We describe below the most basic formulae of the Doppler effect in a (transmission) medium in the classical limit: i.e., when relativistic effects are negligible. Hereafter, for brevity, we just say the classical Doppler effect instead of "the Doppler effect in a medium ... "

- The most basic formula
the classical Doppler effect
is
f' = f(1 - v/v_ph) or f = f'/(1 - v/v_ph) ,

where v is the velocity relative to the medium of an observer moving in the direction of wave propagation, v is negative if the observer is actually moving opposite to the direction of wave propagation, f ' is the frequency observed by the moving observer, f is the frequency observed by an observer at rest in the medium and v_ph is the (medium) phase velocity (i.e., the velocity of wave propagation relative to the medium).Note f ' < f for a redshift and f ' > f for a blueshift.

From the most basic formula, all other formulae for observer motion in the direction of wave propagation can be derived.

- A very important one of these other
formulae is the
classical Doppler effect
formula
for the Doppler shift
in the wavelength
for a source with a fixed
emission frequency: i.e.,
one independent of
the source velocity.
When the source is
at rest
in the medium,
this wavelength is
λ_source = v_ph/f_source .

When the source is moving relative to the medium at velocity v_source, all obsersers on the wave propagation direction no no matter what their velocity observeλ = λ_source(1-v_source/v_ph) ,

where v_source is taken as positive/negative when the observer is ahead/back of the source.The basie reason for the invariance of wavelength λ is that in the classical limit length is an invariant quantity.

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