Malus law: It states that the intensity of polarised light transmitted through the analyser varies as the square of cosine of the angle between the plane of transmission of analyser and polariser. i.e. I ∝ cos2 θ
Proof
Let OQ = amplitude \((\overrightarrow A)\) of vibration of electric vector transmitted by the polariser.
θ = angle between the plane of analyser and polariser.
Let us resolve \((\overrightarrow A)\) into two components.
- A cos θ along OR (i.e. parallel to the plane of transmission of analyser).
- A sin θ along OP (i.e. perpendicular to the plane of transmission of analyser).

Since only A cos θ component is transmitted through the analyser, so the intensity of light transmitted through the analyser is given by:
I = (A cos θ)2
or I = A2 cos2 θ
or I = I0 cos2θ ...........(1)
where I0 = A2 is the intensity of incident light from the polariser.
So Eq. (1) can be written as I cos2θ.
Special cases
(i) When the plane of polariser and analyser are parallel to each other.
i.e. θ = 0°
From Eq. (1), we have
I = I0
i.e. maximum intensity.
(ii) When the plane of polariser and analyser are perpendicular to each other.
i.e. θ = 90°
From Eq. (1), we have I = 0
i.e. zero intensity.