In , let `OS = h` be the max. height of liquid above the source for which the source cannot be seen at all.
`:. /_OSA = C`
Any other ray from `S` will be totally internally reflected because in that case, angle of incidence will be greater them the critical angle.
In `Delta OSA, sin C = (OA)/(SA) = (r)/(sqrt(r^2 + h^2)) = (1)/(mu)`
or `(1)/(mu^2) = (r^2)/(r^2 + h^2)`
`r^2 + h^2 = mu^2 r^2`
`h^2 = r^2 (mu^2 - 1)`
`h = r sqrt(mu^(2) - 1) = 1 sqrt((5//3)^(2) - 1)`
`h = (4)/(3) = 1.33 cm`.

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