p37_037.pdf

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Chapter 37 - 37.37
10 6 m.
(b) Minima of the single-slit diffraction pattern occur at angles θ given by a sin θ = ,where a is
the slit width. Since the fourth-order interference maximum is missing, it must fall at one of these
angles. If a is the smallest slit width for which this order is missing, the angle must be given by
a sin θ = λ . It is also given by d sin θ =4 λ ,so a = d/ 4=(6 . 0 × 10 6 m) / 4=1 . 5 × 10 6 m.
(c) First, we set θ =90 and find the largest value of m for which mλ < d sin θ . This is the highest
order that is diffracted toward the screen. The condition is the same as m<d/λ and since
d/λ =(6 . 0
×
10 9 m) / 0 . 1=6 . 0
×
10 9 m) = 10 . 0, the highest order seen is the m = 9 order. The fourth
and eighth orders are missing, so the observable orders are m =0,1,2,3,5,6,7,and9.
10 6 m) / (600
×
37. (a) Maxima of a diffraction grating pattern occur at angles θ given by d sin θ = ,where d is the slit
separation, λ is the wavelength, and m is an integer. The two lines are adjacent, so their order
numbers differ by unity. Let m be the order number for the line with sin θ =0 . 2and m +1bethe
order number for the line with sin θ =0 . 3. Then, 0 . 2 d = and 0 . 3 d =( m +1) λ . We subtract the
first equation from the second to obtain 0 . 1 d = λ ,or d = λ/ 0 . 1 = (600
×
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