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optical flow velocity and applicate of a gaussian filter (Figure 3). The values of
c
1
and
c
2
are re-estimated during the spread of the curve. The method of levels sets
is used directly representing the curve
Γ
(
x
) as the curve of zero to a continuous
function U(x). Regions and contour are expressed as follows:
Γ
=
∂Ω
in
=
{
x
∈
Ω
I
/U
(
x
)=0
}
Ω
in
=
{
x
∈
Ω
I
/U
(
x
)
<
0
}
(4)
Ω
out
=
{
x
∈
Ω
I
/U
(
x
)
>
0
}
The unknown sought minimizing the criterion becomes the function U. We in-
troduce also the Heaviside function H and the measure of Dirac
δ
0
defined by:
1
if z
0
0
if z >
0
≤
et ∂
0
(
z
)=
dz
H
(
z
)
H
(
z
)=
(a)
(b)
(c)
Fig. 3.
SV
g
Image example
The criterion is then expressed through the functions U, H and
δ
in the following
manner:
J
(
U, c
1
,c
2
)=
Ω
I
λ
2
H
(
U
(
x
))
dx
+
|
SV
g
(
x
)
−
c
1
|
Ω
I
λ
2
(1
(5)
|
SV
g
(
x
)
−
c
2
|
−
H
(
U
(
x
)))
dx
+
Ω
I
μδ
(
U
(
x
))
|∇
U
(
x
)
|
dx
with:
Ω
SV
g
(
x
)
H
(
U
(
x
))
dx
c
1
=
Ω
H
(
U
(
x
))
dx
Ω
SV
g
(
x
)(1
−H
(
U
(
x
)))
dx
Ω
(1
−H
(
U
(
x
)))
dx
(6)
c
2
=
To calculate the Euler-Lagrange equation for unknown function U, we consider
a regularized versions for the functions H and
δ
noted
H
and
δ
. The evolution
equation is found then expressed directly with U, the function of the level set:
2
∂U
∂τ
=
δ
(
U
)[
μdiv
(
∇U
|∇
)+
λ
|
SV
g
(
x
)
−
c
1
|
U
|
2
](
inΩ
I
)
−
λ
|
SV
g
(
x
)
−
c
2
|
(7)
δ
(
U
)
|∇U |
∂U
∂N
=0(
on∂Ω
I
)
with
div
(
∇U
|∇U|
∂U
∂N
) the curvature of the level curve of U via x and
the derivative
of U compared to normal inside the curve N.
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