A convex lens made of glass of μ=1.5 has a focal length f in air. When it is completely immersed in a liquid of μ=2 its focal length and nature will be:
A
2f, converging
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B
3f, converging
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C
2f, diverging
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D
3f, diverging
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Solution
The correct option is C2f, diverging Let k=1R1−1R2
So, 1f=(μ−1)k
or, 1f=(32−1)k
or, k=2f Also, in another medium, 1f′=(1.52−1)k Thus, putting k=2f, we get: f′=−2f