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17.3.4.2
Correction of Nonholonomic Deviation
In order to make u i +1 ( s
, τ
)
,···,
u n ( s
, τ
) tend toward 0 as
τ
increases, we apply the
following linear control:
i
∈{
k + 1
,···,
n
},∀
s
[0
,
S ] ,
v i ( s
, τ
)=
α
u i ( s
, τ
)
where
α
is a positive constraint. We denote by
η 1 the corresponding direction of
deformation for
τ
=
τ j :
j )= A ( s
η 1 ( s
j )+ B ( s
j ) v ( s
, τ
, τ
, τ
, τ
, τ
j )
η
1 ( s
j )
(17.24)
, τ
.
η
1 (0
j )=0
(17.25)
17.3.4.3
Deformation due to Obstacles
Following the procedure described in sections 17.3.1 and 17.3.3, we restrict input
functions ( v 1 ,···,
v k ) to the finite dimensional subspace of functions spanned by
( e 1 ,···,
λ 1 ,···, λ p ) according to (17.19). We denote by
η 2 the direction of deformation obtained with these coefficients:
e p ) and we compute
λ
=(
p
i =1 λ i E i ( s , τ j )
η 2 ( s
, τ j )=
where the E i are now solution of system:
E i ( s
, τ j )= A ( s
, τ j ) E i ( s
, τ j )+ B ( s
, τ j ) e ( s )
(17.26)
, τ
.
E i (0
j )=0
(17.27)
17.3.4.4
Boundary Conditions
We wish the sum of
2 satisfies boundary conditions (17.13) and (17.14).
Again, (17.13) is trivially satisfied. (17.14) is an affine constraint over vector
η
1 and
η
λ
:
η 2 ( S
, τ j )= L
λ
=
η 1 ( S
, τ j )
(17.28)
where L is the matrix defined in Section 17.3.2. Following the same idea as in Sec-
tion 17.3.2, we project vector
λ
over the affine subspace satisfying (17.28):
¯
P ( LP ) +
P ( LP ) + L )
λ
=
η 1 ( S
, τ j )+( I p
λ .
We then get a direction of deformation satisfying the boundary conditions and mak-
ing the component of the velocity along additional vector fields converge toward 0:
p
i =1 λ i E i ( s , τ j )+η 1 ( s , τ j ) .
, τ
η
( s
j )=
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