SONIC DOPPLER SHIFT IN MILITARY JET PT5
INTRODUCTION
We know that Doppler Effect
or Doppler shift occurs between a source and observer when they are in relative
motion with respect to each other. In this case we’ll determine the Doppler
shift that occurs when two sonic military jets are moving toward each other. A
sonic military jet is a jet that moves at the speed of sound. Consider two
military jets, jet1 [source] and jet2 [observer] moving at a speed of 343 m/s
toward each other. We’ll determine the apparent frequency of jet noise as
registered by the observer in jet2 when jet1 approaches him.
ASSUMPTIONS
1 The atmospheric air has standard
temperature and pressure conditions
·
Temperature T = 298 K or 25°C or 77°F
·
Pressure = 1 bar = 105 N/m2
2 2. The effect of humidity on sound is
negligible
3 3. The amplitude of sound is unity
4 4. The
air molecules do not move with respect to source and observer
CALCULATION
The
equation for Doppler shift is given by,
f’
= f0*{[V ± Vo]/[V ± Vs]} (Eq. 1)
f0
– Original frequency (Hz)
f’
– Apparent or observed frequency (Hz)
V
– Velocity of Sound in air at standard temperature and pressure conditions
(m/s) {V = 343 m/s}
Vo
– Velocity of observer [Jet2] (m/s)
Vs
– Velocity of Source [Jet1] (m/s)
The observer and source
are moving at the same velocity hence,
Vo = Vs (Eq. 2)
Substitute equation (2)
in equation (1),
f’ = f0*{[V
+ Vo]/[V
– Vs]} (Eq. 3)
The ‘+’ sign in the
numerator of equation (3) indicates that the observer is moving toward the
source while the ‘–’ sign in the denominator indicates that the source is
moving toward the observer.
The velocity of jet Vo
= Vs = 343 m/s (Eq. 4)
Frequency of jet noise
f0 = 1000 Hz (Eq. 5)
Speed of sound in air V
= 343 m/s (Eq. 6)
Substitute equations
(4), (5) and (6) in equation (3),
f’ = 1000*{[343 + 343]/[343
– 343]}
f’
= ∞ Hz
This is the frequency
of source noise as registered by observer [Jet2] in the military jet when
moving toward the source [Jet1]. The ‘∞’
value of frequency indicates that time is zero. It means that the source is
moving with the sound waves and hence observer will never hear anything as
frequency does not exist for the observer although he may be able to see the
source.
Difference in frequency
= f’ – f0
= ∞ – 1000
= ∞ Hz
CONCLUSION
We thus determined the
apparent frequency of source noise as registered by the observer due to Doppler
shift and concluded that the observer will be able to hear nothing when he is
moving toward the source. In fact both source and observer will each experience
the exact same Doppler shift since they both are source and observer for each
other.
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