9. = OK
⊂
R?
R
( )
( )
/////////////
!
( ) R 2009 3 1 3 / 23
10. 3
x = −x
¨
( ) x = −x + c x
¨ ˙
!) x = −x + c(1 − x2 ) x
Van der Pol ( ¨ ˙
Lorenz attractor ( !) x = σ(y − x)
˙
y = x(ρ − z) − y
˙
z = xy − βz
˙
( ) R 2009 3 1 4 / 23
17. 1: Saddle-Node Bifurcation (1/2)
: x = x2 − r
˙
x=0
˙
! x = x2 − rx = (x + r)(x − r)
˙
√
x=± r( )
r>0
y y y
y = x^2 - r
dx/dt < 0
x x x
dx/dt > 0
dx/dt > 0 dx/dt > 0
dx/dt > 0
(a) r < 0 (b) r = 0 (c) r > 0
( ) R 2009 3 1 11 / 23
18. 1: Saddle-Node Bifurcation (2/2)
: x = x2 − r
˙
(a) r < 0: ( )
(b) r = 0:
x<0 x=0
( )
x>0
(c) r > 0: √
x < √r x=0
( )
x> r
y y y
y = x^2 - r
dx/dt < 0
x x x
dx/dt > 0
dx/dt > 0 dx/dt > 0
dx/dt > 0
(a) r < 0 (b) r = 0 (c) r > 0
( ) R 2009 3 1 12 / 23
19. 2: Pitchfork Bifurcation (1/2)
: x = −x3 + rx
˙
x=0
˙
x
! x = −x3 + rx = − 3 (x + r)(x − r)
˙
√
x=± r( )
r>0
x=0
y y y
y = x^3 + rx
dx/dt < 0
dx/dt < 0
dx/dt < 0
dx/dt < 0
x x x
dx/dt > 0
dx/dt > 0 dx/dt > 0
dx/dt > 0
(a) r < 0 (b) r = 0 (c) r > 0
( ) R 2009 3 1 13 / 23
20. 2: Pitchfork Bifurcation (2/2)
: x = −x3 + rx
˙
(a) r < 0: x = 0
(b) r = 0: x = 0
(c) r > 0: √
x<0 x = − √r
x>0 x=+ r
( )
x=0
y y y
y = x^3 + rx
dx/dt < 0
dx/dt < 0
dx/dt < 0
dx/dt < 0
x x x
dx/dt > 0
dx/dt > 0 dx/dt > 0
dx/dt > 0
(a) r < 0 (b) r = 0 (c) r > 0
( ) R 2009 3 1 14 / 23
32. 3 :
, ,
:
Saddle-Node Bifurcation
Pitchfork Bifurcation
R
( ) R 2009 3 1 22 / 23
33. Kathleen T. Alligood Tim Sauer James A.
Yorke, “Chaos: An Introduction to Dynamical
Systems”, Springer, 1997
Steven H. Strogatz, “Nonlinear Dynamics and
Chaos: With Applications to Physics, Biology,
Chemistry, and Engineering”, Westview Pr, 2001
Randall D. Beer, “On the Dynamics of Small
Continuous-Time Recurrent Neural Networks”,
Adaptive Behavior, Vol. 3, No. 4, 469-509 (1995)
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