Dashboard/Learning Hub/Physics HL/Chapter 16/16.4 Moving Observer, Combined Motion, and Reflections

Physics HL · Chapter 16: The Doppler Effect

16.4 Moving Observer, Combined Motion, and Reflections

Handle observer-motion Doppler shifts, unify source+observer motion in one expression, and solve reflected-wave speed measurements.

Estimated time: 44 minutes

Stationary Source with Moving Observer

For a moving observer, the source still emits into still air with unchanged spacing around a stationary source. The observer's motion changes how fast fronts are encountered. Moving toward the source increases encounter rate; moving away decreases it.

ight); ext{(toward source)},qquad f' = fleft( rac{v-u_o}{v} ight); ext{(away from source)}$$

Observer motion modifies relative speed between observer and passing wavefronts.

Because the medium spacing is unchanged for stationary source cases, observer motion does not alter wavelength in the air itself. It alters only meeting rate with those fronts, which is exactly what frequency records.

General Combined-Motion Form

ight)$$

In one line-of-sight sign convention, u_o is positive toward source and u_s is positive toward observer.

This expression reduces to each special case immediately by setting one speed to zero. It is efficient but only if your sign convention is explicit. Write one short sign sentence before substitution to avoid mixing opposite conventions from different textbooks.

Reflected Sound and Double Shift

In reflected-sound setups, the moving object first acts as observer and then as source of the reflected wave. That creates two Doppler stages. This is the basis for velocity measurements in Doppler ultrasound and speed-detection radar analogs that use acoustic waves.

ight); ext{(approaching reflector)}$$

Equivalent to applying one observer-shift and one source-shift successively.

Note

If the reflector recedes, interchange approach/recede signs so the net returned frequency drops below emitted frequency.

Simulation: Reflection Doppler Analyzer

Model the two-stage shift for a moving reflector and compare intermediate frequency at the reflector with final returned frequency.

Doppler Effect Lab

Frequency at reflector

2.28e+3 Hz

Returned frequency

2.36e+3 Hz

Return factor

1.0732 x

Reflector speed

12.0 m/s

Two-stage shift for reflected ultrasound/radar-style reasoning

EmitterReflectorForward wave f1 = 2.28e+3 HzReturned wave f2 = 2.36e+3 HzReflection uses two Doppler steps: source-to-reflector then reflector-to-emitter.
For an approaching reflector this lab usesf_return = f (v + u)/(v - u)which matches the two-step Doppler process used in medical blood-flow and police-speed measurements.

Test Yourself

A 15.0 kHz sound wave reflects from an approaching car and returns at 16.1 kHz. Take v = 340 m/s. Enter car speed in m/s.

Hint: Treat as two Doppler shifts or use f_return = f(v+u)/(v-u).