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and
F N
N
P
v =
P
v +
F
v
N
+
N
v
To simplify these partial derivatives, it is assumed that the relative magnitude of F is negligible
and can be ignored. Thus,
N
P
u =
P
u +
F
u
N
and
N
P
v =
P
v +
F
v
N
which permits Eq. (10.7) to be written as
P
u +
N
P
v +
N
F
u
F
v
N =
×
(10.8)
N
N
Basically, Eq. (10.8) has the form of four vectors:
a
+
b
×
c
+
d
which, when expanded, equals
a
+
b
×
c
+
d
=
a
×
c
+
b
×
c
+
a
×
d
+
b
×
d
Expanding Eq. (10.8) along similar lines, we obtain
N
P
u ×
P
u ×
P
v +
F
u
P
v
F
v
N
F
u
F
v
N
N
N =
×
+
+
×
N
N
N
N
But
N
N
×
=
0
N
N
and
P
u ×
P
v =
N
Therefore,
P
u ×
F
u
N
P
v
F
v
N
N =
N
+
×
+
N
N
or
N
P
u ×
N
F
u
P
v
F
v
×
+
N =
N
+
N
 
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