Discrete logistic map - umu.se · Peter Olsson (Ume a University) Discrete logistic map September...
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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
Transcript of Discrete logistic map - umu.se · Peter Olsson (Ume a University) Discrete logistic map September...
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
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
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
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).
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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
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
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
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
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
