P16_026.PDF
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Chapter 16 - 16.26
26. (a) The textbook notes (in the discussion immediately after Eq. 16-7) that the acceleration amplitude
is
a
m
=
ω
2
x
m
,where
ω
is the angular frequency (
ω
=2
πf
since there are 2
π
radians in one cycle).
Therefore, in this circumstance, we obtain
a
m
=(2
π
(1000Hz))
2
(0
.
00040m) =1
.
6
×
10
4
m
/
s
2
.
(b) Similarly, in the discussion after Eq. 16-6, we find
v
m
=
ωx
m
so that
v
m
=(2
π
(1000Hz))(0
.
00040m) =2
.
5m
/
s
.
(c) From Eq. 16-8, we have (in absolute value)
|
a
|
=(2
π
(1000Hz))
2
(0
.
00020m) =7
.
9
×
10
3
m
/
s
2
.
16-4, but here we will use trigonometric
relations along with Eq. 16-3 and Eq. 16-6. Thus, allowing for both roots stemming from the
square root,
§
sin(
ωt
+
φ
)=
±
1
−
cos
2
(
ωt
+
φ
)
−
v
ωx
m
=
±
1
−
x
2
x
2
m
.
Taking absolute values and simplifying, we obtain
|
v
|
=2
πf
x
2
m
−
x
2
=2
π
(1000)
0
.
00040
2
−
0
.
00020
2
=2
.
2m
/
s
.
(d) This can be approached with the energy methods of
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