Doppler Effect: PYQ Walkthrough (1)

easy 2 min read

Question

A train approaches a stationary observer at 30m/s30\,\text{m/s} while sounding a horn of frequency 500Hz500\,\text{Hz}. The speed of sound in air is 340m/s340\,\text{m/s}. What frequency does the observer hear when the train is approaching, and what does the observer hear after the train has passed and is receding at the same speed?

Solution — Step by Step

For a moving source and stationary observer:

f=fvv±vsf' = f \cdot \frac{v}{v \pm v_s}

The minus sign applies when the source approaches; plus when it recedes.

fapp=500×34034030=500×340310f'_{\text{app}} = 500 \times \frac{340}{340 - 30} = 500 \times \frac{340}{310}

fapp=500×1.0968548.4Hzf'_{\text{app}} = 500 \times 1.0968 \approx 548.4\,\text{Hz}

frec=500×340340+30=500×340370f'_{\text{rec}} = 500 \times \frac{340}{340 + 30} = 500 \times \frac{340}{370}

frec=500×0.9189459.5Hzf'_{\text{rec}} = 500 \times 0.9189 \approx 459.5\,\text{Hz}

The pitch jumps from about 548 Hz down to about 460 Hz as the train passes — a drop of nearly 90 Hz. This is the characteristic “neeeeoooom” of a fast vehicle going past.

Final: approaching 548\approx 548 Hz, receding 460\approx 460 Hz.

Why This Works

When the source moves toward you, each successive wavefront is emitted from a closer position, so the wavefronts crowd together — shorter wavelength, higher frequency. When the source recedes, wavefronts spread apart and frequency drops.

Note that the shift is not symmetric — the drop on receding is slightly larger than the rise on approaching, because the formula has the source velocity in the denominator. For small velocities (vsvv_s \ll v), the shifts become approximately symmetric.

Alternative Method

For small Mach numbers, use the linearised approximation:

Δf±fvsv\Delta f \approx \pm f \cdot \frac{v_s}{v}

This gives a shift of ±500×30/340±44\pm 500 \times 30/340 \approx \pm 44 Hz, predicting roughly 544 and 456 Hz. Close to the exact answers but not identical.

Common Mistake

Students mix up source-moving and observer-moving formulas. For a moving source, vsv_s goes in the denominator. For a moving observer, vov_o goes in the numerator. Memorise these positions or rederive — never guess.

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