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Definition The logistic map is defined by u t +1 = ru t (1 - u t ), 0 < r < 4. The steady states and the corresponding eigenvalues λ = f 0 (u * ) are u * 1 =0, λ 1 = r , u * 2 = r - 1 r , λ 2 =2 - r . Curves for r = 1, 1.5,. . . 3.5. 0.0 0.2 0.4 0.6 0.8 1.0 0.0 0.2 0.4 0.6 0.8 1.0 u t u t+1 Peter Olsson (Ume˚ a University) Discrete logistic map September 12, 2019 1/1
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Discrete logistic map - umu.se · Peter Olsson (Ume a University) Discrete logistic map September 12, 2019 6/1. The path to chaos For 1

Sep 27, 2020

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Page 1: Discrete logistic map - umu.se · Peter Olsson (Ume a University) Discrete logistic map September 12, 2019 6/1. The path to chaos For 1

DefinitionThe logistic map is defined by

ut+1 = rut(1− ut), 0 < r < 4.

The steady states and the corresponding eigenvalues λ = f ′(u∗) are

u∗1 = 0, λ1 = r ,

u∗2 =r − 1

r, λ2 = 2− r .

Curves for r = 1, 1.5,. . . 3.5.0.0 0.2 0.4 0.6 0.8 1.0

0.0

0.2

0.4

0.6

0.8

1.0

ut

ut+

1

Peter Olsson (Ume̊a University) Discrete logistic map September 12, 2019 1 / 1

Page 2: Discrete logistic map - umu.se · Peter Olsson (Ume a University) Discrete logistic map September 12, 2019 6/1. The path to chaos For 1

Stable fixed point r = 2.8, λ = 2− r = −0.8

0 10

1

ut

ut+

1

0 10 200

1

t

ut

Peter Olsson (Ume̊a University) Discrete logistic map September 12, 2019 2 / 1

Page 3: Discrete logistic map - umu.se · Peter Olsson (Ume a University) Discrete logistic map September 12, 2019 6/1. The path to chaos For 1

Unstable fixed point r = 3.2, λ = 2− r = −1.2

0 10

1

ut

ut+

1

0 10 200

1

t

ut

Peter Olsson (Ume̊a University) Discrete logistic map September 12, 2019 3 / 1

Page 4: Discrete logistic map - umu.se · Peter Olsson (Ume a University) Discrete logistic map September 12, 2019 6/1. The path to chaos For 1

To understand period doubling

Consider the map from ut to ut+2 defined by

ut+1 = rut(1− ut),

ut+2 = rut+1(1− ut+1).

0 10

1

A

B

C

ut

ut+

2,

ut+

1

Figure for r = 3.2.

Peter Olsson (Ume̊a University) Discrete logistic map September 12, 2019 4 / 1

Page 5: Discrete logistic map - umu.se · Peter Olsson (Ume a University) Discrete logistic map September 12, 2019 6/1. The path to chaos For 1

Period doubling, again!

Figure for r = 3.5

0 10

1

A

B

C

ut

ut+

2,

ut+

1

The behaviors at A and C are unstable, f ′ < −1!

Peter Olsson (Ume̊a University) Discrete logistic map September 12, 2019 5 / 1

Page 6: Discrete logistic map - umu.se · Peter Olsson (Ume a University) Discrete logistic map September 12, 2019 6/1. The path to chaos For 1

Oscillations with period 4, r = 3.5.

0 10 20 300

1

t

ut

The same reasoning may be applied for ut+4 which gives an oscillation ofperiod eight. . . this period doubling may be continued without limit.

Peter Olsson (Ume̊a University) Discrete logistic map September 12, 2019 6 / 1

Page 7: Discrete logistic map - umu.se · Peter Olsson (Ume a University) Discrete logistic map September 12, 2019 6/1. The path to chaos For 1

The path to chaos

For 1 < r ≤ 3 there is a unique solution (r − 1)/r .

For 3 < r ≤ 1 +√

6(≈ 3.45) the system has periodic fluctuationsbetween two values.

For 1 +√

6 < r < 3.54 (approximately) the system has periodicoscillations between four values.

For 3.54 < r < 3.57 the system oscillates between 8, 16, 32, values,etc.

At r ≈ 3.57 is the onset of chaos. We can no longer see anyoscillations of finite period and slight variations in the initial valueyields dramatically different results over time.

Peter Olsson (Ume̊a University) Discrete logistic map September 12, 2019 7 / 1

Page 8: Discrete logistic map - umu.se · Peter Olsson (Ume a University) Discrete logistic map September 12, 2019 6/1. The path to chaos For 1

Period doublings and the onset of chaos

1 2 3 40.0

0.5

1.0

r

ut

Peter Olsson (Ume̊a University) Discrete logistic map September 12, 2019 8 / 1