When two plane-polarised waves are superimposed, then under certain conditions, the resultant light vector rotates with a constant magnitude in a plane perpendicular to the direction of propagation. The tip of the vector traces a circle and the light is said to be circularly polarised.
To form circularly polarised light Ex=E0sinωt Ey=E0cosωt=E0sin(ωt+2π)
where E0 is amplitude.
Resultant amplitude ∣E∣2=E0+E0+2E0⋅E0cos2π ∣E∣2=E02= constant