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The derivative of V along the solutions of system (8.6) is
H )+ 1
H ) T ˙
k A tr( A T ˙
V =
A )
tr(( I
1
H A
k A tr( A T
H ) T
H ) T
H Ad H 1 α
=
tr(( I
( I
)
β
)
.
(3),tr( B T G )=tr( B T
sl
Knowing that for any matrices G
SL (3) and B
P
( G )) =
, P
B
( G )
, one obtains:
1
k A β .
V =
( H T ( I
H ))
α A
( H T ( I
H )) +
P
,
Ad H 1
, P
Introducing the expressions of
α
and
β
(8.7) in the above equation yields
V =
( H T ( I
H ))
2
k H || P
||
.
(8.9)
The derivative of the Lyapunov function is negative semidefinite, and equal to zero
when
( H T ( I
H )) = 0. The dynamics of the estimation error is autonomous, i.e.
P
it is given by
H = H A + k H
H ))
˙
( H T ( I
P
(8.10)
˙
A = k A
( H T ( I
H ))
P
.
Therefore, we deduce from LaSalle theorem that all solutions of this system con-
verge to the largest invariant set contained in
( H
, A )
( H T ( I
H )) = 0
.
We now prove that, for system (8.10), the largest invariant set E contained in
{
| P
}
( H
, A )
( H T ( I
H )) = 0
{
| P
}
is equal to E s
E u . We need to show that the solutions
( H
, A )
( H T ( I
H )) = 0
of system (8.10) belonging to
{
| P
}
for all t consist of all fixed
points of E s
E u . Note that E s =( I
,
0) is clearly contained in E . Let us thus consider
˙
such a solution ( H ( t )
, A ( t )). First, we deduce from (8.10) that
A ( t ) is identically zero
H ( t ))) is identically zero on the invariant set E and therefore A
is constant. We also deduce from (8.10) that H is solution to the equation
( H T ( t )( I
since
P
˙
H = H A .
Note that at this point one cannot infer that H is constant. Still, we omit from now
on the possible time-dependence of H to lighten the notation.
Since
( H T ( I
H )) = 0, we have that
P
H )= 1
H ( I
3 trace( H ( I
H )) I
(8.11)
which means that H is a symmetric matrix. Therefore, it can be decomposed as:
H = UDU
(8.12)
where U
SL (3) is a diagonal matrix which con-
tains the three real eigenvalues of H . Without loss of generality let us suppose that
the eigenvalues are in increasing order:
SO (3) and D = diag(
λ 1 , λ 2 , λ 3 )
λ 1 λ 2 λ 3 .
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