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Relativity The Relativistic Doppler Effect Now consider A to be sending a continuous beam of electro-magnetic radiation (for example radio waves) rather than a series of pulses. It is clear that each wave crest will have a little further to go than the preceding wave crest. So, as before, the interval between received crests will be greater than the interval between transmitted crests. Now, if A and B both measure the frequency of the waves, B will obtain a lower frequency. We therefore have an effect which is very similar to the Doppler effect observed using sound waves.
Rearranging the equation for relative velocity gives us
Note that if v is changed to -v, k changes to 1/k.
the effect is usually expressed in the following way
This quantity is called the Doppler shift and can be written as (fT - fR)/fT = 1 - (fR/fT) = 1 - 1/k It can easily be shown that if v << c we have
Practical importance of the Relativistic Doppler Effect
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© David Hoult 2008 |
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