chaos in low-dimensional lotka-volterra models of competition
DESCRIPTION
Chaos in Low-Dimensional Lotka-Volterra Models of Competition. J. C. Sprott Department of Physics University of Wisconsin - Madison Presented at the UW Chaos and Complex System Seminar on February 3, 2004. Collaborators. John Vano Joe Wildenberg Mike Anderson Jeff Noel. Rabbit Dynamics. - PowerPoint PPT PresentationTRANSCRIPT
Chaos in Low-Dimensional Lotka-Volterra Models of Competition
J. C. Sprott
Department of PhysicsUniversity of Wisconsin - Madison
Presented at the
UW Chaos and Complex System Seminaron February 3, 2004
Collaborators
John Vano
Joe Wildenberg
Mike Anderson
Jeff Noel
Rabbit Dynamics Let R = # of rabbits dR/dt = bR - dR
Birth rate Death rate
= rR
• r > 0 growth
• r = 0 equilibrium
• r < 0 extinction
r = b - d
Logistic Differential Equation dR/dt = rR(1 – R)
R
rt
Exponentialgrowth
Nonlinearsaturation
• Let xi be population of the ith species
(rabbits, trees, people, stocks, …)
• dxi / dt = rixi (1 - Σ aijxj )
• Parameters of the model:
• Vector of growth rates ri
• Matrix of interactions aij
• Number of species N
Multispecies Lotka-Volterra Model
j=1
N
Parameters of the Model
1r2
r3
r4
r5
r6
1 a12 a13 a14 a15 a16
a21 1 a23 a24 a25 a26
a31 a32 1 a34 a35 a36
a41 a42 a43 1 a45 a46
a51 a52 a53 a54 1 a56
a61 a62 a63 a64 a65 1
Growthrates Interaction matrix
Choose ri and aij randomly from an exponential distribution:
P(a)
a00 5
1 P(a) = e-a
a = -LOG(RND)
mean = 1
Typical Time History
Time
xi
15 species
Coexistence Coexistence is unlikely unless the
species compete only weakly with one another.
Species may segregate spatially. Diversity in nature may result from
having so many species from which to choose.
There may be coexisting “niches” into which organisms evolve.
A Deterministic Chaotic Solution
27.153.172.01
ir
135.051.021.147.01033.236.144.010052.109.11
ija
Largest Lyapunov exponent: 1 0.0203
Time Series of Species
Strange Attractor
Attractor Dimension:DKY = 2.074
Route to Chaos
Homoclinic Orbit
Self-Organized Criticality
Extension to High Dimension(Many Species)
1 x 0 0x 1 x 0x x 1 xx 0 x 1
1 2
34
Future Work
1. Is chaos generic in high-
dimensional LV systems?
2. What kinds of behavior occur for
spatio-temporal LV competition
models?
3. Is self-organized criticality generic in
high-dimension LV systems?
Summary
Nature is complex
Simple models may suffice
but
References http://sprott.physics.wisc.edu/
lectures/lvmodel.ppt (This talk)
http://sprott.physics.wisc.edu/chaos/lvmodel/pla.doc (Preprint)