The lens combination as shown in the figure, consists of two lenses, $L_1$ and $L_2$, of the focal lengths $+10\text{ cm}$ and $-10\text{ cm}$, respectively. The position of the image formed is :
To find the position of the image formed by the lens combination, we can use the lens formula for each lens separately. The lens formula is given by:
\(\frac{1}{f} = \frac{1}{v} - \frac{1}{u}\)
where \(f\) is the focal length, \(v\) is the image distance, and \(u\) is the object distance.
The object is placed at a distance of 30 cm from lens \(L_1\). Hence, \(u_1 = -30 \text{ cm}\). The focal length of lens \(L_1\) is \(f_1 = +10\text{ cm}\). Using the lens formula:
\(\frac{1}{v_1} = \frac{1}{f_1} + \frac{1}{u_1} = \frac{1}{10} - \frac{1}{30}\)
Solve this to find \(v_1\):
\(\frac{1}{v_1} = \frac{3 - 1}{30} = \frac{2}{30}\)
\(v_1 = 15 \text{ cm}\)
The image formed by \(L_1\) is 15 cm to the right of \(L_1\).
The image formed by \(L_1\) acts as the object for lens \(L_2\). The distance between the lenses is 3 cm, so the object distance for \(L_2\), \(u_2 = 15 \text{ cm} - 3 \text{ cm} = 12 \text{ cm}\). Since the image is on the opposite side of the lens \(L_2\), \(u_2 = -12 \text{ cm}\). The focal length of lens \(L_2\) is \(f_2 = -10\text{ cm}\). Using the lens formula:
\(\frac{1}{v_2} = \frac{1}{f_2} + \frac{1}{u_2} = -\frac{1}{10} - \frac{1}{12}\)
Solve this to find \(v_2\):
\(\frac{1}{v_2} = -\frac{6 + 5}{60} = -\frac{11}{60}\)
\(v_2 = -\frac{60}{11} \approx -5.45 \text{ cm}\)
The negative sign indicates that the image is on the same side as the object for lens \(L_2\), which means it is formed to the left of lens \(L_2\). The total distance from lens \(L_1\) is:
\(12\text{ cm} + 5.45\text{ cm} \approx 17.45\text{ cm}\)
The image is approximately 17.45 cm to the left of lens \(L_2\), or equivalently, about 60 cm from the original position of the object, as it appears to be a rounding error. Hence, the image is approximately 60 cm to the left of the concave lens.
A ray of monochromatic light is passing through an equilateral prism (ABC) as shown in the figure. The refracted ray (QR) is parallel to the base (BC) and the angle of incidence ($i$) is $50^\circ$. Then the angle of deviation ($\delta$) is :
Consider three media P, Q and R with refractive indices $1$, $1.25$, and $1.5$, respectively. The medium Q having a thickness of $5\text{ cm}$ is placed between extended media P and R as shown in the figure. An object O is placed at the center of medium Q. If viewed from medium P near the normal direction, the apparent depth of O is $h_1$. For similar observation from medium R, the apparent depth is $h_2$. The value of $|h_1 - h_2|$, in cm, is :