EXAMPLE 7.6.3 :
Find the fundamental frequency and the frequency of the first three overtones of a pipe 45.0 cm long
(a) if the pipe is open at both ends and
(b) if the pipe is closed at one end.
Use v = 344 m/s.
Solution:
A pipe closed at one end is a closed pipe. From fn = nf1 Where n=1,2,3,…
For the open pipe n =1, 2, and 3 for the first three harmonics. f2 = 764 Hz 1st Overtone
For the closed pipe n =1, 3, and 5. (odd number only) f3 = 1146 Hz 2nd Overtone
f4 = 1528 Hz 3rd Overtone
(a) Fundamental frequency of open pipe: f1 = v
2L
f1 = 344ms-1
2(0.450m)
= 382Hz
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(b) Fundamental frequency of closed pipe:
f1 = v
4L
= 344ms-1
4(0.450m)
= 191 Hz
From fn = nf1 Where n=1,3,5,7…
f3 = 573 Hz 1st Overtone
f5 = 955 Hz 2nd Overtone
f7 = 1337 Hz 3rd Overtone
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7.7 : Doppler Effects
Learning Outcome:
a) State Doppler Effect for sound waves.
b) Apply Doppler Effect equation = ± for relative motion between
∓
source and observer. Limit to stationary observer and moving source,
and vice versa.
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7.7 (a) State Doppler Effect for sound waves.
• A stationary observer notices for a truck that approaches with its horn blowing, the pitch of
the sound is higher as the vehicle approaches and lower as it recedes.
• The same situation happen when an observer is approaching or moving away from a
stationary source of sound.
• This phenomenon is called Doppler Effect.
Doppler effect is defined as the apparent change in the pitch or frequency of a sound
when there is relative motion between the source & the observer.
**If the pitch increases hence the frequency also increases but the wavelength, λ will decrease.
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Motion of source • Due to the motion of source, the wavefronts λ
are shortened as source S moves towards O.
Longer ↦ lower Shorter ↦ higher
• From v = f λ:
(f will increases as λ decreases at constant v )
Thus, observer at O hear sound of higher
frequency.
• But as source S moves away from P, the
wave fronts are spaced further apart.
• From v = f λ:
(f will decreases as λ increases at constant v )
Thus, observer at P hear sound of lower
frequency.
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7.7 (b) Apply Doppler Effect equation .
Equation for Doppler Effect
∶ = velocity of sound
= velocity of the source
= velocity of the observer
= apparent frequency
= the frequency of the source
(1) Source approaches stationary observer, = −
= ± is in the same
∓ direction with , thus
= − use minus sign (-)
= ( )
−
f a > f : observer receives a higher frequency
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(2) Source moving away from stationary observer, = −
= ± is in the opposite
∓ direction with , thus
= − use plus sign (+)
= ( )
+
f a < f : observer receives a lower frequency
(3) Observer approaches stationary source, = − is in the opposite
direction with , thus
± use plus sign (+)
∓
=
+
= ( )
= − f a > f : observer receives a higher frequency 106
(4) Observer moving away from stationary source, = −
= ± is in the same
∓ direction with , thus
use minus sign (-)
= ( − )
= − f a < f : observer receives a lower frequency
You can also remember the sign as below:
−+ :: observer approaches the source
+− :: observer moves away from the source
source moves away from the observer
source approaches the observer
For stationary observer : = 0
For stationary source : = 0
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EXAMPLE 7.7.1 :
A train moving at constant speed 20 m s–1 towards a stationary observer standing on the station platform
produces a loud sound signal at frequency 500 Hz. Determine the frequency of sound heard by the
observer when the train
(a) Towards the observer
(b) Passes the observer.
[ given : speed of sound in air = 340 m s–1 ]
Solution: : = 0 −1 ( ) (b) When the train passes the observer ,
= 20 −1 apparent frequency of sound heard :
= 500 ; = 340 −1 = ( ) 340
+ = ( 340 + 20 ) 500
(a) When the train approaches the observer , apparent
frequency of sound heard : = .
= ( ) 340
− = ( 340 − 20 ) 500
= .
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EXAMPLE 7.7.2 :
The whistle from a stationary policeman at a junction emits sound of frequency 1000 Hz. If the
speed of sound is 330 m s–1, what is the frequency of the sound heard by a passenger inside a
car moving with a speed of 20 m s–1
(a) Towards the junction
(b) Away from the junction ?
Solution: : = 20 −1 ( )
= 0 −1
(b) When the car moves away from the
= 1000 ; = 330 −1 source , apparent frequency of sound
heard :
(a) When the car approaches the source , apparent frequency = ( − ) 330 − 20
of sound heard : = ( 330 ) 1000
= ( + ) 330 + 20 = .
= ( 330 ) 1000
= .
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End of Chapter 7
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