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(ii) If
N
D
8;
then it is globally asymptotically stable if and only if
LT
ยค
1;
where
L
D
a=.N
C
1/;
(iii) If
N
9;
then the steady state is globally asymptotically stable if and only
if either
LT < .LT/
1
or
LT > .LT/
2
;
where
.LT/
1
and
.LT/
2
are given
by (5.134). At these critical values Hopf bifurcations occur giving rise to the
possibility of the birth of limit cycles.
Proof.
Let T>0and m
D
0. Then (5.130) becomes the quadratic equation
C
T
C
2
T.N
C
1/
a
N
C
1
a
C
.N
C
1/
D
0:
Since all coefficients are positive, all roots have negative real parts (see Lemma F.2
in Appendix F) implying global asymptotic stability.
Consider next the case of T>0and m
D
1. Then (5.130) becomes a cubic
equation, and with the notation L
D
a=.N
C
1/ it has the form
.
C
L/.1
C
2T
C
2
T
2
/
C
NL
D
0;
that is,
T
2
3
C
2
.2T
C
LT
2
/
C
.1
C
2LT/
C
L.N
C
1/
D
0:
(5.131)
Since all coefficients are positive, the Routh-Hurwitz stability condition implies that
all eigenvalues have negative real parts if and only if
.2T
C
LT
2
/.1
C
2LT/ > T
2
L.N
C
1/;
(5.132)
which can be rewritten as a quadratic inequality in LT , namely
2.LT/
2
C
.LT/.4
N/
C
2>0:
(5.133)
The discriminant of the left hand side is
.4
N/
2
16
D
N.N
8/:
Depending on the number of roots of the left hand side of (5.133) we have to
consider the following cases.
Case 1. If N<8, then the discriminant is negative, so (5.133) always holds and
the steady state is always globally asymptotically stable.
Case 2. If N
D
8, then there is a unique real root
N
4
4
D
1;
LT
D
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