Chemistry Reference
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x ( T,x 0 , u 1 )
x ( T,x 0 , u 2 )
Figure 2. Schematic representation
of the accessibility set A ( x 0 ,T ) in gray.
The control fields u 1 and u 2 are respec-
tively singular, and regular.
x 0
Let x 1 =
x ( T ) be a point reached in time T from x 0 by a regular trajectory. Then
the accessibility set A ( x 0 ,T ) is a neighborhood of the point x 1 , which implies
that the system is locally controllable around x 1 .If x ( T )
∂A ( x 0 ,T ) (i.e., the
boundary of A ), then u is said to be singular on [0 ,T ]. This case is schematically
illustrated in Fig. 2 for a regular and singular control field. The most interesting
case is therefore the singular one and this case can be viewed as a first step to-
ward the maximum principle. Indeed, a key observation for this principle is that
if the trajectory ( x, u ) is optimal, then the point x ( T, x 0 ,u ) must belong to the
boundary of the accessibility set. This assertion can be understood in the time-
minimal case, where the goal is to reach the target state x 1 in minimum time.
It is clear that if x 1 =
x ( x 0 ,T,u ) belongs to the interior of A ( x 0 ,T ), then one
can find a smaller time T <T and a point x ( x 0 ,T ,u )of ∂A ( x 0 ,T ), such that
x 1 =
x ( x 0 ,T ,u ) (one can draw the accessibility set at different times to be con-
vinced of this point). This result finally implies that u is not optimal for this control
problem.
Computation of Singular Controls
We assume that Im E
n and the corresponding control u is singular.
= R
/
n
Theorem 1
If u is singular, then there exists p ( t )
∈ R
\{
0
}
, such that if
H ( x, p, u )
=
p
·
F ( x, u ) , the triplet ( x, p, u ) satisfies almost everywhere
∂H
∂p
x
=
∂H
∂x
(2)
p
=−
∂H
∂u
=
0
 
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