Graphics Reference
In-Depth Information
6.5 Inner and Outer Products
Let's assume that the products ij and ji in ( 6.1 ) anticommute: ji
=−
ij . Therefore,
a 1 b 1 i 2
a 2 b 2 j 2
ab
=
+
+
(a 1 b 2
a 2 b 1 ) ij
(6.2)
and if we reverse the product to ba we obtain
a 1 b 1 i 2
a 2 b 2 j 2
a 2 b 1 ) ij . (6.3)
From ( 6.2 ) and ( 6.3 ) we see that the product of two vectors contains a symmetric
component
ba
=
+
(a 1 b 2
a 1 b 1 i 2
+ a 2 b 2 j 2
and an antisymmetric component
a 2 b 1 ) ij .
Geometric algebra defines the product ab as the sum of two other products called
the inner and outer products. The inner product has the form
(a 1 b 2
·
=|
||
|
a
b
a
b
cos β
(6.4)
where
a
·
b
= (a 1 i
+ a 2 j ) · (b 1 i
+ b 2 j )
= a 1 b 1 i
·
i
+ a 1 b 2 i
·
j
+ a 2 b 1 j
·
i
+ a 2 b 2 j
·
j
a 2 b 2
which is the familiar scalar product. The outer product uses the wedge '
=
a 1 b 1 +
' symbol,
which is why it is also called the wedge product and has the form
a
b
=|
a
||
b
|
sin β i
j
(6.5)
where
=
+
+
a
b
(a 1 i
a 2 j )
(b 1 i
b 2 j )
=
a 1 b 1 i
i
+
a 1 b 2 i
j
+
a 2 b 1 j
i
+
a 2 b 2 j
j
= (a 1 b 2 a 2 b 1 ) i
j
which enables us to write
ab
=
a
·
b
+
a
b
(6.6)
ab
=|
a
||
b
|
cos β
+|
a
||
b
|
sin β i
j .
(6.7)
6.6 The Geometric Product in 2D
Clifford named the sum of the two products the geometric product , which means
that ( 6.6 ) reads: The geometric product ab is the sum of the inner product “ a dot b
and the outer product “ a wedge b ”.
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