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Question: A stationary swimmer S, inside a liquid of refractive index, \({\mu _1}\) is at distance \(d\) from ...

A stationary swimmer S, inside a liquid of refractive index, μ1{\mu _1} is at distance dd from a fixed point P inside the liquid. A rectangular block of width tt and refractive index μ2(μ2>μ1){\mu _2}\left( {{\mu _2} > {\mu _1}} \right) is now placed between S and P. S will observe P to be at a distance.
A) dt(2μ1μ21)d - t\left( {\dfrac{{2{\mu _1}}}{{{\mu _2}}} - 1} \right).
B) dt(1μ23μ1)d - t\left( {1 - \dfrac{{{\mu _2}}}{{3{\mu _1}}}} \right).
C) dt(1μ2μ1)d - t\left( {1 - \dfrac{{{\mu _2}}}{{{\mu _1}}}} \right).
D) dt(μ1μ21)d - t\left( {\dfrac{{{\mu _1}}}{{{\mu _2}}} - 1} \right).

Explanation

Solution

The formula of an apparent distance can be used to calculate the distance which is observed when seen from a body under a different medium. When there is change of refractive index from one medium to another medium then the object distance is observed at some apparent distance this happens as the two medium has different refractive index.

Formula used: The formula for apparent distance for a body in a medium with μ1{\mu _1} as refractive index and another object is placed in a medium μ2{\mu _2} and when one object is seen from other medium is given by, t=t(11μ)t' = t\left( {1 - \dfrac{1}{\mu }} \right) where tt is the actual distance of the object and tt' is the apparent distance of the object and μ\mu is the ratio of refractive index of the two mediums.

Complete step-by-step answer:
As it is given that a rectangular block of width tt can is placed at the medium with refractive index μ2{\mu _2} and the swimmer is at a refractive index ofμ1{\mu _1}. The refractive index of rectangular block with respect to
Swimmer is μ=μ2μ1\mu = \dfrac{{{\mu _2}}}{{{\mu _1}}}.
Now apply the formula for apparent distance,
t=t(11μ)t' = t\left( {1 - \dfrac{1}{\mu }} \right) Where tt is the width of the rectangular block.
Replace the value of μ=μ2μ1\mu = \dfrac{{{\mu _2}}}{{{\mu _1}}} in the relation above,

t=t(11μ) t=t(1μ2μ1)  t' = t\left( {1 - \dfrac{1}{\mu }} \right) \\\ t' = t\left( {1 - \dfrac{{{\mu _2}}}{{{\mu _1}}}} \right) \\\

The distance at which S will observe the P to be is,
d=dt d=dt(1μ2μ1)  d' = d - t' \\\ d' = d - t\left( {1 - \dfrac{{{\mu _2}}}{{{\mu _1}}}} \right) \\\

So the correct answer for this problem is C.

Note: The formula for calculating the apparent image for different refractive index of the medium should be remembered by students for solving such types of problems. We have subtracted the apparent distance from the distance dd while solving is because the distance between the observer and point P is given as dd and from S the apparent image will be formed before point P.