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Physics CPhysics CPhysics CPhysics C
Chapter Chapter Chapter Chapter 17 17 17 17
From From From From serwayserwayserwayserway book book book book
Prepared by Prepared by Prepared by Prepared by
AnasAnasAnasAnas A. A. A. A. AlkanoaAlkanoaAlkanoaAlkanoa
Prepared by Prepared by Prepared by Prepared by
AnasAnasAnasAnas A. A. A. A. AlkanoaAlkanoaAlkanoaAlkanoa
M.Sc.( master degree) in Theoretical Physics,M.Sc.( master degree) in Theoretical Physics,M.Sc.( master degree) in Theoretical Physics,M.Sc.( master degree) in Theoretical Physics,
Electromagnetic Waves (Optical Science) ,Electromagnetic Waves (Optical Science) ,Electromagnetic Waves (Optical Science) ,Electromagnetic Waves (Optical Science) ,
Islamic University of Gaza (Gaza, Palestine).Islamic University of Gaza (Gaza, Palestine).Islamic University of Gaza (Gaza, Palestine).Islamic University of Gaza (Gaza, Palestine).
Chapter TwoSound waves
17.1 speed of sound waves17.1 speed of sound waves
17.2 periodic sound waves
17.3 Intensity of Periodic Sound Waves
17.4 The Doppler Effect
* Sound waves* Sound waves* Sound waves* Sound waves are the most common example of longitudinal waves.
introductionintroductionintroductionintroduction
* * * * The speed of soundThe speed of soundThe speed of soundThe speed of sound waves depends on the propertiespropertiespropertiesproperties of the medium.
****Sound waves are divided into three types that cover Sound waves are divided into three types that cover Sound waves are divided into three types that cover Sound waves are divided into three types that cover
different frequency ranges:different frequency ranges:different frequency ranges:different frequency ranges:
(1) Audible wavesAudible wavesAudible wavesAudible waves :::: lie within the range of sensitivity of the human ear.(1) Audible wavesAudible wavesAudible wavesAudible waves :::: lie within the range of sensitivity of the human ear.
((((2222)))) Infrasonic wavesInfrasonic wavesInfrasonic wavesInfrasonic waves : : : : have frequencies below the audible range, have frequencies below the audible range, have frequencies below the audible range, have frequencies below the audible range,
Elephants can use infrasonic waves to communicate with each Elephants can use infrasonic waves to communicate with each Elephants can use infrasonic waves to communicate with each Elephants can use infrasonic waves to communicate with each
other, even when separated by many kilometers.other, even when separated by many kilometers.other, even when separated by many kilometers.other, even when separated by many kilometers.
((((3333)))) Ultrasonic waves :Ultrasonic waves :Ultrasonic waves :Ultrasonic waves :
((((3333) ) ) ) Ultrasonic wavesUltrasonic wavesUltrasonic wavesUltrasonic waves : : : : have frequencies above the audible range.have frequencies above the audible range.have frequencies above the audible range.have frequencies above the audible range.
17171717....1 1 1 1 Speed of Sound Waves:Speed of Sound Waves:Speed of Sound Waves:Speed of Sound Waves:
** Before the piston is moved, the gas is
undisturbed and of uniform density, as
represented by the uniformly shaded
region in Figure (a). region in Figure (a).
**When the piston is suddenly pushed to
the right Figure (b). the gas just in front
of it is compressed (shaded regionshaded regionshaded regionshaded region).
**the pressure and density in this region
are now higher than others.
** When the piston comes to
rest Figure c, the compressed
region of the gas continues to
move to the right,
corresponding to a longitudinal
pulse traveling through the tube
with speed vvvv....with speed vvvv....
*** Now the speed of sound waves in a medium depends on the
compressibilitycompressibilitycompressibilitycompressibility and densitydensitydensitydensity of the medium.
**If the medium is a liquid or a gas and has a bulk modulus B and density then the speed of sound waves in medium is ρ
ρB
v =
µT
v =
Remark: Remark: Remark: Remark: this speed as the speed of transverse waves on
a string,
In fact, the speed of all mechanical wavesspeed of all mechanical wavesspeed of all mechanical wavesspeed of all mechanical waves follows an expression In fact, the speed of all mechanical wavesspeed of all mechanical wavesspeed of all mechanical wavesspeed of all mechanical waves follows an expression
of the general form
propertyinertial
propertyelasticv =
The speed of sound also depends on the temperature of the medium.
For example: the speed of sound in air given byFor example: the speed of sound in air given byFor example: the speed of sound in air given byFor example: the speed of sound in air given by
C
Tsmv
oc
2731/331 +=
where 331m/s is the speed of sound in air at 0°C,
Tc is the air temperature in degrees Celsius.
Using this equation the speed of sound at is v = m/sUsing this equation the speed of sound at Tc =20 °C is v = 343 m/sRemark : Remark : Remark : Remark : the way to estimate the distance (Km) to a thunderstorm is
number of seconds between seeing the flash of lightning and hearing
the thunder divided by 3 . (explain ??)(explain ??)(explain ??)(explain ??)
17171717....2 2 2 2 Periodic Sound Waves: Periodic Sound Waves: Periodic Sound Waves: Periodic Sound Waves:
** the gas is compressed and thus the
density and pressure are above their
equilibrium values.
** This compressed region, called a
compressioncompressioncompressioncompression
** The areas of low pressure regions,
called rarefactionsrarefactionsrarefactionsrarefactions
** As the piston oscillates
sinusoidally, regions of compression
and rarefaction are continuously set
up.
the position of a small element relative to its equilibrium position is
given by )cos(),( max tkxstxs ω−=
Where SSSSmaxmaxmaxmax is the maximum position of the element relative to equilibrium
(displacement amplitude).(displacement amplitude).(displacement amplitude).(displacement amplitude).
The type of wave in the figure is longitudinal wavelongitudinal wavelongitudinal wavelongitudinal wave
(1)
P∆
The type of wave in the figure is longitudinal wavelongitudinal wavelongitudinal wavelongitudinal wave
The variation in the gas pressure measured from the equilibrium
value is also periodic. And given by,
)sin(max tkxPP ω−∆=∆ (2)
maxP∆where is the pressure amplitude
maxmax svP ωρ=∆
which is the maximum change in pressure from the equilibrium value
Equations (1) and (2) shows that the pressure wave is 90°out of
phase with the displacement wave.
(3)
RemarksRemarksRemarksRemarks::::
1) the pressure variation is a
maximum when the displacement
from equilibrium is zero.
2) the displacement from equilibrium
is a maximum when the pressureis a maximum when the pressure
variation is zero.
17171717....3 3 3 3 Intensity of Periodic Sound Waves :Intensity of Periodic Sound Waves :Intensity of Periodic Sound Waves :Intensity of Periodic Sound Waves :
To evaluate the rate of energy transfer for the sound wave, we
shall evaluate the kinetic energy of this element of air, which is
In the preceding chapter, we showed that a wave traveling on a taut
string transports energy. The same concept applies to sound waves.
Consider an element of air of mass m and width x in front of a
piston oscillating with a frequency , as shown in Figure
∆
ω∆
shall evaluate the kinetic energy of this element of air, which is
undergoing simple harmonic motion.
Firstly the kinetic element of one element is given by 2
2
1vdmdk =
[ ] )sin()cos(),(),( maxmax tkxStkxSx
txsx
txv ωωω −−=−∂∂=
∂∂=
Now, we must find the speed of the element dm
(1)
(2)
Also the element is given by dmAlso the element is given by dm
dxAdm ρ= (3)
Substituting from Eqn (2) and Eqn (3) into Eqn (1) to get
[ ]
0)(sin2
1
)(sin2
1)sin(
2
1
222max
222max
2max
==
−=−−=
tatdxkxSAdk
tkxdxSAtkxSdxAdk
ωρ
ωωρωωρ
(4)
22
1
4
)2sin(
22
1
)2cos(2
1
2
1
2
1)(sin
2
1
22max
0
22max
0
22max
0
222max
λωρωρ
ωρωρ
λ
λ
λλ
λ
SAk
kxxSAk
dxkxSAdxkxSAk
=
−=
−== ∫∫
Integrating the both sides of Eqn (4) to get
That is, the kinetic energy in one wave length is given by
λωρλ22
max4
1SAk =
and the potential energy in one wave length is given by
λωρλ22
max4
1SAU =
and the total energy in one wave length is given by
λωρλ22
max2
1SAE =
The rate of energy transfer (power)(power)(power)(power) is given by
vSAT
SAT
EP 22
max22
max 2
1
2
1 ωρλωρλ ===
vSAP 22max2
1 ωρ= (5)
We define the intensity of a wave, or the power per unit area, to beWe define the intensity I of a wave, or the power per unit area, to be
the rate at which the energy being transported by the wave transfers
through a unit area A perpendicular to the direction of travel of the
wave:
A
PI = (6)
A
vSA
A
PI
22max2
1 ωρ==
From Eqn (5) into Eqn (6) to get
vSI 221 ωρ=
Finally, the intensity can be written as
(7)vSI 22max2
ωρ= (7)
RemarkRemarkRemarkRemark:::: we see that the intensity of a periodic sound wave is
proportional to the squaresquaresquaresquare ofofofof thethethethe displacementdisplacementdisplacementdisplacement amplitudeamplitudeamplitudeamplitude and to
the squaresquaresquaresquare ofofofof thethethethe angularangularangularangular frequencyfrequencyfrequencyfrequency (as in the case of a periodic
string wave).
The intensity can also be written in terms of the pressure amplitudepressure amplitudepressure amplitudepressure amplitude
v
PI
ρ2
2max∆
=
That is Eqn (7) becomes
(8)
Now consider a point source emitting sound waves equally in all directions.Now consider a point source emitting sound waves equally in all directions.
We identify an imaginary sphere of radius r centered on the source.
The average power emitted by the source must be distributed
uniformly over this spherical surface of area .
avP24 rπ
24 r
PI av
π=
Hence, the wave intensity at a distance r from the source is
(9)
Sound Level in DecibelsSound Level in DecibelsSound Level in DecibelsSound Level in Decibelsthe sound level (Greek beta) is defined by the equationβ
=
oI
Ilog10β
The constant Io is the reference intensity, taken to be at the threshold of
hearing212 /101 mwI o
−×=hearing
β is is is is measured in decibelsdecibelsdecibelsdecibels (dB).
Remark: Remark: Remark: Remark:
1)1)1)1) The sound level of the threshold of pain is The sound level of the threshold of pain is The sound level of the threshold of pain is The sound level of the threshold of pain is
2222) ) ) ) The sound level of the threshold of hearingThe sound level of the threshold of hearingThe sound level of the threshold of hearingThe sound level of the threshold of hearing
is is is is
2/1 mwI = dB120=β212 /101 mwI o
−×=
dB0=β