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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