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Resting Stages and the Population Dynamics of Harmful Algae in ...

Resting Stages and the Population Dynamics of Harmful Algae in ...

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So if we are <strong>in</strong> Case 1 <strong>of</strong> feasibility <strong>the</strong>n Condition (12) is met which impliesCondition (19) is also met. Therefore <strong>in</strong> Case 1 <strong>the</strong> determ<strong>in</strong>ant <strong>of</strong> <strong>the</strong> Jacobianmatrix (18) must be positive. The trace <strong>of</strong> <strong>the</strong> Jacobian matrix (18) is−2D−δ + R <strong>in</strong>µ maxK +R <strong>in</strong>−γ.Thus <strong>the</strong> condition for <strong>the</strong> trace to be negative is2D+δ +γ > R <strong>in</strong>µ maxK +R <strong>in</strong>. (20)Us<strong>in</strong>g <strong>the</strong> fact thatD(D+δ +γ)2D+δ +γ > ,(D +γ)Condition (11), <strong>and</strong> <strong>the</strong> transitivity property we know that if we are <strong>in</strong> Case1 <strong>the</strong>n Condition (20) has been met. Therefore we can say that <strong>in</strong> Case 1 <strong>of</strong>feasibility <strong>the</strong> trace <strong>of</strong> <strong>the</strong> Jacobian matrix (18) is negative. Fur<strong>the</strong>rmore wecan say that Ec 0 is stable <strong>in</strong> Case 1.The Jacobianmatrix (17) is evaluated at Ec ∗ for <strong>the</strong> chemostat model. Aga<strong>in</strong>we want to f<strong>in</strong>d conditions for a positive determ<strong>in</strong>ant <strong>and</strong> a negative trace. Thecondition for a positive determ<strong>in</strong>ant isD(D +γ) . (23)K +R <strong>in</strong> D+γSo for Case 1 <strong>of</strong> feasibility <strong>the</strong> equilibrium Ec ∗ is unstable, because Condition(11) is directly contradicted by Condition (23), mean<strong>in</strong>g that <strong>the</strong> determ<strong>in</strong>ant isnotpositive <strong>and</strong><strong>the</strong> traceis notnegative. In Case1<strong>of</strong>feasibility <strong>the</strong> equilibriumEc 0 is stable <strong>and</strong> <strong>the</strong> equilibrium E∗ c is unstable. This is shown <strong>in</strong> Figure 2.10

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