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Question: The effective focal length of the lens combination shown in the figure is \[60cm\] . The radii of cu...

The effective focal length of the lens combination shown in the figure is 60cm60cm . The radii of curvature of the curved surfaces of the Plano-convex lenses are 12cm12cm each and the refractive index of the material of the lens is 1.51.5 . The refractive index of the liquid is:

A) 1.331.33
B) 1.421.42
C) 1.531.53
D) 1.601.60

Explanation

Solution

In case of using a single lens, there is only one optical element. In contrast to this, a compound lens is an array or combination of simple lenses having a common axis. Usually, the lenses are placed in contact with each other but sometimes we put a material between the lenses such as done in this question. In the case of lens combination, the powers of the lenses are added.

Formula Used:
1f=2f1+1f2\dfrac{1}{f}=\dfrac{2}{{{f}_{1}}}+\dfrac{1}{{{f}_{2}}} , 1f=(μ2μ1)[1R11R2]\dfrac{1}{f}=\left( {{\mu }_{2}}-{{\mu }_{1}} \right)\left[ \dfrac{1}{{{R}_{1}}}-\dfrac{1}{{{R}_{2}}} \right]

Complete step by step solution:
We know that power of a lens is the reciprocal of its focal length and the powers in a lens combination are added. Hence we can say that the effective power of the combination will be equal to the sum of the powers of the two Plano-convex lenses and the power of the concave lens which the liquid is forming. Mathematically, P=2P1+P2P=2{{P}_{1}}+{{P}_{2}} where P1{{P}_{1}} is the power of the Plano-convex lens, P2{{P}_{2}} is the power of the lens formed by the liquid and PP is the effective power of the combination
Substituting power by the reciprocal of focal lengths, we get
1f=2f1+1f2\dfrac{1}{f}=\dfrac{2}{{{f}_{1}}}+\dfrac{1}{{{f}_{2}}} where f1{{f}_{1}} and f2{{f}_{2}} are the focal lengths of the Plano-convex lenses equation(1)--equation(1)
It is to be noted that for the plane surface of the Plano-convex lenses, the radius of curvature of the surface will be infinite, that is Rplane={{R}_{plane}}=\infty
Hence, the reciprocal of the radius of the plane surface will be zero, since 1/=01/\infty =0 , and can be neglected
The expression for the focal lengths of the lenses can be written as,
1f1=(μ1)1R\dfrac{1}{{{f}_{1}}}=\left( \mu -1 \right)\dfrac{1}{R} and 1f2=(μL1)1R\dfrac{1}{{{f}_{2}}}=\left( {{\mu }_{L}}-1 \right)\dfrac{1}{R} where μ\mu stands for the refractive index of the lens and μL{{\mu }_{L}} stands for the refractive index of the liquid
The effective focal length of the combination is given to be 60cm60cm , that is, f=60cmf=60cm
The radius of curvature of the curved surfaces (R)=12cm(R)=12cm
The values of the focal lengths will be as given below

& \dfrac{1}{{{f}_{1}}}=\left( 1.5-1 \right)\dfrac{1}{12} \\\ & \Rightarrow \dfrac{1}{{{f}_{1}}}=\dfrac{1}{24} \\\ \end{aligned}$$ Similarly, for the lens formed by the liquid, we have $$\begin{aligned} & \dfrac{1}{{{f}_{2}}}=\left( {{\mu }_{L}}-1 \right)\dfrac{-2}{12} \\\ & \Rightarrow \dfrac{1}{{{f}_{2}}}=\dfrac{-\left( {{\mu }_{L}}-1 \right)}{6} \\\ \end{aligned}$$ Substituting these values in $$equation(1)$$ , we get $$\begin{aligned} & \dfrac{1}{f}=\dfrac{2}{{{f}_{1}}}+\dfrac{1}{{{f}_{2}}} \\\ & \Rightarrow -\dfrac{1}{60}=\dfrac{2}{24}-\dfrac{\left( {{\mu }_{L}}-1 \right)}{6} \\\ & \Rightarrow -\dfrac{1}{60}=\dfrac{1-2\left( {{\mu }_{L}}-1 \right)}{12} \\\ & \Rightarrow 1-2\left( {{\mu }_{L}}-1 \right)=-\dfrac{1}{5} \\\ & \Rightarrow 10\left( {{\mu }_{L}}-1 \right)-5=1 \\\ & \Rightarrow \left( {{\mu }_{L}}-1 \right)=0.6 \\\ & \Rightarrow {{\mu }_{L}}=1.6 \\\ \end{aligned}$$ **Hence (D) is the correct option.** **Note:** The most common error which students make in such problems is in the substitution of the values of focal length and the radius of curvature. The sign convention is extremely important in numerical optics since one misplaced minus sign can waste the entire effort put into the question. The distance measured along the direction of motion of light ray is taken to be positive and those opposite are taken negatively.