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Question: An equi concave diverging lens of focal length \(F\) is cut into two equal halves. The two halves ar...

An equi concave diverging lens of focal length FF is cut into two equal halves. The two halves are turned around and joined with some liquid between them. The lens obtained is converging with a focal length FF. If the refractive index of the liquid is 33, then what is the refractive index of the lens?

& A.4 \\\ & B.2 \\\ & C.5 \\\ & D.1.5 \\\ \end{aligned}$$
Explanation

Solution

We know that the lens makers formula for thin lenses, where FF is the focal length, also R=2FR=2F, μ\mu is the refractive index of the lens and R1R_{1} and R2R_{2} is the radius of curvature of the spheres of surfaces 1 and 2 respectively.

Formula used:
1F=(μ1)(1R11R2)\dfrac{1}{F}=(\mu-1)\left(\dfrac{1}{R_{1}}-\dfrac{1}{R_{2}}\right)

Complete step by step answer:
We also know that the focal length FF of the concave lens given by the lens makers formula is expressed as 1F=(μ1)(2R)\dfrac{1}{F}=(\mu-1)\left(\dfrac{2}{R}\right), where μ\mu is the refractive index of the concave lens and RR is its radius of curvature.
Now consider the focal length of the combination of two halves of the concave lens and the liquid with refractive index μl=3\mu_{l}=3.
Then clearly 1f1=(μ1)(11R)=(μ1)(1R)\dfrac{1}{f_{1}}=(\mu-1)\left(\dfrac{1}{\infty}-\dfrac{1}{R}\right)=(\mu-1)\left(\dfrac{1}{-R}\right)
Similarly, 1f3=(μ1)(11R)=(μ1)(1R)\dfrac{1}{f_{3}}=(\mu-1)\left(\dfrac{1}{\infty}-\dfrac{1}{R}\right)=(\mu-1)\left(\dfrac{1}{-R}\right)
But since the f2f_{2} has some liquid between them, then we get, 1f2=(μl1)(1R1R)=(μl1)(2R)\dfrac{1}{f_{2}}=(\mu_{l}-1)\left(\dfrac{1}{R}-\dfrac{1}{R}\right)=(\mu_{l}-1)\left(\dfrac{2}{R}\right)
We can write it as 1f1+1f2+1f3=(μ1)(1R)+(μl1)(2R)+(μ1)(1R)\dfrac{1}{f_{1}}+\dfrac{1}{f_{2}}+\dfrac{1}{f_{3}}=(\mu-1)\left(\dfrac{1}{-R}\right)+(\mu_{l}-1)\left(\dfrac{2}{R}\right)+(\mu-1)\left(\dfrac{1}{-R}\right)

An equiconvex lens of focal length FF is cut into two equal halves and the joined with some liquid between them, we can say that 1F=1f1+1f2+1f3\dfrac{1}{F}=\dfrac{1}{f_{1}}+\dfrac{1}{f_{2}}+\dfrac{1}{f_{3}}
Then we can get, (μ1)(2R)=(μ1)(1R)+(μl1)(2R)+(μ1)(1R)(\mu-1)\left(\dfrac{2}{R}\right)=(\mu-1)\left(\dfrac{1}{-R}\right)+(\mu_{l}-1)\left(\dfrac{2}{R}\right)+(\mu-1)\left(\dfrac{1}{-R}\right)
(μ1)(2R)=(μ1)(2R)+(μl1)(2R)\Rightarrow (\mu-1)\left(\dfrac{2}{R}\right)=(\mu-1)\left(\dfrac{2}{-R}\right)+(\mu_{l}-1)\left(\dfrac{2}{R}\right)
(μ1)(2R)=[(1)(μ1)+(μl1)]×(2R)\Rightarrow (\mu-1)\left(\dfrac{2}{R}\right)=[(-1)(\mu-1)+(\mu_{l}-1)]\times\left(\dfrac{2}{R}\right)
μ1=μ+μl\Rightarrow \mu-1=-\mu+\mu_{l}
2μ=μl+12\mu=\mu_{l}+1
Given μl=3\mu_{l}=3
μ=42=2\mu=\dfrac{4}{2}=2
Thus the refractive index of the lens 22
Hence the answer is B.2B.2

Note:
The lens makers formula as the name suggests is used in the making of the lens. Also clearly, more the refractive index of the lens or combination of lens and liquid, less the focal length. Whereas, the more the radius of curvature of the spherical lens, the more is the focal length of the lens.