SONIC DOPPLER SHIFT IN MILITARY JET PT3
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 an observer [pilot] in a sonic military jet is moving
toward a stationary source. A sonic military jet is a jet that moves at the
speed of sound. Consider an observer in a military jet moving at a speed of 343
m/s toward the source. We’ll determine the apparent frequency of the source as
registered by the observer in the jet.
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. The
effect of humidity on sound is negligible
3. The
amplitude of sound is unity
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 [Jet] (m/s)
Vs
– Velocity of Source (m/s)
Since the source is
stationary,
Vs = 0 (Eq.2)
Substitute equation (2)
in equation (1),
f’ = f0*{[V
+ Vo]/[V]} (Eq.3)
The ‘+’ sign in the
numerator of equation (3) indicates that the observer is moving toward the
source.
The velocity of jet Vo
= 343 m/s (Eq.4)
Frequency of source 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}
f’
= 2000 Hz
This is the frequency
of source noise as registered by observer in the military jet when approaching
the source. We can observe that the frequency increased to twice its original
value which means the observer will hear twice the original frequency of noise.
Difference in frequency
= f’ – f0
= 2000
– 1000
= 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 twice the original
frequency of sound when he is moving toward the source.
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