Let I0 be the intensity of polarized light after passing through the first polarizer P1. Then the intensity of light after passing through second polarizer P2 will be L=I0cos2q
where θ is the angle between pass axes of P1 and P2. since, P1 and P3 are crossed the angle between the pass axes of P2 and P3 will be (2π−θ). Hence, the intensity of light emerging from P2 will be I=I0(cos)2θ(cos)2(2π−θ) I=I0(cos)2θ(sin)2θ=(4I0)(sin)2 2θ
Hence, transmitted intensity will be maximum,
when θ=4π.