org/wiki/Feigenbaum_constants

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