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Question
A transparent cube of side, made of a material of refractive index n2, is immersed in a liquid of refractive index n1 (n1 < n2). A ray is incident on the face AB at an angle θ (shown in the figure). Total internal reflection takes place at point E on the face BC. Then θ must satisfy:

Options
`θ > sin^-1 sqrt((n_2^2)/(n_1^2) - 1)`
`θ < sin^-1 sqrt((n_2^2)/(n_1^2) - 1)`
`θ < sin^-1 n_1/n_2`
`θ > sin^-1 n_1/n_2`
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Solution
`bb(θ < sin^-1 sqrt((n_2^2)/(n_1^2) - 1))`
Explanation:

Let the angle of refraction for i = θ be α.
Then by Snell’s law
n1 sin θ = n2 sin α ...(i)
For TIR at E
n2 sin (90° − α) > n1
From the equation (i),
sin α = `n_1/n_2` sin θ
cos α = `sqrt((n_2^2 - n_1^2 sin^2 θ)/n_2^2)`
= `sqrt((n_2^2)/(n_2^2) - (n_1^2 sin^2 θ)/n_2^2)`
= `sqrt(1 - n_1^2/n_2^2 sin^2 θ)` ...(ii)
But sin (90° − α) = `cos α > n_1/n_2`
Hence from (ii),
`1 - n_1^2/n_2^2 sin^2 θ > n_1^2/n_2^2`
Or `sin^2 θ < (n_2^2/n_1^2 - 1)`
Or `θ < sin^-1 sqrt((n_2^2)/n_1^2 - 1)`
