p37_037.pdf
(
63 KB
)
Pobierz
Chapter 37 - 37.37
10
−
6
m.
(b) Minima of the single-slit diffraction pattern occur at angles
θ
given by
a
sin
θ
=
mλ
,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
=
mλ
,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
=
mλ
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
×
Plik z chomika:
kf.mtsw
Inne pliki z tego folderu:
p37_001.pdf
(57 KB)
p37_002.pdf
(55 KB)
p37_003.pdf
(56 KB)
p37_004.pdf
(61 KB)
p37_005.pdf
(59 KB)
Inne foldery tego chomika:
chap01
chap02
chap03
chap04
chap05
Zgłoś jeśli
naruszono regulamin