Lecture 22: Doppler effect


Readings: Textbook pages 552-557

Some effects that change wave properties: Propagation in non-uniform medium

  • Simple waves propagate in the medium that have fixed speed of the waves v and thus have specific frequency f and wavelength λ related by f λ =v

  • What happens if the properties of the meidum are not uniform, for example temperature of the gas or density of the metal rod changes ?
    • speed of the wave have to change
    • relation f λ =v still holds ( it is local )
    • Something, frequency or wavelength, or both have to change.
  • Frequency does not change - if you push a piece of gas with a particular frequency, it reacts with the same frequency, and pushes at the next piece with the same frequency
  • So what changes is the wavelength
  • Indeed, if v decreases, in the same time interval (equal say the period) the perturbations propagates over a shorter distance, creating shorter wave.
  • Of course, if the properties of the materials change too rapidly, part or all of the wave will reflect of such "boundary"

Doppler effect as frequency changing effect

  • Doppler effect arise when receiver and/or emitter of a wave move relative to each other.

Motion of the receiver (listener)

  • In case of sound the wave propagates in the medium that we condider at rest
  • If the receiver (listener) moves wrt to the air, the frequecy of the sound that it receives is
    fL = (v + vL )/ λ = f (v+vL)/v
  • The frequency and wave length of the wave in the air is the reference f and λ.
  • Important is the sign of the effect We consider vL positive if receiver moves towards the source . Then the frequency at the receiver is higher than the frequency of the wave.

Motion of the emitter (source)

  • If the source moves wrt to the air, its oscillations at frequency fS produce the wave in the medium with wavelength not v/fS but λfront = ( v - vS ) / fS in fron of the source and λbehind = ( v + vS ) / fS behind the source.
  • The wave still has speed v so behind the source its frequency adjusts to be
    f= v/λbehind = fS v / (v+vS)
  • This frequency is the freuency of the wave that a listener behind the source will receive. If listener does not move wrt air, it will be the frequency it hears.
  • Important is the sign of the effect We consider vS positive if the source moves away from the receiver. Then the frequency of the wave lower than the frequency of the source.
  • Combinining two results when both the source and receiver moves wrt the air, we obtain (speed of sound is positive, speed of receiver and the source is positive in the direction from the receiver to the source)
    fL = f (v+vL)/v = fS (v+vL)/(v+vS)

Doppler effect when reciever and the source move not strictly towards each other