
STEP 1:-
In order to find the focal length of the concave lens of liquid:
The formula used will be: \(\frac{1}{f}=\frac{1}{f_1}+\frac{1}{f_2}\)
In the absence of the liquid, for the combination of the convex lens and plane mirror, the inverted image coincides with the object only when the object is placed at the focus of the convex lens. The same principle applies when the liquid is introduced between the lens and the mirror. Therefore, the given object or image distance can be considered as the focal length of the respective combinations.
When the liquid is present, the system acts as a combination of a convex lens and a concave lens. Hence, the focal length of the combination is denoted as f (let's say): f = 45 cm
When the liquid is removed, the image is formed at 30 cm.
Therefore, the focal length of the convex lens (f1) is: f1 = 30 cm
Let the focal length of the concave lens with the liquid be f2.
For a pair of optical systems in contact, the equivalent focal length is given by:
\(\frac{1}{f}=\frac{1}{f_1}+\frac{1}{f_2}\)
Putting the values, we get,
\(\frac{1}{45}=\frac{1}{30}+\frac{1}{f_2}\)
\(\frac{1}{f_2}=\frac{1}{45}-\frac{1}{30}\)
\(\frac{1}{f_2}=\frac{2-3}{90}=-\frac{1}{90}\)
\(f_2=-90\text{ cm}\)
STEP 2:-
In order to find the value of radius of curvature:
Lens makers formula: \(\frac{1}{f}=(n_{21}−1)(\frac{1}{R_1}−\frac{1}{R_2})\)
Let the refractive index of the lens be n1,
and the radius of curvature of one surface be R1=R.
The radius of curvature of the other surface is R2=-R.
Using the lens makers formula,
\(\frac{1}{f}=(n_{21}−1)(\frac{1}{R_1}−\frac{1}{R_2})\)
\(\frac{1}{30}=(1.5−1)(\frac{1}{R}−\frac{1}{-R})\)
\(\frac{1}{30}=0.5(\frac{2}{R})\)
\(\frac{1}{30}=\frac{1}{R}\)
\(R=30\text{ cm}\)
STEP 3:-
In order to find the refractive index of the liquid:
Lens makers formula: \(\frac{1}{f}=(n_{21}−1)(\frac{1}{R_1}−\frac{1}{R_2})\)
The radius of curvature of the liquid lens, R'1=-30 cm.
The other side of the liquid is a plane, so R'2=∞.
Let n2 be the refractive index of the liquid.
Using the lens maker's formula,
\(\frac{1}{f_2}=(n_2−1)(\frac{1}{R_1}−\frac{1}{R_2})\)
\(−\frac{1}{90}=(n_2−1)(\frac{1}{-30}−\frac{1}{∞})\)
\(−\frac{1}{90}=−\frac{1}{30}(n_2−1)\)
\(n_2−1=\frac{1}{3}\)
\(n_2=1.33\)
Hence, the refractive index of the liquid is 1.33.
Therefore, the final Answer: n=1.33
A small candle,2.5cm in size is placed at 27cm in front of a concave mirror of radius of curvature 36cm.At what distance from the mirror should a screen be placed in order to obtain a sharp image? Describe the nature and size of the image.If the is moved closer to the mirror, how would the screen have to be moved?
A 4.5cm needle is placed 12cm away from a convex mirror of focal length 15cm. Give the location of the image and the magnification.Describe what happens as the needle is moved farther from the mirror.
A tank is filled with water to a height of 12.5cm. The apparent depth of a needle lying at the bottom of the tank is measured by a microscope to be 9.4cm. What is the refractive index of water? If water is replaced by a liquid of refractive index 1.63 up to the same height, by what distance would the microscope have to be moved to focus on the needle again?

(a)and(b)show the refraction of a ray in air incident at 60° with the normal to a glass-air and water-air interface, respectively. Predict the angle of refraction in glass when the angle of incidence in water is 45° with the normal to a water-glass interface
A small bulb is placed at the bottom of a tank containing water to a depth of 80cm. What is the area of the surface of water through which light from the bulb can emerge? The refractive index of water is 1.33. (Consider the bulb to be a point source.)

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.