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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
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
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