Information Technology Reference
In-Depth Information
2
4
3
5
;
cos
u
z
ð
i
Þ
sin
u
z
ð
i
Þ
0
R
z
ðu
z
ð
i
ÞÞ
¼
sin
u
z
ð
i
Þ
cos
u
z
ð
i
Þ
0
ð
17
Þ
0
0
1
with the center of rotation at point cðiÞ
ð
i
Þ
¼
ð
c
x
ð
i
Þ;
c
y
ð
i
Þ;
c
z
ð
i
ÞÞ
. On the other hand, if
uð
i
Þ
¼
u
w
ð
i
Þ
(Eq.
14
), meaning that
the axial vertebral rotation is de
ned in
transverse planes of measurement that are orthogonal to the spine curve cðiÞ,
ð
i
Þ
, then
the modi
ed unit normal vector
n
u
ð
^
i
Þ
equals:
n
u
ð
ÞÞ
e
Iy
ð
i
Þ
¼
R
t
ð
i
Þ
ðu
w
ð
i
i
Þ;
ð
18
Þ
where e
Iy
ð
i
Þ
is the unit vector in the direction of the projection of e
Iy
¼½
0
;
1
;
0
I
to
the plane orthogonal to the spine curve (Eq.
14
), and matrix R
t
ð
i
Þ
ðu
w
ð
i
ÞÞ
represents
ned by the unit tangent vector t^ðiÞ:
the rotation for angle
u
w
ð
i
Þ
about the axis de
ð
i
Þ
:
R
t
ð
i
Þ
ðu
w
ð
i
ÞÞ
¼ cos
ðu
w
ð
i
ÞÞ
I
3
þ
ÞÞ
½t
ð
19
Þ
sin
ðu
w
ð
i
ð
i
Þ
ÞÞÞ
½t
Þ
t
þð
1
cos
ðu
w
ð
i
ð
i
ð
i
Þ;
with the center of rotation at point cðiÞ
ð
i
Þ
¼
ð
c
x
ð
i
Þ;
c
y
ð
i
Þ;
c
z
ð
i
ÞÞ
. In Eq.
19
, I
3
denotes
½t
ð
½t
ð
Þ
t
ð
the identity matrix of size 3
3, and
i
Þ
and
i
i
Þ
are, respectively, the
cross and tensor product matrix of t^ðiÞ:
ð
i
Þ
:
2
4
3
5
;
t
z
ð
t
y
ð
0
i
Þ
i
Þ
½t
t
z
ð
t
x
ð
ð
i
Þ
¼
i
Þ
0
i
Þ
ð
20
Þ
t
y
ð
t
x
ð
i
Þ
i
Þ
0
2
3
2
ð
t
x
ð
t
x
ð
Þ
t
y
ð
Þ
t
x
ð
Þ
t
z
ð
i
ÞÞ
i
i
i
i
Þ
4
5:
½t
Þ
t
2
ð
i
ð
i
Þ
¼
t
x
ð
Þ
t
y
ð
Þ
t
y
ð
t
y
ð
Þ
t
z
ð
ð
21
Þ
i
i
i
ÞÞ
i
i
Þ
2
t
x
ð
Þ
t
z
ð
Þ
t
y
ð
Þ
t
z
ð
Þ
t
z
ð
i
i
i
i
i
ÞÞ
In both cases, the unit binormal vector also changes its direction to
t the
orthonormal basis, and is therefore equal to b
u
ð
Þ
¼
t
ð
Þ
n
u
ð
Þ
. The resulting
axes u, v and w of the spine-based coordinate system are therefore represented by:
i
i
i
$
b
u
ð
u
:
^
e
Su
¼½
1
;
0
;
0
S
i
Þ;
ð
22
Þ
v
:
e
Sv
¼½
0
;
1
;
0
S
$
n
u
ð
i
Þ;
ð
23
Þ
$
t
w
:
^
e
Sw
¼½
0
;
0
;
1
S
ð
i
Þ:
ð
24
Þ