P18_033.PDF
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)
Pobierz
Chapter 18 - 18.33
10
−
6
kg)
/
(0
.
220 m)
(405 m
/
s)
2
= 596 N.
(c) The wavelength is
λ
=2
L
=2(0
.
220 m) = 0
.
440 m.
(d) The frequency of the sound wave in air is the same as the frequency of oscillation of the string.
The wavelength is different because the wave speed is different. If
v
a
is the speed of sound in air
the wavelength in air is
λ
a
=
v
a
/f
= (343 m
/
s)
/
(920 Hz) = 0
.
373 m.
×
33. (a) When the string (fixed at both ends) is vibrating at its lowest resonant frequency, exactly one-
half of a wavelength fits between the ends. Thus,
λ
=2
L
.Weobin
v
=
fλ
=2
Lf
=
2(0
.
220 m)(920 Hz) = 405 m
/
s.
(b) The wave speed is given by
v
=
τ/µ
,where
τ
is the tension in the string and
µ
is the linear
mass density of the string. If
M
is the mass of the (uniform) string, then
µ
=
M/L
.Thus
τ
=
µv
2
=(
M/L
)
v
2
=
(800
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P18_003.PDF
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P18_004.PDF
(58 KB)
P18_001.PDF
(61 KB)
P18_002.PDF
(62 KB)
P18_005.PDF
(60 KB)
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chap03
chap04
chap05
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