DOPPLER SHIFT IN A HIGH SPEED CHASE
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 cop car is chasing the fugitive car on a straight long
freeway. Consider two cars, cop car [source] moving at 90 mph [144 kph] toward
a fugitive car [observer] moving at 65 mph [104 kph] on a long freeway. We’ll
determine the apparent frequency as registered by the observer in fugitive car
when cop car sounds the siren.
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 fugitive car [observer] (m/s)
Vs
– Velocity of cop car [source] (m/s)
The Doppler shift
equation for this case is,
f’ = f0*{[V
– Vo]/[V – Vs]} (Eq.2)
The ‘–’ sign in the
numerator of equation (2) indicates that the observer is moving away from the
source while the ‘–’ sign in the denominator indicates that the source is
moving toward the observer.
The velocity of
fugitive car is Vo = 65 mph
= 28.88 m/s (Eq. 3)
The velocity of cop car
is Vs = 90 mph
= 40 m/s (Eq. 4)
Frequency of cop car
siren f0 = 700 Hz (Eq. 5)
Speed of sound in air V
= 343 m/s (Eq.6)
Substitute equations (3),
(4), (5) and (6) in equation (2),
f’ = 700*{[343 –
28.88]/[343 – 40]}
f’
= 725.68 Hz
This is the frequency
of sound as registered by the observer [fugitive car] at the freeway when
source [cop car] approaches him.
Difference in frequency
= f’ – f0
= 725.68
– 700
= 25.68
Hz
CONCLUSION
We thus determined the
apparent frequency as registered by the observer due to Doppler shift.
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