Hence for a constant value v 2 [0;a]; and for q = 0;
bpq = f
v(p) = 2 : (3.30) + Gv + dp
3
The family of functions fv are all stricly increasing (see Figure 3.1) and bounded by fv(0) = 0
and fv(peq)(upper bound)
3b(b
2f d )
v(peq) = 3 2 (3.31) + Gv + d((b
d )2)3
3 1 )
2
= b d (b 2)Gv + + (b (3.3)
3 b 1
2
= (b ) (3.33)b + Gv d
b= p
b + Gv eq: (3.34)
On the following boundary segment, Q = f(p;q) : 0 < p < peq;q = qeqg;
bpq =
2
2q
eq Gu + + dp3 < 0: (3.35) + dp
3 + Gu
The point (peq;qeq) is the equilibrium point for u = 0 and (p;q) 2 D: Hence, regardless of
the values taken by the control u, the trajectory always remains within the boundary of D.
However for the control taking constant value u = a, the equilibrium becomes:
3 b Ga
2
peq = qeq = : (3.36)d
When b Ga; the system no longer has an equilibrium point and now all the trajectories
converge to the origin as t goes to in
nity. This is a desired situation which means that
theoretically (i.e. given in
nite amount of time and inhibitors), we could eradicate the
13
Page 1 |
Page 2 |
Page 3 |
Page 4 |
Page 5 |
Page 6 |
Page 7 |
Page 8 |
Page 9 |
Page 10 |
Page 11 |
Page 12 |
Page 13 |
Page 14 |
Page 15 |
Page 16 |
Page 17 |
Page 18 |
Page 19 |
Page 20 |
Page 21 |
Page 22 |
Page 23 |
Page 24 |
Page 25 |
Page 26 |
Page 27 |
Page 28 |
Page 29 |
Page 30 |
Page 31 |
Page 32 |
Page 33 |
Page 34 |
Page 35 |
Page 36 |
Page 37 |
Page 38 |
Page 39 |
Page 40 |
Page 41 |
Page 42 |
Page 43 |
Page 44 |
Page 45 |
Page 46 |
Page 47 |
Page 48 |
Page 49 |
Page 50 |
Page 51 |
Page 52 |
Page 53 |
Page 54 |
Page 55 |
Page 56