178 Chapter 9 The M athematics of Rotations
which we can verify with the matrix multiplication,
⎡
⎢
⎣
abc
def
ghi
⎤
⎥
⎦
⎡
⎢
⎣
1
0
0
⎤
⎥
⎦
=
⎡
⎢
⎣
a ×1 +b × 0 + c × 0
d ×1 +e × 0 +f × 0
g × 1 +h ×0 + i ×0
⎤
⎥
⎦
=
⎡
⎢
⎣
a
d
g
⎤
⎥
⎦
and so on for the other two axes. When I introduced vectors , I mentioned that their
three components could be thought of as a position along three axes. The x compo-
nent is the distance along the X axis and so on. We could write the vector as
v =
⎡
⎢
⎣
x
y
z
⎤
⎥
⎦
=x
⎡
⎢
⎣
1
0
0
⎤
⎥
⎦
+y
⎡
⎢
⎣
0
1
0
⎤
⎥
⎦
+z
⎡
⎢
⎣
0
0
1
⎤
⎥
⎦
In other words, a vector is made up of some proportion of each basic axis.
If the three ax es move under a transformation, then the new location o f the vector
will be determined in the same way as before. The axes will have moved but the new
vector will still combine them