Biomedical Engineering Reference
In-Depth Information
models include Gradient, Balloon [44], the Distance Map [63], and Gradient Vector
Flow (GVF) [46]. The goal of modeling an external force is to find one kind of
force that has the capability of pushing the curve to significant concavities or
convexes, retaining a large capture range, stopping the evolving curve at the edge
gaps, and processing high-noise images. For our purposes, we will now give a
brief overview of the classic snake model and the GVF snake model.
2.1.1. Classic snake model
x ( s )=( x ( s ) ,y ( s )),
where s is the arc length, and x ( s ) and y ( s ) are x and y coordinates along the
contour, and the energy of the model is given by
Geometrically, a classic snake model is described by
E snake =
E ( x ( s )) ds =
E int ( x ( s )) + E ext ( x ( s )) ds,
(1)
snake
snake
where E ext is the external energy, and E int is the internal energy, given by
α ( t )
2 ,
2
2 x ( s )
∂s 2
E int = 1
2
x ( s )
∂s
+ β ( t )
(2)
where α and β are the coefficients that control the snake's tension and rigidity,
respectively. The goal is to find a snake,
x ( s ), that minimizes E snake . The external
energy is in accord with the image features, and for a given image f ( x, y ),
γ
G σ ( x,y )
f ( x, y ) ,
E ext =
(3)
where G σ ( x,y )
is the two-dimensional Gaussian kernel with σ as the standard
deviation.
Solved by the variational method, the minimum of E snake
has to satisfy the
following Euler-Lagrange equation:
x ( s )+ β
x ( s )+
α
E ext =0 .
(4)
Discretization of Eq.
(4) by the finite-difference method yields a linear system
[43]:
AP = L
,
(5)
where
denote the
discrete contour points vector and the forces at these points, respectively. From
the initial position of the contour, the following associated evolution equation can
be solved:
A
is a pentadiagonal matrix depending on α and β , and
P
and
L
= P
L P
t− 1 ,
t
t− 1 + τ
( I + τ
A ) P
(6)
x ( s ), can be achieved
where t is time, and τ is the time step. The final solution,
by solving Eq. (6) iteratively.
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