This article was automatically translated from the original Turkish version.
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The Doppler effect is the phenomenon in which the frequency or wavelength of a wave, as measured by an observer, changes due to the relative motion between the wave source and the observer. When the source approaches the observer, the perceived frequency increases (wavelength shortens), and when the source recedes, the frequency decreases (wavelength lengthens). This physical phenomenon was first described by Austrian physicist Christian Doppler and has broad applications ranging from acoustics to astronomy, medical imaging to radar systems.

Basic illustration of the Doppler effect showing how sound waves compress in front of and expand behind a moving ambulance, depending on its speed (generated by artificial intelligence).
The concept was first proposed in 1842 by Christian Doppler in a paper titled "On the Coloured Light of Double Stars and Certain Other Celestial Bodies" (Über das farbige Licht der Doppelsterne und einiger anderer Gestirne des Himmels). Doppler hypothesized that the relative motion of stars would alter the color of the light they emit: a light source approaching an observer shifts toward blue, while one receding shifts toward red.
The validity of the theory for sound waves was experimentally demonstrated in 1845 by Dutch scientist Christophorus Buys Ballot. Buys Ballot showed that notes played by musicians on a moving train were perceived as higher in pitch as the train approached and lower in pitch as it moved away. The optical Doppler effect for light waves was later confirmed by astronomers such as William Huggins and Hermann Vogel, who observed shifts in spectral lines from stars.
The Doppler effect exhibits different dynamics depending on the type of wave and the nature of the motion. The fundamental principle is that the rate at which wave crests reach the observer (frequency) changes due to motion.
This effect is typically associated with linear motion and is related to the linear momentum of the wave. In mechanical waves such as sound, which require a material medium, the wave speed depends on the medium. The motion of the observer or the source affects the perceived frequency according to the following general formula (for reflective systems such as medical ultrasound):
<span class="katex-error" title="ParseError: KaTeX parse error: Unexpected end of input in a macro argument, expected '}' at end of input: … \frac{2VF_0}{C" style="color:#C41718">\Delta F = \frac{2VF_0}{C</span>
Here, <span class="katex"><span class="katex-html" aria-hidden="true"><span class="base"><span class="strut" style="height:0.6833em;"></span><span class="mord">Δ</span><span class="mord mathnormal" style="margin-right:0.13889em;">F</span></span></span></span> represents the frequency shift, <span class="katex"><span class="katex-html" aria-hidden="true"><span class="base"><span class="strut" style="height:0.6833em;"></span><span class="mord mathnormal" style="margin-right:0.22222em;">V</span></span></span></span> the relative velocity, <span class="katex"><span class="katex-html" aria-hidden="true"><span class="base"><span class="strut" style="height:0.8333em;vertical-align:-0.15em;"></span><span class="mord"><span class="mord mathnormal" style="margin-right:0.13889em;">F</span><span class="msupsub"><span class="vlist-t vlist-t2"><span class="vlist-r"><span class="vlist" style="height:0.3011em;"><span style="top:-2.55em;margin-left:-0.1389em;margin-right:0.05em;"><span class="pstrut" style="height:2.7em;"></span><span class="sizing reset-size6 size3 mtight"><span class="mord mtight">0</span></span></span></span><span class="vlist-s"></span></span><span class="vlist-r"><span class="vlist" style="height:0.15em;"><span></span></span></span></span></span></span></span></span></span> the source frequency, and <span class="katex"><span class="katex-html" aria-hidden="true"><span class="base"><span class="strut" style="height:0.6833em;"></span><span class="mord mathnormal" style="margin-right:0.07153em;">C</span></span></span></span> the speed of wave propagation in the medium. If the motion is not aligned with the direction of wave propagation, the velocity component must be corrected by multiplying it with the cosine of the angle (<span class="katex"><span class="katex-html" aria-hidden="true"><span class="base"><span class="strut" style="height:0.6944em;"></span><span class="mord mathnormal">cos</span><span class="mord mathnormal" style="margin-right:0.02778em;">θ</span></span></span></span>).
The rotational Doppler effect arises when dealing with rotating objects or waves carrying angular momentum (OAM/SAM). This effect is related to the angular momentum of the wave and is observed when the polarization or azimuthal phase distribution of light changes. The rotational Doppler shift (<span class="katex"><span class="katex-html" aria-hidden="true"><span class="base"><span class="strut" style="height:0.8889em;vertical-align:-0.1944em;"></span><span class="mord">△</span><span class="mord mathnormal" style="margin-right:0.03588em;">ω</span></span></span></span>) is related to the angular rotation speed of the system (<span class="katex"><span class="katex-html" aria-hidden="true"><span class="base"><span class="strut" style="height:0.6833em;"></span><span class="mord">Ω</span></span></span></span>) and the change in topological charge (<span class="katex"><span class="katex-html" aria-hidden="true"><span class="base"><span class="strut" style="height:0.8889em;vertical-align:-0.1944em;"></span><span class="mord">△</span><span class="mord mathnormal" style="margin-right:0.01968em;">l</span></span></span></span>):
<span class="katex"><span class="katex-html" aria-hidden="true"><span class="base"><span class="strut" style="height:0.8889em;vertical-align:-0.1944em;"></span><span class="mord">△</span><span class="mord mathnormal" style="margin-right:0.03588em;">ω</span><span class="mspace" style="margin-right:0.2778em;"></span><span class="mrel">=</span><span class="mspace" style="margin-right:0.2778em;"></span></span><span class="base"><span class="strut" style="height:1em;vertical-align:-0.25em;"></span><span class="mopen">(</span><span class="mord">△</span><span class="mord mathnormal" style="margin-right:0.01968em;">l</span><span class="mspace" style="margin-right:0.2222em;"></span><span class="mbin">+</span><span class="mspace" style="margin-right:0.2222em;"></span></span><span class="base"><span class="strut" style="height:1em;vertical-align:-0.25em;"></span><span class="mord">△</span><span class="mord mathnormal" style="margin-right:0.03588em;">σ</span><span class="mclose">)</span><span class="mord">Ω</span></span></span></span>
Here, <span class="katex"><span class="katex-html" aria-hidden="true"><span class="base"><span class="strut" style="height:0.8889em;vertical-align:-0.1944em;"></span><span class="mord">△</span><span class="mord mathnormal" style="margin-right:0.03588em;">σ</span></span></span></span> denotes the change in spin angular momentum. This effect is independent of frequency and requires angular momentum transfer during light-matter interaction.
The Doppler effect is widely used in science and technology for measurement and imaging purposes.
In medicine, ultrasound devices use the Doppler principle to examine blood flow and vascular structure. The frequency shift of sound waves scattered by erythrocytes (red blood cells) is analyzed to determine the speed and direction of blood flow.

Medical cross-sectional image showing how an ultrasound probe analyzes the direction and velocity of blood flow within a vessel using red and blue color coding (generated by artificial intelligence).
Astronomers use the Doppler effect to measure the radial velocities of celestial objects relative to Earth. A shift of spectral lines toward red or blue indicates whether a star is receding or approaching.

Astronomical infographic comparing the redshift or blueshift of stellar spectral lines based on their motion relative to Earth (generated by artificial intelligence).
Doppler measurements are affected by observation angle and data processing limitations. In medical measurements, when the angle between the ultrasound beam and the vessel approaches 90 degrees, the Doppler shift approaches zero and measurement error increases; an angle less than 60 degrees is recommended for optimal accuracy. Additionally, in pulsed Doppler systems, insufficient sampling rate can cause the "aliasing" artifact, where high velocities are incorrectly perceived as moving in the opposite direction or at lower speeds. In educational contexts, a common misconception is confusing sound intensity (loudness) with frequency (pitch), leading to misunderstandings of the Doppler effect.
Historical Development
Physical Principles and Types
Linear Doppler Effect
Rotational Doppler Effect
Applications
Medical Imaging (Sonography)
Astronomy and Cosmology
Other Applications
Limits and Misconceptions