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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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