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Question: In the figure, light is incident on a thin lens as shown. The radius of curvature for both the surfa...

In the figure, light is incident on a thin lens as shown. The radius of curvature for both the surfaces is R. The focal length of this system is.
A. f=μ3Rμ3μ1f = \dfrac{{{\mu _3}R}}{{{\mu _3} - {\mu _1}}}
B. f=μ2Rμ1μ2f = \dfrac{{{\mu _2}R}}{{{\mu _1} - {\mu _2}}}
C. f=μ3μ2μ1f = \dfrac{{{\mu _3}}}{{{\mu _2} - {\mu _1}}}
D. f=μ1Rμ1μ2f = \dfrac{{{\mu _1}R}}{{{\mu _1} - {\mu _2}}}

Explanation

Solution

The focal length can be defined as the distance between the centre of the lens (as it is a curve in shape) and the focus of it. So here it is given two surfaces, firstly find the refractive index of the first surface and the second surface and then add both to get the focal length.

Complete step by step answer:
Given:
Let the radius of the curvature for the surface is R.
Let the incident of the light one a thin lens isff.
Then the refractive index of the first surface is μ1{\mu _1}.
The refractive index of the second surface is μ2{\mu _2}
The refractive index of the other surface is μ3{\mu _3}
The distance between the image to the first surface of the lens is ν1{\nu _1}
The distance between the image to the second surface of the lens is ν2{\nu _2}
Then the refraction at the first surface involves
μ2{\mu _2},μ1{\mu _1}and ν1{\nu _1}then it can be written as
μ2ν1μ1=μ2μ1R\dfrac{{{\mu _2}}}{{{\nu _1}}} - \dfrac{{{\mu _1}}}{{ - \infty }} = \dfrac{{{\mu _2} - {\mu _1}}}{R}-- (1)
Now, taking the refraction at the second surface, it involvesμ2{\mu _2},μ3{\mu _3},ν1{\nu _1}and ν2{\nu _2}, then the equation will be
μ3ν2μ2ν1=μ3μ2R\dfrac{{{\mu _3}}}{{{\nu _2}}} - \dfrac{{{\mu _2}}}{{{\nu _1}}} = \dfrac{{{\mu _3} - {\mu _2}}}{R}--(2)
Now, adding the both equations 1 and 2, then
μ2ν1μ1+μ3ν2μ2ν1=μ2μ1R+μ3μ2R\dfrac{{{\mu _2}}}{{{\nu _1}}} - \dfrac{{{\mu _1}}}{{ - \infty }} + \dfrac{{{\mu _3}}}{{{\nu _2}}} - \dfrac{{{\mu _2}}}{{{\nu _1}}} = \dfrac{{{\mu _2} - {\mu _1}}}{R} + \dfrac{{{\mu _3} - {\mu _2}}}{R}
Now solving the above equation we will get
μ3ν2μ3μ1R\dfrac{{{\mu _3}}}{{{\nu _2}}} - \dfrac{{{\mu _3} - {\mu _1}}}{R}
ν2=Rμ3μ3μ1{\nu _2} = \dfrac{{R{\mu _3}}}{{{\mu _3} - {\mu _1}}}
Here, ν2{\nu _2}will be the focal length then, replacing the ν2{\nu _2}asff, then the equation becomes
f=Rμ3μ3μ1f = \dfrac{{R{\mu _3}}}{{{\mu _3} - {\mu _1}}}
Therefore, the focal length of the system isf=Rμ3μ3μ1f = \dfrac{{R{\mu _3}}}{{{\mu _3} - {\mu _1}}}

So, the correct answer is “Option A”.

Note:
here we have to take the ratios of the refracting length and the focal length in the both surfaces. So remember this while taking those ratios. While adding the both equations, do not confuse between the focal length and the refractive index.