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A Steady State Analysis of a Rosenzweig-MacArthur Predator-Prey System
Caitlin Brown and Lianne Pinsky
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Overview We will examine this system of equations:
Without harvesting and stocking, this system has three steady states: a saddle, a saddle or stable node and a Hopf bifurcation between stable and unstable equilibria
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The Equations r = growth rate s = growth rate K = carrying capacity
A & B are related to predator-prey interaction G & H are stocking and harvesting terms
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Simplified equations We use the simplified equations:
by using the following substitutions:
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The Jacobian The Jacobian for this system is:
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First Steady State (x0, y0)=(0,0) The equilibrium is a saddle
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Second Steady State (x1, y1)=(1,0)
This equilibrium bifurcates between a stable node and a saddle
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Third Steady State This equilibrium is stable then bifurcates and is unstable
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The Hopf Bifurcation The Hopf Bifurcation occurs when the trace is 0
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Bifurcation Diagrams
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Phase Portrait:
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Phase Portrait:
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Phase Portrait:
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Phase Portrait:
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Conclusions This system has three steady states
One steady state is a saddle One steady state bifurcates between a stable node and a saddle One steady state has a Hopf Bifurcation between a stable and an unstable equilibrium
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