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A Primer in Bifurcation Theory for Computational Cell Biologists Lecture 4: Global Bifurcations
John J. Tyson Virginia Polytechnic Institute & Virginia Bioinformatics Institute Click on icon to start audio
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Signal-Response Curve = One-parameter Bifurcation Diagram
Saddle-Node (bistability, hysteresis) Hopf Bifurcation (oscillations) Subcritical Hopf Cyclic Fold Saddle-Loop Saddle-Node Invariant Circle
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Homoclinic Orbits Heteroclinic Orbits saddle-loop
saddle-saddle-connection saddle-node-loop
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Heteroclinic Orbits p = pHC p < pHC p > pHC
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Homoclinic Orbits p = pSL p < pSL p > pSL p = pSNIC p < pSNIC
Saddle- Loop Bifurcation p = pSL p < pSL p > pSL Saddle- Node Invariant Circle p = pSNIC p < pSNIC p > pSNIC
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Homoclinic Bifurcation
Hopf Bifurcation Small amplitude, frequency = Im(l), finite period Homoclinic Bifurcation Finite amplitude, small frequency, infinite period
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Andronov-Leontovich Theorem
In a two-dimensional system, a homoclinic orbit gives birth to a finite amplitude, large-period limit cycle; either stable: or unstable:
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Shil’nikov Theorem In a three-dimensional system, a homoclinic orbit gives birth to a stable or unstable limit cycle, or to much more complicated behavior … Saddle Saddle-Focus l3 < l2 < 0 < l Re(l2,3) < 0 < l1 s = l1+ l s = l1 + Re(l2,3) < 0: one stable limit cycle s < 0: one stable limit cycle > 0: one unstable limit cycle s > 0: infinite # unstable limit cycles plus a stable chaotic attractor
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One-parameter Bifurcation Diagram
SL HB sss uss HB SN Variable, x Parameter, p
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One-parameter Bifurcation Diagram
SL sss uss sss uss Variable, x sss SNIC Parameter, p
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References Strogatz, Nonlinear Dynamics and Chaos (Addison Wesley)
Kuznetsov, Elements of Applied Bifurcation Theory (Springer) XPP-AUT Oscill8
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