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Mini-course bifurcation theory. Part three: bifurcations of 2D systems. George van Voorn. Bifurcations. Bifurcations of equilibria in 1D Transcritical ( λ = 0) Tangent ( λ = 0) In 2D Transcritical (One λ = 0) Tangent (One λ = 0). Example. 2D ODE Rosenzweig-MacArthur (1963).
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Mini-course bifurcation theory Part three: bifurcations of 2D systems George van Voorn
Bifurcations • Bifurcations of equilibria in 1D • Transcritical (λ = 0) • Tangent (λ = 0) • In 2D • Transcritical (One λ = 0) • Tangent (One λ = 0)
Example • 2D ODE Rosenzweig-MacArthur (1963) R = intrinsic growth rate K = carrying capacity A/B = searching and handling C = yield D = death rate
Example • At K = 0 x = 0, y = 0 • 0 < K < 6 x > 0, y = 0 • At K = 6 x = K, y = 0 • 6 < K < ? x = K, y > 0 • K = 0 and K = 6 transcritical • Invasion criterion species x,y
Hopf bifurcation • Andronov-Hopf bifurcation: • Transition from stable spiral to unstable spiral (equilibrium becomes unstable) • Or vice versa • Periodic orbit (limit cycle), stable • Or vice verse, respectively • Conditions:
x,y α Hopf bifurcation
Example • At K≈ 20 x = K, y > 0 • Limit cycle • Change in dynamics of species x,y
Paradox of enrichment • Isoclines RM model x = K, for all K > 6 increase only in y
Paradox of enrichment One-parameter bifurcation diagram
Paradox of enrichment Maximal values x and y Minimal values x and y Equilibria One-parameter bifurcation diagram
Paradox of enrichment Oscillations increase in size for larger K
Paradox of enrichment • Large oscillations extinction probabilities • Paradox: • Increase in food availability K • No benefit for prey x • Increased probability of extinction system
Limit cycle bifurcations • For limit cycles same bifurcations as for equilibria • Imagine cross section
Limit cycle bifurcations • Transcritical Cycle on axis (mostly) • Tangent Birth or destruction cycle(s)
Limit cycle bifurcations • Hopf (called Neimark-Sacker) Torus
Limit cycle bifurcations • Flip bifurcation • Manifold around cycle
Flip bifurcations • Manifold twisted
Flip bifurcations • Flip bifurcation of limit cycle • Manifold twisted (Möbius ribbon) • Period doubling
Codim 2 points • Bifurcation points can be continued in two-parameter space = bifurcation curve • Continuation can result in: • Bifurcation points of higher co-dimension
Codim 2 points • Bogdanov-Takens • Cusp • Generalised Hopf (Bautin)
Example • Bazykin model • Calculate equilibrium • Vary one parameter until a bifurcation is encountered
Bazykin x*,y* Continuation in two-parameter space
Bazykin: dynamics Stable node: coexistence No positive equilibria: extinction Stable cycle: coexistence Unstable equilibria: extinction
Bazykin: BT point Bogdanov-Takens point tangent & Hopf
Bazykin: GH point Bautin point transition Hopf from stable to unstable point
Bazykin: cusp point Cusp point collision two tangent points
Question What happens here? Stable cycle: coexistence Unstable equilibria: extinction
Global bifurcations • BT point: origin of homoclinic bifurcation
Bazykin: homoclinic Starting at Hopf continue cycle. What happens?
Bazykin: homoclinic Limit cycle period to infinity. Why?
Homoclinic connection Wu Ws Homoclinic connecting orbit: Wu = Ws Time to infinity near equilibrium
Heteroclinic connection Ŵs Wu Heteroclinic connecting orbit: Wu = Ŵs