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then
×
N
=
×
+
=
×
+
×
=
×
N
N
N
D
N
N
N
D
N
D
(10.11)
If we now substitute Eq. (10.10) in Eq. (10.11), we obtain
N
N
F
u
P
v
F
v
P
u
×
×
×
N =
×
=
×
N
N
D
N
N
N
N
N
N
F
u
P
v
F
v
P
u
×
×
×
×
N =
N
×
(10.12)
N
Equation (10.12) now contains a triple product, which, as we discovered in Section 2.9.2, has
the following identity:
a
×
b
×
c
=
a
·
c b
a
·
b c
Expanding Eq. (10.12) produces
N
N
N
N
F
u
P
v
N P
v
F
v
P
u
N P
u
·
·
·
·
N
N
N =
N
×
N
But
2
N
·
N
=
N
and
P
v =
P
u =
N
·
0 and N
·
0
Therefore,
F
u
2 P
v
F
v
2 P
u
F
v
N
N
P
u
F
u
P
v
N =
N
×
=
N
N
which can be expressed as
×
N
=
N
N
A
(10.13)
where
P
v
Because of the cross product in Eq. (10.13), A must be perpendicular to the plane containing
N and N . Therefore, one can imagine that N has been rotated about A to N .
Now since
F
v
P
u
F
u
A
=
N
N
×
=
N
×
D
 
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