Biomedical Engineering Reference
In-Depth Information
The transformation matrix is indeed a partitioned matrix where the upper left
corner sub-matrix is the rotation matrix and the upper right vector is the position
vector
rotation
position
⎡
⎤
⎢
⎥
A
T
B
=
(2.9)
ma
trix
ve
c
tor
⎢
⎥
0
1
⎣
⎦
2.4
Basic transformations
Figure 2.6
shows two coordinate systems
x
1
y
1
z
1
and
x
2
y
2
z
2
that are coincident.
Consider the matrix generated by the rotation of the coordinates system
x
2
y
2
z
2
about the
z
1
axis.
By definition, this rotation can be written as the dot product of unit vectors as
2
4
3
5
x
1
U
x
2
x
1
U
y
2
x
1
U
z
2
R
z;θ
5
y
1
Ux
2
y
1
Uy
2
y
1
Uz
2
(2.10)
z
1
Ux
2
z
1
Uy
2
z
1
Uz
2
where the subscripts
z
and
θ
denote a rotation about
z
with an angle
θ
. From
Figure 2.6(B)
, carrying out the dot product yields
2
4
3
5
cos
θ
cos
ð
90
1
θÞ
0
R
z;θ
5
cos
ð
90
2
θÞ
cos
θ
0
(2.11)
0
0
1
Further simplification using the identity cos(90
1
θ
)
sin
θ
and cos(90
2
θ
)
52
5
sin
θ
yields the basic rotation matrix
2
4
3
5
cos
θ
2
sin
θ
0
R
z;θ
5
sin
θ
cos
θ
0
(2.12)
0
0
1
z
1
z
1
z
1
z
2
y
2
z
2
z
2
y
1
y
1
y
1
y
2
y
2
c
x
2
a
x
2
b
θ
x
2
x
1
x
1
x
1
(A)
(B)
(C)
FIGURE 2.6
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