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is
d
1
(
i
)
p
1
(
i
)
2
q
1
N
+
d
2
(
i
)
p
2
(
i
)
2
q
2
min
(2.15)
i
=1
s.t.
p
1
(
i
)+
p
2
(
i
)=1
,
p
1
(
i
)
,p
2
(
i
)
≥
0
,i
=1
,
···
,N ,
where
p
1
(
i
)
,p
2
(
i
) are the cluster probabilities at
x
i
and
d
1
(
i
)
,d
2
(
i
) are the cor-
responding distances. The problem separates into
N
problems like (2.12), and its
optimal value is
N
d
1
(
i
)
d
2
(
i
)
/q
1
q
2
d
1
(
i
)
/q
1
+
d
2
(
i
)
/q
2
(2.16)
i
=1
the sum of the joint distance functions of all points.
2.2.4.
An Extremal Principle for the Cluster Sizes
Taking the cluster sizes as variables in the extremal principle (2.15),
d
1
(
i
)
p
1
(
i
)
2
q
1
N
+
d
2
(
i
)
p
2
(
i
)
2
q
2
min
(2.17)
i
=1
s.t.
q
1
+
q
2
=
N
q
1
,q
2
≥
0
with
p
1
(
i
)
,p
2
(
i
) assumed known, we have the Lagrangian
d
1
(
i
)
p
1
(
i
)
2
q
1
+
λ
(
q
1
+
q
2
−
N
+
d
2
(
i
)
p
2
(
i
)
2
q
2
L
(
q
1
,q
2
,λ
)=
N
) (2.18)
i
=1
Zeroing the partials
∂L/∂q
k
gives,
N
d
k
(
i
)
p
k
(
i
)
2
,k
=1
,
2
,
q
k
=
1
λ
(2.19)
i
=1
and since
q
1
+
q
2
=
N
,
N
d
k
(
i
)
p
k
(
i
)
2
1
/
2
i
=1
q
k
N
=
i
=1
d
2
(
i
)
p
2
(
i
)
2
1
/
2
,k
=1
,
2
.
(2.20)
N
i
=1
d
1
(
i
)
p
1
(
i
)
2
1
/
2
+
N
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