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Y c
Z
Y
c
Y p
X p
C
θ p
Y
b
a
M
D x
P
y
θ
X
M
M
X
x
O
Fig. 15.2 Camera fixed on a pan-platform supported by a wheeled robot
which constitutes the actual system input is described by the vector q = v 1 v 2 v 3 ,
where v 1 and v 2 are the linear and the angular velocities of the cart with respect to R ,
respectively, while v 3 is the pan-platform angular velocity with respect to the robot
main axis X M . The system kinematics is
x
y
˙
cos
θ
00
v 1
v 2
v 3
sin
00
010
001
θ
.
=
˙
θ p
The kinematic screw of the camera T is linked to the velocity vector q by the relation
T = J ( q ) q ,where J ( q ) is the robot Jacobian given by
sin
θ p D x cos
θ p + aa
.
J ( q )=
cos
θ p
D x sin
θ p
b
b
(15.46)
0
1
1
As shown in [18], the rotational degree of freedom of the pan-platform allows to
overcome the nonholonomic constraint of the wheeled base.
15.5.0.1
Application 1
In the first application, the robot has to track a moving target and stabilize its cam-
era in front of it when it stops. The initial robot configuration is xy
θθ p =
4
175 rad , and the initial value of the state vector is
.
85 m
0
.
8 m 0 rad 0
.
ξ
(0)=
0849 m 0 ms 1 0 ms 1 0 rads 1 . At the beginning of the
task, the coordinates of the three target points, with respect to R ,are: E 1 10 m 0
0
.
12 m
0
.
0159 m 0
.
5 m ,
.
E 2 10 m 0 m and E 3 10 m
5 m . According to condition C4, the target veloc-
ity is supposed to be unknown but square integrable, and its bound is defined by
taking
0
.
δ 1 = 12
.
1949 in (15.11). The interval of distance between the robot and the
 
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