Doppler_effect

A source of waves moving to the left. The frequency is higher on the left, and lower on the right.
The Doppler effect, named after Christian Doppler, is the apparent change in frequency and wavelength of a wave that is perceived by an observer moving relative to the source of the waves. For waves, such as sound waves, that propagate in a wave medium, the velocity of the observer and the source are reckoned relative to the medium in which the waves are transmitted. The total Doppler effect may therefore result from either motion of the source or motion of the observer. Each of these effects is analyzed separately. For waves which do not require a medium, such as light or gravity in special relativity only the relative difference in velocity between the observer and the source needs to be considered.

Contents

1 Development
2 General
3 Analysis
4 Applications

4.1 Everyday
4.2 Astronomy
4.3 Temperature measurement
4.4 Radar
4.5 Medical imaging and blood flow measurement
4.6 Flow measurement


5 Notes
6 References
7 Credits



 A schematic representation of the Doppler effect.
Development
Doppler first proposed the Doppler Effect 1842 in his paper, "On the Coloured Light of Double Stars and Certain Other Stars of the Heavens."[1] The hypothesis was tested for sound waves by the Dutch scientist Christoph Hendrik Diederik Buys Ballot in 1845. He confirmed that the sound's pitch was higher as the sound source approached him, and lower as the sound source receded from him. Hippolyte Fizeau discovered independently the same phenomenon on electromagnetic waves in 1848 (in France, the effect is sometimes called "effet Doppler-Fizeau").

General
For waves that travel through a medium (sound, ultrasound, etc...) the relationship between observed frequency f' and emitted frequency f is given by:






f
′

=

(



v
+

v

o




v
−

v

s





)

f



{\displaystyle f'=\left({\frac {v+v_{o}}{v-v_{s}}}\right)f\,}


where




v



{\displaystyle v\,}

 is the velocity of the waves (340 m/s for sound)





v

o





{\displaystyle v_{o}\,}

 is the velocity of the observer and





v

s





{\displaystyle v_{s}\,}

 is the velocity of the source (the thing emitting the sound)
For sign convention on velocity: A positive value is used if the motion is towards the other, and a negative value if the motion is away from the other.

Analysis
It is important to realize that the frequency of the sounds that the source emits does not actually change. To understand what happens, consider the following analogy. Someone throws one ball every second in a man's direction. Assume that balls travel with constant velocity. If the thrower is stationary, the man will receive one ball every second. However, if the thrower is moving towards the man, he will receive balls more frequently because the balls will be less spaced out. The converse is true if the thrower is moving away from the man. So it is actually the wavelength which is affected; as a consequence, the perceived frequency is also affected.
The first attempt to extend Doppler's analysis to light waves was soon made by Fizeau. In fact, light waves do not require a medium to propagate and the correct understanding of the Doppler effect for light requires the use of the Special Theory of Relativity.

Applications
 A stationary microphone records moving police sirens at different pitches depending on their relative direction.
Everyday
The siren on a passing emergency vehicle will start out higher than its stationary pitch, slide down as it passes, and continue lower than its stationary pitch as it recedes from the observer. The reason for this is that the frequency of the sound waves emitted by the siren, as perceived by the observer, is shifting. As the vehicle approaches the observer, the sound waves become compacted, as in the image at the right, and this results in the higher pitch. When the vehicle is receding from the observer, the sound waves become further and further spaced out and this is the lower pitch. This shift is not sudden, but gradual, according to the speed of the vehicle. Astronomer John Dobson explained the effect thus:

"The reason the siren slides is because it doesn't hit you."
In other words, if the siren approached the observer directly, the pitch would remain constant (as vs, r is only the radial component) until the vehicle hit him, and then immediately jump to a new lower pitch. The difference between the higher pitch and rest pitch would be the same as the lower pitch and rest pitch. Because the vehicle passes by the observer, the radial velocity does not remain constant, but instead varies as a function of the angle between his line of sight and the siren's velocity:






v

s
,
r


=

v

s


⋅
cos
⁡

θ



{\displaystyle v_{s,r}=v_{s}\cdot \cos {\theta }}


where vs is the velocity of the object (source of waves) with respect to the medium, and 



θ


{\displaystyle \theta }

 is the angle between the object's forward velocity and the line of sight from the object to the observer.

Astronomy
 Redshift of spectral lines in the optical spectrum of a supercluster of distant galaxies (right), as compared to that of the Sun (left).
The Doppler effect for electromagnetic waves such as light, is of great use in astronomy, and results in either a redshift or blueshift. It has been used to measure the speed at which stars and galaxies are approaching toward or receding from Earth, that is, the radial velocity. This is used to detect if a single star is, in fact, a close binary (i.e. double star) and even to measure the speed of rotation of stars and galaxies.
The use of the Doppler effect for light in astronomy depends on the fact that the spectra of stars are not continuous. They show absorption lines at well defined frequencies that are correlated with the energies required to excite electrons in various elements from one level to another. The Doppler effect is recognizable in the fact that the absorption lines are not always at the frequencies that are obtained from the spectrum of a stationary light source. Since blue light has a higher frequency than red light, the spectral lines from an approaching astronomical light source show a blueshift and those of receding sources show a redshift.
Among the nearby stars, the largest radial velocities with respect to the Sun are +308 km/s (BD-15°4041, also known as LHS 52, 81.7 light-years away) and -260 km/s (Woolley 9722, also known as Wolf 1106 and LHS 64, 78.2 light-years away). Positive radial velocity means the star is receding from the Sun, negative that it is approaching.

Temperature measurement
Another use of the Doppler effect which is found mostly in astronomy is the estimation of the temperature of a gas which is emitting a spectral line (a dark or bright line in a spectrum, whether visible light or otherwise). Due to the thermal motion of the gas, each emitter can be slightly red or blue shifted, and the net effect is a broadening of the line. This line shape is called a Doppler profile and the width of the line is proportional to the square root of the temperature of the gas, allowing the Doppler-broadened line to be used to measure the temperature of the emitting gas.

Radar
The Doppler effect is also used in some forms of radar to measure the velocity of detected objects. A radar beam is fired at a moving target, such as a car, moving away from the radar source (a police car, for example). Each successive wave has to travel further to reach the car, before being reflected and re-detected near the source. As each wave has to move further, the gap between each wave increases, increasing the wavelength. In some situations, the radar beam is fired at the moving car as it approaches, in which case each successive wave travels a lesser distance, decreasing the wavelength. In either situation, calculations from the Doppler effect accurately determine the car's velocity.
The Proximity fuze which was developed during World War II also relies on the Doppler effect.

Medical imaging and blood flow measurement
An echocardiogram can, within certain limits, produce accurate assessment of the direction of blood flow and the velocity of blood and cardiac tissue at any arbitrary point using the Doppler effect. One of the limitations is that the ultrasound beam should be as parallel to the blood flow as possible. Velocity measurements allow assessment of cardiac valve areas and function, any abnormal communications between the left and right side of the heart, any leaking of blood through the valves (valvular regurgitation), and calculation of the cardiac output. Contrast-enhanced ultrasound using gas-filled microbubble contrast media can be used to improve velocity or other flow-related medical measurements.
Although "Doppler" has become synonymous with "velocity measurement" in medical imaging, in many cases it is not the frequency shift (Doppler shift) of the received signal that is measured, but the phase shift (when the received signal arrives).
Velocity measurements of blood flow are also used in other fields of medical ultrasonography, such as obstetric ultrasonography and neurology. Velocity measurement of blood flow in arteries and veins based on Doppler effect is an effective tool for diagnosis of vascular problems like stenosis.[2]

Flow measurement
Instruments such as the laser Doppler velocimeter (LDV), and Acoustic Doppler Velocimeter (ADV) have been developed to measure velocities in a fluid flow. The LDV and ADV emit a light or acoustic beam, and measure the Doppler shift in wavelengths of reflections from particles moving with the flow. This technique allows non-intrusive flow measurements, at high precision and high frequency.

Notes

↑ Reprinted in: Kurt Bretterbauer et al., Christian Doppler, Leben und Werk. Der Dopplereffekt, Salzburg 1988.

↑ D. H. Evans and W. N. McDicken, Doppler Ultrasound (Second Edition, John Wiley and Sons, 2000).


ReferencesISBN links support NWE through referral fees
Evans, D. H. & McDicken, W. N. Doppler Ultrasound, Second Edition. John Wiley and Sons, 2000. ISBN 0471970018



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