Understanding the Doppler Effect with Animation
doppler
Created: 2025/3/10

Have you heard of the Doppler effect? It is a phenomenon where the observed frequency changes depending on the speed of the wave source or the observer. Let's explore the Doppler effect through an animation!

Animation

Wave Speed

You can drag the three points above to change the speed of the points or the wind. Additionally, you can adjust the speed of the wave using the slider below the graph.

When the wave collides, the observer (green circle) flashes red. Observe how this red flashing changes when you vary the speed of the wave source!

Two Types of Frequencies

To understand the Doppler effect, let's first understand the difference between the frequency of the wave source and the frequency observed by the observer!

Frequency of the Wave Source

The frequency of the wave source represents how many waves the source generates per unit time. For example, if the source generates 3 waves per second, its frequency is 3Hz3\,\mathrm{Hz}.

Frequency Observed by the Observer

The frequency observed by the observer represents how many waves the observer detects per unit time. For example, if the observer detects 5 waves per second, the observed frequency is 5Hz5\,\mathrm{Hz}.

Observe the Doppler Effect Through Animation

Now, let's observe the Doppler effect by interacting with the animation!

When the Wave Source Approaches

Initially, the wave source is set to approach the observer.

Can you see that the waves on the right side of the wave source are more compressed compared to the left side? More precisely, the wavelength on the right side is shorter.

Due to the shorter wavelength, the observer receives more waves in a shorter time. In other words, the observed frequency increases.

When the Wave Source Moves Away

Now, set the wave source's speed to move leftward, away from the observer.

Drag the blue point representing the wave source's speed to the left, as shown in the image above.

You should see the following:

This time, the waves on the right side of the wave source are more spread out compared to the left side. In other words, the wavelength on the right side is longer, and the observed frequency decreases.

Calculating the Observed Frequency

Let's calculate the observed frequency in detail.

For simplicity, consider motion along the xx axis. Let the frequency of the wave source be f[Hz]f\,[\mathrm{Hz}], the speed of the wave be c[m/s]c\,[\mathrm{m/s}], the speed of the wave source be vsource[m/s]v_{\textrm{source}}\,[\mathrm{m/s}], and the speed of the observer be vobserver[m/s]v_{\textrm{observer}}\,[\mathrm{m/s}].

Assume that the direction from the wave source to the observer is positive.

First, let's determine the wavelength.

The wave source emits fΔtf\varDelta t waves in Δt[s]\varDelta t\,[\mathrm s]. During this time, the wave source moves vsourceΔt[m]v_{\textrm{source}}\varDelta t\,[\mathrm{m}], as shown in the figure.

Note that the first wave emitted is cΔt[m]c\varDelta t\,[\mathrm{m}] ahead after Δt[s]\varDelta t\,[\mathrm s].

Therefore, there are fΔtf\varDelta t waves in the range cΔtvsourceΔt[m]c\varDelta t-v_{\textrm{source}}\varDelta t\,[\mathrm{m}], and the wavelength is:

λ=cΔtvsourceΔtfΔt=cvsourcef[m]\lambda = \frac{c\varDelta t-v_{\textrm{source}}\varDelta t}{f\varDelta t}=\frac{c-v_{\textrm{source}}}{f}\,[\mathrm m]

Next, let's calculate the observed frequency based on this wavelength. Consider the number of waves received by the observer in Δt[s]\varDelta t\,[\mathrm s].

From the observer's perspective, the wave approaches at a speed of cvobserver[m/s]c-v_{\textrm{observer}}\,[\mathrm{m/s}], so the observer receives waves in the range (cvobserver)Δt[m](c-v_{\textrm{observer}})\varDelta t\,[\mathrm m].

The number of waves in this range is:

(cvobserver)Δtλ=cvobservercvsourcefΔt\frac{(c-v_{\textrm{observer}})\varDelta t}{\lambda}=\frac{c-v_{\textrm{observer}}}{c-v_{\textrm{source}}}f\varDelta t

Therefore, the observed frequency ff' is the number of waves received per unit time:

f=cvobservercvsourcef[Hz]f'=\frac{c-v_{\textrm{observer}}}{c-v_{\textrm{source}}}f\,[\mathrm{Hz}]

And that's how it's calculated!

Shock Waves

By carefully adjusting the speed of the wave and the wave source, you can create a phenomenon called a shock wave, which is a wave with a very large amplitude.

Details about shock waves will be introduced in another article.

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