To find the refractive index of the lens material, we can use the Lens Maker's Formula, which relates the focal length of a lens to the refractive index of the material and the radii of curvature:
\(\frac{1}{f} = \left(n - 1\right) \left(\frac{1}{R_1} - \frac{1}{R_2}\right)\)
where:
Given:
Now, substitute the values into the lens maker's formula:
\(\frac{1}{12} = \left(n - 1 \right) \left(\frac{1}{10} - \frac{1}{-15}\right)\)
Simplifying the terms inside the parentheses:
\(\frac{1}{10} - \left(-\frac{1}{15}\right) = \frac{1}{10} + \frac{1}{15}\)
To combine these fractions, find a common denominator (30):
\(\frac{3}{30} + \frac{2}{30} = \frac{5}{30} = \frac{1}{6}\)
Substitute back into the formula:
\(\frac{1}{12} = \left(n - 1\right) \frac{1}{6}\)
Multiplying both sides by 6 to solve for \(n - 1\):
\(\frac{6}{12} = n - 1\)
\(\frac{1}{2} = n - 1\)
Add 1 to both sides:
\(n = \frac{1}{2} + 1 = \frac{3}{2} = 1.5\)
Therefore, the refractive index of the lens material is 1.5. This matches with Option 3.
Light from a point source in air falls on a spherical glass surface (refractive index, \( \mu = 1.5 \) and radius of curvature \( R = 50 \) cm). The image is formed at a distance of 200 cm from the glass surface inside the glass. The magnitude of distance of the light source from the glass surface is 1cm.

Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
An organic compound (X) with molecular formula $\mathrm{C}_{3} \mathrm{H}_{6} \mathrm{O}$ is not readily oxidised. On reduction it gives $\left(\mathrm{C}_{3} \mathrm{H}_{8} \mathrm{O}(\mathrm{Y})\right.$ which reacts with HBr to give a bromide (Z) which is converted to Grignard reagent. This Grignard reagent on reaction with (X) followed by hydrolysis give 2,3-dimethylbutan-2-ol. Compounds (X), (Y) and (Z) respectively are: