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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8.3 Using f2 as the bifurcation parameter 91<br />
NODf 2 -USB<br />
f2 ∈ (0;1.4 × 10 −1 ) (1.4 × 10 −1 ; 2.15) (2.15; 8.544) (8.544; 9.184) (9.184; 9.2205)<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 SS SS SP SP<br />
s )<br />
Dim(W<br />
5 5 5 3 3<br />
u ) 0 0 0 2 2<br />
Table 8.3 Gives an overview of the eigenvalues, and the behavior of the fixed points on the<br />
NODf2-USB. “S” stands <strong>for</strong> stable, “SS” stands <strong>for</strong> stable spiral, and “SP” stands <strong>for</strong> saddlepoint.<br />
Dim(W s ) is the dimension of the stable manifold, and Dim(W u ) is the dimension of<br />
the unstable manifold. All intervals are in the order of 10 −5 , and all values are approximate.<br />
Figure 8.14 The real (upper subplot) and imaginary (lower subplot) parts of the eigenvalues<br />
of the fixed point along the NODf2-LUB.<br />
features similar to the NODf1-LUB. The behavior of the eigenvalues is less erratic <strong>for</strong><br />
the eigenvalues along the NODf2-LUB, than along the NODf2-USB, as we see when we<br />
compare table 8.4 to table 8.3. The bifurcation diagram <strong>for</strong> f2 with Balb/c parameters<br />
is given in figure 8.15. We clearly see that <strong>for</strong> the value of f2 that Balb/c-mice have<br />
inflammation is non-persistent, in agreement with what we would expect. The way the<br />
concentration of active macrophages decreases along the Balb/cf2-USB makes it look<br />
similar to figure 8.12, but we see that the shift between a stable and an unstable USB<br />
comes at a much lower f2-value when we use the Balb/c-value <strong>for</strong> f1.<br />
As we did in the case of the NOD-mice we have also searched <strong>for</strong> additional fixed