SONIC DOPPLER SHIFT IN MILITARY JET PT2
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 a sonic military jet is moving away from a stationary
observer in a building. A sonic military jet is a jet that moves at the speed
of sound. Consider a military jet moving at a speed of 343 m/s receding away
from an observer who is inside a building. We’ll determine the apparent
frequency of the jet’s noise as registered by the observer.
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 (m/s)
Vs
– Velocity of Source [Jet] (m/s)
Since the observer is
stationary,
Vo = 0 (Eq. 2)
Substitute equation (2)
in equation (1),
f’ = f0*{[V]/[V
+ Vs]} (Eq. 3)
The ‘+’ sign in the
denominator of equation (3) indicates that the source is receding away from the
observer.
The velocity of jet Vs
= 343 m/s (Eq. 4)
Frequency of jet
exhaust 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]}
f’
=
500 Hz
This is the frequency
of jet noise as registered by the stationary observer in a building when a
military jet is receding away from him. We can observe that the frequency
reduced to half its original value which means the observer will only hear half
of the original frequency.
Difference in frequency
= f’ – f0
= 500 – 1000
= – 500 Hz
Negative sign indicates
that apparent frequency is less than original but magnitude is always positive.
CONCLUSION
We thus determined the apparent
frequency of jet noise as registered by the observer due to Doppler shift and
concluded that the observer will be able to hear only half of the original
frequency of jet noise when he watches the jet receding away from him.
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