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nr. 477 - 2011 - Institut for Natur, Systemer og Modeller (NSM)

nr. 477 - 2011 - Institut for Natur, Systemer og Modeller (NSM)

nr. 477 - 2011 - Institut for Natur, Systemer og Modeller (NSM)

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86 Bifurcation Diagrams and Analysis<br />

Flow tends to the<br />

USB <strong>for</strong> all initial<br />

values in this area<br />

Line of unstable fixed points. The<br />

flow tends to the HRS <strong>for</strong> all initial<br />

values above this.<br />

Flow tends to the<br />

USB <strong>for</strong> all initial<br />

values in this area<br />

Hopf bifurcation pt.<br />

Flow tends to<br />

the HRS <strong>for</strong> all<br />

initial values in<br />

this area<br />

Figure 8.9 Shows a modified version of figure 8.1, where we have added a curve that<br />

approximates the UUB. We have also added legends to facilitate the overview.<br />

a curve that approximates the UUB. 12 We have also added text to explain how the<br />

flow behaves <strong>for</strong> different initial Ma-concentrations. We see that the UUB and the<br />

NODf1-USB ultimately coincide. This appears in the eigenvalues of the NODf1-USB approximately with the advent of positive eigenvalues. We dare not state that it is<br />

exactly when the eigenvalues become positive. If the UUB is in fact a line of unstable<br />

fixed points then the collision between the NODf1-USB and the UUB is basically a<br />

(presumably degenerate) sub-critical pitch<strong>for</strong>k bifurcation – an unstable and a stable<br />

fixed point coalesce to produce one unstable fixed point.<br />

We have speculated if the UUB constitutes a section of the unstable limit cycle that<br />

12 Notice that though we used matlab to approximate the demarcation values, the UUB-curve shown<br />

in figure 8.9 is not made with matlab it was drawn using Adobe Illustrator CS3.

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