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Asked in GUJCET 2015 · Total internal reflection and optical fibres
Given: n_A=1.6 (denser) and n_B=1.5 (rarer).
Idea: at the critical angle the refracted ray just grazes the boundary, so r=90°.
Snell's law n_A sin C=n_B sin 90° then gives sin C=(n_B)/(n_A).
sin C=(1.5)/(1.6)=(15)/(16)
C=sin⁻¹((15)/(16))≈ 69.6°
The two media are close in density, so the critical angle is large: only a very steep ray is turned back.
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