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5. Using Eq. 282 and Eq. 330, we obtain
G
Fq
v
B v
B
q
v B v
B
xy
yx
x
x
=−
=
−
di
bg
±±
kk
3
where we use the fact that
B
y
= 3
B
x
. Since the force (at the instant considered) is
F
z
±
k
where
F
z
= 6.4
×
10
–19
N, then we are led to the condition
()
3.
3
z
x
z
x
F
qv vB F
B
qv v
−=
⇒
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 Spring '08
 Any
 Physics, Force

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