The process of apparent change in frequency (or wavelength) of the light due to relative motion between the source of light and the observer is called Doppler's effect.
If V = actual frequency, V' = Apparent frequency, v = speed of source w.r.t stationary observer, c = speed of light
1. Source of light moves towards the stationary observer: When a light source is receding from an observer with a relative velocity v then the apparent frequency (v) is less than the actual frequency (v) of light. Thus apparent wavelength (λ') is greater the actual wavelength (λ).
For v < < c :
(i) Apparent frequency v' = v(1+v/c) and
(ii) Apparent wavelength λ' = λ(1+v/c)
(iii) Doppler's shift: Apparent wavelength < actual wavelength. This is called violet shift.
Doppler's shift Δλ = λ.v/c
(iv) The fraction decrease in wavelength = Δλ/λ =v/c
2. Source of light moves away from the stationary observer : In this case v′<v and λ′>λ
For v < < c :
(i) Apparent frequency v' = v(1-v/c) and (ii) Apparent wavelength λ' = λ(1+v/c)
(iii) Doppler's shift : Apparent wavelength > actual wavelength. This is called red shift.
Doppler's shift Δλ = λ.v/c
(iv) The fractional increase in wavelength = Δλ/λ =v/c
3. Doppler broadening: For a gas in a discharge tube, atoms are moving randomly in all directions. When spectrum of light emitted from these atoms is analyzed, then due to Doppler effect (because some atoms are moving towards detector, some atoms are moving away from detector), the frequency of a spectral line is not observed as having one value, but is spread over a range
±Δv = ±(v/c)v , ±Δλ = ±(v/c)λ
This broadens the spectral line by an amount ( 2Δλ ). It is known as Doppler broadening. It is relaying on v, which in part is proportional to√T , where T is the temperature in Kelvin.
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