Biomedical Engineering Reference
In-Depth Information
18000
S
16000
u=0
14000
u=a
12000
full dosage
10000
beginning of therapy
8000
partial dosages along singular arc
x *
6000
endpoint − (q(T),p(T))
4000
no dose
2000
0
0
2000
4000
6000
8000
10000
12000
14000
16000
18000
carrying capacity of the vasculature, q
Fig. 1
A 2-dimensional projection of the optimal synthesis for the monotherapy model [A] into
(
p
,
q
)
-space
optimal solution, no minimization algorithm needs to be invoked, but the procedure
simply consists in evaluating a piecewise defined, albeit somewhat complicated
function.
We briefly describe the structure of optimal controlled trajectories. First of
all, note that we plot the tumor-volume p vertically and the carrying capacity q
horizontally in Fig. 1 . This simply better visualizes a decrease or increase in the
primary cancer volume. The anchor piece of the synthesis is an optimal singular
arc
-space along which
the best tumor reductions occur and optimal controls follow this curve whenever
the data allow. That is, if
S
shown in blue. This is a unique curve defined in
(
p
,
q
)
, and if angiogenic inhibitors
y are still available, then the optimal control consists in giving a specific time-
varying dosage that makes the system stay on this curve, i.e., makes the singular
arc invariant. There is a unique control that has this property, the corresponding
singular control, and as long as its values lie in the admissible range
(
p
,
q
)
happens to lie on
S
,thisis
the optimal control. For the model by Hahnfeldt et al., there is a unique point on the
singular arc when the control reaches its saturation limit u max which is denoted by
x u in Fig. 1 . Mathematically, the structure of the optimal synthesis near a saturating
singular arc is well understood [ 26 , 55 ], but for simplicity of presentation we limit
our discussions here to cases when saturation does not occur. In this case, once
(
[
0
,
u max ]
, the optimal protocol then simply consists in giving these singular
dosages until all inhibitors are exhausted. At that time, the state of the system lies
in the region
p
,
q
)
lies on
S
and, because of aftereffects, the tumor volume
will still be decreasing until it reaches the diagonal
D + = { (
p
,
q
)
: p
>
q
}
of the
system. This behavior is preprogrammed in the properties of the Gompertz growth
D 0 = { (
p
,
q
)
: p
=
q
}
 
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