In the drawing, suppose that the angle of incidence is 1 = 42.5°, the thickness of the pane is 3.15 mm, and the refractive index of the pane is n2 = 1.58. Find the amount (in mm) by which the emergent ray is displaced relative to the incident ray.
Given,
n1 = n-air = 1 ; theta1 = 42.5 deg ;
n2 = 1.58 ; d = 3.15 mm
We know from Snell's law
n1 sin(theta1) = n2 sin(theta2)
sin(theta2) = n1 sin(theta1)/n2
sin(theta2) = 1 x sin42.5/1.58 => theta2 = 25.31 deg
Hence, theta2 = 25.31 deg
Again from snell's law
n2 sin(theta2) = n3 sin(theta3)
theta3 = sin^-1(1.58 x sin25.31/1) = 42.5 deg
theta1 = theta3
using trigonometry
x = d sin(theta1 - theta2)
x = 3.15 mm sin(42.5 - 25.31) = 0.931 mm
Hence, x = 0.931 mm
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