Imagine a 🚗 speeding past you while its horn blares. The sound you hear is a bit higher in pitch than the horn’s actual tone. That change in pitch is the Doppler Effect – the shift in frequency of a wave when the source and/or observer are moving relative to each other.
The observed frequency \(fo\) depends on the source frequency \(fs\), the speed of sound \(v\), and the speed of the source \(v_s\) (positive when moving toward the observer, negative when moving away):
\$fo = fs \frac{v}{v \pm v_s}\$
• Use the minus sign in the denominator when the source is moving toward the observer (frequency increases).
• Use the plus sign when the source is moving away (frequency decreases).
Let’s work through a couple of quick examples.
An ambulance (source frequency \(fs = 600\,\text{Hz}\)) approaches you at \(vs = 20\,\text{m/s}\). Speed of sound \(v = 340\,\text{m/s}\). Find the frequency you hear.
| Step | Calculation |
|---|---|
| Denominator | \(v - v_s = 340 - 20 = 320\) |
| Observed frequency | \(f_o = 600 \times \frac{340}{320} \approx 637.5\,\text{Hz}\) |
A train emits a whistle at \(fs = 400\,\text{Hz}\) and moves away at \(vs = 15\,\text{m/s}\). What frequency do you hear?
| Step | Calculation |
|---|---|
| Denominator | \(v + v_s = 340 + 15 = 355\) |
| Observed frequency | \(f_o = 400 \times \frac{340}{355} \approx 383.0\,\text{Hz}\) |
Remember: the Doppler Effect is all about relative motion – the faster the relative speed, the bigger the frequency shift! 🚀