i=sin⁻¹(1μ)
Reflected light is polarised with its electric vector perpendicular to the plane of incidence
i=tan⁻¹(μ)
Reflected light is polarised with its electric vector parallel to the plane of incidence
When the reflected and refracted rays are perpendicular to each other, the angle of incidence is the Brewster angle (iB). At the Brewster angle, the reflected light is completely plane polarised with its electric vector perpendicular to the plane of incidence. The relationship between the Brewster angle and the refractive index is given by:
tan iB = μ
where μ is the refractive index of the material. Therefore, the angle of incidence i is equal to the Brewster angle iB, and i = tan⁻¹(μ). The reflected light is polarised with its electric vector perpendicular to the plane of incidence.