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Question: A lens has a power of \[ + 5\,{\text{diopter}}\] in the air. What will be its power if completely im...

A lens has a power of +5diopter + 5\,{\text{diopter}} in the air. What will be its power if completely immersed in water? The refractive index of the lens in air is 1.5. (μw=43{\mu _w} = \dfrac{4}{3})
A.+54D + \dfrac{5}{4}\,{\text{D}}
B. +214D + \dfrac{{21}}{4}\,{\text{D}}
C. +103D + \dfrac{{10}}{3}\,{\text{D}}
D. +5D + 5\,{\text{D}}

Explanation

Solution

Use the lens maker’s formula. This formula gives the relation between the power of the lens and refractive indices of the lens and the medium.

Formula used:
The lens maker’s formula is
D=(μμm1)(1R11R2)D = \left( {\dfrac{\mu }{{{\mu _m}}} - 1} \right)\left( {\dfrac{1}{{{R_1}}} - \dfrac{1}{{{R_2}}}} \right) …… (1)
Here, DD is the power of the lens, R1{R_1} and R2{R_2} are the radii of curvature of the lens, μ\mu is the refractive index of the lens and

Complete step by step answer:
The refractive indices of the lens, air and water are 1.51.5, 11 and 43\dfrac{4}{3} respectively.
The power of the lens in the air is +5diopter + 5\,{\text{diopter}}.
Calculate the power of the lens in water.
Rewrite equation (1) for the power of the lens in the air.
Dla=(μμa1)(1R11R2){D_{la}} = \left( {\dfrac{\mu }{{{\mu _a}}} - 1} \right)\left( {\dfrac{1}{{{R_1}}} - \dfrac{1}{{{R_2}}}} \right)
Here, Dla{D_{la}} is the power of the lens in the air, μ\mu is the refractive index of the lens and μa{\mu _a} is the refractive index of air.
Substitute +5diopter + 5\,{\text{diopter}} for Dla{D_{la}}, 1.51.5 for μ\mu and 11 for μa{\mu _a} in the above equation.
+5diopter=(1.511)(1R11R2)\Rightarrow + 5\,{\text{diopter}} = \left( {\dfrac{{1.5}}{1} - 1} \right)\left( {\dfrac{1}{{{R_1}}} - \dfrac{1}{{{R_2}}}} \right)
+5diopter=(0.5)(1R11R2)\Rightarrow + 5\,{\text{diopter}} = \left( {0.5} \right)\left( {\dfrac{1}{{{R_1}}} - \dfrac{1}{{{R_2}}}} \right)
(1R11R2)=10\Rightarrow \left( {\dfrac{1}{{{R_1}}} - \dfrac{1}{{{R_2}}}} \right) = 10 …… (2)
Rewrite equation (1) for the power of the lens in the water.
Dlw=(μμw1)(1R11R2)\Rightarrow {D_{lw}} = \left( {\dfrac{\mu }{{{\mu _w}}} - 1} \right)\left( {\dfrac{1}{{{R_1}}} - \dfrac{1}{{{R_2}}}} \right)
Here, Dlw{D_{lw}} is the power of the lens in the water, μ\mu is the refractive index of the lens and μw{\mu _w} is the refractive index of water.
Substitute 1.51.5 for μ\mu and 43\dfrac{4}{3} for μa{\mu _a} in the above equation.
Dlw=(1.5431)(1R11R2)\Rightarrow {D_{lw}} = \left( {\dfrac{{1.5}}{{\dfrac{4}{3}}} - 1} \right)\left( {\dfrac{1}{{{R_1}}} - \dfrac{1}{{{R_2}}}} \right)
(1R11R2)=Dlw0.125\Rightarrow \left( {\dfrac{1}{{{R_1}}} - \dfrac{1}{{{R_2}}}} \right) = \dfrac{{{D_{lw}}}}{{0.125}} …… (3)
Divide equation (3) by equation (2).
(1R11R2)(1R11R2)=0.12510\Rightarrow \dfrac{{\left( {\dfrac{1}{{{R_1}}} - \dfrac{1}{{{R_2}}}} \right)}}{{\left( {\dfrac{1}{{{R_1}}} - \dfrac{1}{{{R_2}}}} \right)}} = \dfrac{{0.125}}{{10}}
10=Dlw0.125\Rightarrow 10 = \dfrac{{{D_{lw}}}}{{0.125}}
Dlw=+54D\Rightarrow {D_{lw}} = + \dfrac{5}{4}\,{\text{D}}
Therefore, the power of the lens when completely immersed in water is+54D + \dfrac{5}{4}\,{\text{D}}.
Hence, the correct option is A.

Note: Remember that the radii of curvature R1{R_1} and R2{R_2}of the lens are constant whatever may be the medium and sign should be taken as positive if we measured the distance along the direction of incident rays and vice-versa.