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14.
(a) For the maximum adjacent to the central one, we set
m
= 1 in Eq. 3614 and obtain
θ
1
= sin
−
1
µ
mλ
d
¶
¯
¯
¯
¯
m
=1
= sin
−
1
·
(1)(
λ
)
100
λ
¸
=0
.
010 rad
.
(b) Since
y
1
=
D
tan
θ
1
(see Fig. 368(a)), we obtain
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This note was uploaded on 11/12/2011 for the course PHYS 2001 taught by Professor Sprunger during the Fall '08 term at LSU.
 Fall '08
 SPRUNGER
 Physics

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