We call the lab and the water tank reference frames S and S’, respectively. The relative speed between S and S’ is . The speed of light relative to S’ (the tank water frame) is , where n is the refractive index of water. The speed of light relative to S (the lab frame) is v . The speeds of light in S and S’ are related by the Lorentz velocity transformation [Eq. ()], from which the dragging coefficient can be obtained.
From Eq. (),
where we used . The Taylor expansion of in powers of gives us the series
We see that Fizeau's experimental formula is the linear approximation of the relativistic-based calculated series. Moreover, we find . Using n = 1.333 (for water), we find
In Fizeau's experiment the speed of the water tank is much smaller than c , so the higher order terms in the relativistic series are negligibly small and Fizeau's formula is a good approximation to the relativistic result; Fizeau's experimental value for K is within 1% of the relativistic calculated value.