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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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80 Bifurcation Diagrams and Analysis<br />

NODf 1 -USB<br />

f1 ∈ (0;3.4 × 10 −2 ) (3.4 × 10 −2 ; 2.15) (2.15; 2.57) (2.57; 2.8) (2.8; 3.45)<br />

Nr. λ ∈ R +<br />

0 0 0 0 2<br />

Nr. λ ∈ R −<br />

5 3 1 1 1<br />

Nr. λ ∈ C(Re(λ)) 0 2(-) 4(-) 2(-),2(+) 2(-)<br />

Fixed pt.<br />

Dim(W<br />

S S SS USS SP<br />

s )<br />

Dim(W<br />

5 5 5 3 3<br />

u ) 0 0 0 2 2<br />

Table 8.1 Gives an overview of the eigenvalues, and the behavior of the fixed points on the<br />

NODf1-USB. By C(Re(λ)) we mean the sign of the real part of the complex eigenvalues. “S”<br />

stands <strong>for</strong> stable, “SS” stands <strong>for</strong> stable spiral, “USS” stands <strong>for</strong> unstable spiral, and “SP”<br />

stands <strong>for</strong> saddle-point. Dim(W s ) is the dimension of the stable manifold, and Dim(W u ) is<br />

the dimension of the unstable manifold. All intervals are in the order of 10 −5 , and all values<br />

are approximate.<br />

Figure 8.5 In the upper figure we see (real) values of the eigenvalues of the NODf1-LUB.<br />

At f1 ≈ 1.165 × 10 −5 two of the eigenvalues become complex, and stay complex up until<br />

f1 = 3.45 × 10 −5 where the NODf1-LUB coalesces with the NODf1-USB (that consists of<br />

saddle-points at this point); cf. figure 8.1. The values of the complex part of these two<br />

eigenvalues are plotted in the lower figure. The complex eigenvalues retain negative real parts<br />

through the entire interval.

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