On an optics bench

PHYSICS · Multi-part · Fermi University Physics · Optics & Photonics · Polarisation and anisotropic media · Polarisation and anisotropic media

Optics and Photonics, Ch Birefringence and crystal optics

Problem

On an optics bench, a half-wave plate (Γ=π\Gamma = \pi) is mounted with its fast axis at 15∘15^\circ to the horizontal. Horizontal linearly polarised light (polarised at 0∘0^\circ) is incident on it. ((a)) Without multiplying out the Jones matrices, use the reflection rule for a half-wave plate to state the direction of the output polarisation, measured from the horizontal. ((b)) A photoelastic model of a cantilever bracket, of thickness d=6.0d = 6.0 mm (the thickness the light travels through), is loaded so that the stress-induced index difference n1−n2n_1 - n_2 grows with distance xx from the free end as Δn(x)=Δnmax⁡(x/L)2\Delta n(x) = \Delta n_{\max}(x/L)^2, reaching Δnmax⁡=2.0×10−4\Delta n_{\max} = 2.0\times10^{-4} at the clamped end (x=Lx=L). The model is viewed in light of wavelength λ=589\lambda = 589 nm between crossed polarisers set at 45∘45^\circ to the bracket's principal stress directions, so that isoclinic bands are absent. State, with a reason, whether the isochromatic (dark) bands are more closely spaced near the free end or near the clamped end, and find the total number of dark isochromatic bands (orders m=0,1,2,…m = 0, 1, 2, \dots) seen along the bracket.

Browse the problem library