In Fig., `O` is a dot on the bottom surface of jar height `h`, filled with a transparent liquid of refractive index `mu`. `AB = d` is diameter of a disc such that when placed on the top surface, symmetrically about the centre, the dot is invisible. This would happen when rays `OA and OB` suffer total internal reflection.
If `/_AOC = i`,
then `tan i= (AC)/(OC) = (d//2)/(h)` ...(i)
For total internal reflection, `i ge c`,
when `sin i= sin c = (1)/(mu)` and `tan i= (1)/(sqrt(mu^2 - 1))`, Fig. ...(ii)
From (i) and (ii), `(d)/(2 h) = (1)/(sqrt(mu^2 - 1))`
`d = (2 h)/(sqrt(mu^2 - 1))`
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