The phase shift between ordinary and extraordinary waves in the plastic and thus the degree of transmission is dependent on both the birefringence An (= no-ne), and the air wavelength λo: ΔΦ = (nod - ned) (Σπίλο) where the symbols have their usual meaning. If we have a situation whereby, at a particular region in the plastic, for blue light (o= 450nm) the phase shift is 4x and the blue light is not transmitted, at what wavelength will the phase shift be 3r, where the transmission will be a maximum? What will happen to the blue light if we rotate one of the polarisers so that the transmission axes of the two are now parallel?

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The phase shift between ordinary and extraordinary waves in the plastic and thus the
degree of transmission is dependent on both the birefringence An (= no-ne), and the
air wavelength 20:
Ap= (nod-ned) (2π/20)
where the symbols have their usual meaning.
If we have a situation whereby, at a particular region in the plastic, for blue light (20=
450nm) the phase shift is 47 and the blue light is not transmitted, at what wavelength
will the phase shift be 3r, where the transmission will be a maximum? What will
happen to the blue light if we rotate one of the polarisers so that the transmission
axes of the two are now parallel?
Transcribed Image Text:The phase shift between ordinary and extraordinary waves in the plastic and thus the degree of transmission is dependent on both the birefringence An (= no-ne), and the air wavelength 20: Ap= (nod-ned) (2π/20) where the symbols have their usual meaning. If we have a situation whereby, at a particular region in the plastic, for blue light (20= 450nm) the phase shift is 47 and the blue light is not transmitted, at what wavelength will the phase shift be 3r, where the transmission will be a maximum? What will happen to the blue light if we rotate one of the polarisers so that the transmission axes of the two are now parallel?
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