P17_054.PDF
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)
Pobierz
Chapter 17 - 17.54
54. (a) The frequency is
f
=1
/T
=1
/
4Hz,so
v
=
fλ
=5
.
0cm/s.
(b) We refer to the graph to see that the maximum transverse speed (which we will refer to as
u
m
)is
5
.
0 cm/s. Recalling from Ch
.
12 the simple harmonic motion relation
u
m
=
y
m
ω
=
y
m
2
πf
,wehave
5
.
0=
y
m
2
π
1
4
=
⇒
y
m
=3
.
2cm
.
(c) As already noted,
f
=0
.
25 Hz.
(d) Since
k
=2
π/λ
,wehave
k
=10
π
rad/m. There must be a sign difference between the
t
and
x
terms in the argument in order for the wave to travel to the right. The figure shows that at
x
=0,
the transverse velocity function is 0
.
050 sin
2
t
. Therefore, the function
u
(
x, t
)is
u
=0
.
050 sin
π
2
t
−
10
πx
with lengths in meters and time in seconds. Integrating this with respect to time yields
y
=
−
2(0
.
050)
π
cos
π
2
t
−
10
πx
+
C
where
C
is an integration constant (which we will assume to be zero). The sketch of this function
at
t
=2
.
0sfor0
≤
x
≤
0
.
20 m is shown.
0.03
0.02
0.01
0
0.02 0.04 0.06 0.08 0.1 0.12 0.14 0.16 0.18 0.2
x
–0.01
–0.02
–0.03
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