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From Eq. ( 8.14 ) it can be seen that g.x i
x j / Dg.x j
x i /, i.e. g./ is an odd
function. Therefore, it holds that
0
1
M
X
1
M
@
A D 0
g.x i
x j /
(8.21)
jD1;j¤i
X
M
1
M
x D
Œr x i V i .x i /
(8.22)
iD1
Denoting the goal position by x , and the distance between the i-th particle and
the mean position of the multi-particle system by e i .t/ D x i .t/ x the objective
of the learning algorithm for can be summarized as follows: (i) lim t!1 x D x ,
i.e. the center of the multi-particle system converges to the goal position, (ii)
lim t!1 x i
Dx, i.e. the i-th particle converges to the center of the multi-particle
system, (iii) lim t!1 x D 0, i.e. the center of the multi-particle system stabilizes at
the goal position. If conditions (i) and (ii) hold then, lim t!1 x i
D x . Furthermore,
if condition (iii) also holds, then all particle will stabilize close to the goal position
[ 64 , 108 , 150 , 152 ].
To prove the stability of the multi-particle system the following simple Lyapunov
function is considered for each particle:
1
1
2 jje i jj
2 e i T e i
2
V i D
) V i D
(8.23)
Thus, one gets
D e i T
V i
) V i
x/e i
e i
D .x i
)
h
M P jD1 r x j V j .x j / i e i :
r x i V i .x i / P jD1;j¤i g.x i
V i
x j / C
1
D
Substituting g.x i
x j / from Eq. ( 8.14 ) yields
2
M
X
V i D
4 r x i V i .x i /
.x i
x j /a
jD1;j¤i
3
M
M
X
X
jD1 r x j V j .x j /
1
M
5 e i
.x i
x j /g r .jjx i
x j
C
jj/ C
jD1;j¤i
which gives
 
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