P17_019.PDF
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)
Pobierz
Chapter 17 - 17.19
19. (a) We read the amplitude from the graph. It is about 5
.
0cm.
(b) We read the wavelength from the graph. The curve crosses
y
= 0 at about
x
= 15 cm and again
with the same slope at about
x
=55cm,so
λ
=55cm
−
3
.
6N
25
v
=
×
10
−
3
kg
/
m
=12m
/
s
.
(d) The frequency is
f
=
v/λ
=(12m
/
s)
/
(0
.
40 m) = 30 Hz and the period is
T
=1
/f
=1
/
(30 Hz) =
0
.
033 s.
(e) The maximum string speed is
u
m
=
ωy
m
=2
πfy
m
=2
π
(30 Hz)(5
.
0 cm) = 940 cm
/
s=9
.
4m
/
s.
(f) The string displacement is assumed to have the form
y
(
x, t
)=
y
m
sin(
kx
+
ωt
+
φ
). A plus sign
appears in the argument of the trigonometric function because the wave is moving in the negative
x
direction. The amplitude is
y
m
=5
.
0
×
10
−
2
m. The formula for the displacement
gives
y
(0
,
0) =
y
m
sin
φ
. We wish to select
φ
so that 5
.
0
×
10
−
2
. The solution is
either 0
.
93 rad or 2
.
21 rad. In the first case the function has a positive slope at
x
= 0 and matches
the graph. In the second case it has negative slope and does not match the graph. We select
φ
=0
.
93 rad. The expression for the displacement is
×
10
−
2
sin
φ
=4
.
0
×
y
(
x, t
)=(5
.
0
×
10
−
2
m) sin
(16 m
−
1
)
x
+ (190 s
−
1
)
t
+0
.
93
.
15 cm = 40 cm = 0
.
40 m.
(c) The wave speed is
v
=
τ/µ
,where
τ
is the tension in the string and
µ
is the linear mass density
of the string. Thus,
10
−
2
m,the angular frequency is
ω
=2
πf
=2
π
(30 Hz) =
190 rad
/
s,and the angular wave number is
k
=2
π/λ
=2
π/
(0
.
40 m) = 16 m
−
1
. According to the
graph,the displacement at
x
=0and
t
=0is4
.
0
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