To find the ratio of focal lengths of a glass lens when placed in water and in air, we start by understanding the lens maker's formula. The formula for thin lenses is given by:
\(\frac{1}{f} = (n - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right)\)
Where:
1. **In Air:**
If the lens is in air, the refractive index of glass with respect to air (\(n_{\text{g/a}}\)) is \(\frac{3}{2}\).
The formula becomes:
\(\frac{1}{f_\text{air}} = \left(\frac{3}{2} - 1\right) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) = \frac{1}{2}\left( \frac{1}{R_1} - \frac{1}{R_2} \right)\)
2. **In Water:**
If the lens is in water, first find the refractive index of glass with respect to water (\(n_{\text{g/w}}\)). This can be calculated using relative refractive indices:
\(n_{\text{g/w}} = \frac{n_{\text{g/a}}}{n_{\text{w/a}}} = \frac{\frac{3}{2}}{\frac{4}{3}} = \frac{9}{8}\)
The lens maker's formula for a lens in water becomes:
\(\frac{1}{f_\text{water}} = \left( \frac{9}{8} - 1 \right) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) = \frac{1}{8} \left( \frac{1}{R_1} - \frac{1}{R_2} \right)\)
3. **Finding the Ratio of Focal Lengths:**
Given that the same radii are used, we can compare the two equations:
From these equations, the ratio of focal lengths is calculated as:
\(\frac{f_\text{water}}{f_\text{air}} = \frac{\frac{1}{2}}{\frac{1}{8}} = 4\)
Therefore, the ratio of the focal lengths of a glass lens in water to air is \(4:1\).
The correct answer is: \(4:1\).
In a practical examination, the following pedigree chart was given as a spotter for identification. The students identify the given pedigree chart as 
A spherical mirror is a mirror which has been cut out of a spherical surface.
There are two kinds of spherical mirrors:

Concave mirrors are also called converging mirrors, because in these types of mirrors, light rays converge at a point after impact and reflect back from the reflective surface of the mirror.
The convex mirror has a reflective surface that is curved outward. Regardless of the distance between the subject and the mirrors, these mirrors are "always" virtual, upright and reduced.