A source of light is moving with speed \(\frac{c}{2}\) towards an observer who is also moving towards the source with speed \(\frac{c}{2}\), Both the velocities are with respect to lab. If the source emits light of frequency f0 then Frequency measured by the observer will be

1
\(f_0\)
2
\(\frac{\sqrt{3}f_0}{2}\)
3
\(\sqrt{3}f_0\)
4
\(3f_0\)

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