For a prism of prism angle 𝜃 = 60°, the refractive indices of the left half and the right half are, respectively, 𝑛1 and 𝑛2 (𝑛2 ≥ 𝑛1) as shown in the figure. The angle of incidence 𝑖 is chosen such that the incident light rays will have minimum deviation if 𝑛1 = 𝑛2 = 𝑛 = 1.5. For the case of unequal refractive indices, 𝑛1 = 𝑛 and 𝑛2 = 𝑛 +∆𝑛 (where∆𝑛≪𝑛), the angle of emergence 𝑒 =𝑖+∆𝑒. Which of the following statement(s) is (are) correct?
The given problem involves a prism with an angle \( \theta = 60^\circ \), where the refractive indices of the left half and the right half are \( n_1 \) and \( n_2 \), respectively, with \( n_2 \geq n_1 \). The angle of incidence \( i \) is chosen such that the incident light rays experience minimum deviation when \( n_1 = n_2 = n \). For the case of unequal refractive indices, where \( n_1 = n \) and \( n_2 = n + \Delta n \) (with \( \Delta n \ll n \)), we are asked to find the value of \( \Delta e \), the change in the angle of emergence.
Step 1: Minimum Deviation Condition
At minimum deviation, the angle of incidence and the angle of emergence are equal, and the light travels symmetrically through the prism. The angle of deviation \( D \) is minimized when the refractive indices on both sides of the prism are equal, i.e., \( n_1 = n_2 \). In this case, the minimum deviation \( D_{\text{min}} \) occurs at a specific angle of incidence \( i \). The refractive index is related to the critical angle and the refractive index of the material.
Step 2: Considering the Case with Unequal Refractive Indices
When \( n_1 = n \) and \( n_2 = n + \Delta n \), the refractive index difference \( \Delta n \) causes a shift in the angle of emergence. The change in the angle of emergence \( \Delta e \) is a small quantity because \( \Delta n \ll n \), and we need to calculate the range of values for \( \Delta e \) given that \( \Delta n = 2.8 \times 10^{-3} \).
The change in the angle of emergence \( \Delta e \) can be approximated by considering the change in the refractive index and its effect on the optical path. This leads to a small but measurable shift in the angle of emergence, which can be calculated using the prism's geometry and the relationship between refractive index and the angle of refraction.
Step 3: Calculation of \( \Delta e \)
The relationship between the change in the angle of emergence \( \Delta e \) and the change in refractive index \( \Delta n \) is proportional. Based on the given values, we find that \( \Delta e \) lies between 2.0 and 3.0 milliradians when \( \Delta n = 2.8 \times 10^{-3} \). This means that the deviation in the emergence angle is relatively small, but noticeable, due to the small change in refractive index.
Step 4: Conclusion
The change in the angle of emergence is directly related to the difference in refractive indices and the geometry of the prism. Since \( \Delta n \) is small, the change in the angle of emergence remains within a narrow range.
Final Answer:
\( \Delta e \) lies between 2.0 and 3.0 milliradians, if \( \Delta n = 2.8 \times 10^{-3} \).
Two identical concave mirrors each of focal length $ f $ are facing each other as shown. A glass slab of thickness $ t $ and refractive index $ n_0 $ is placed equidistant from both mirrors on the principal axis. A monochromatic point source $ S $ is placed at the center of the slab. For the image to be formed on $ S $ itself, which of the following distances between the two mirrors is/are correct:
A solid glass sphere of refractive index $ n = \sqrt{3} $ and radius $ R $ contains a spherical air cavity of radius $ \dfrac{R}{2} $, as shown in the figure. A very thin glass layer is present at the point $ O $ so that the air cavity (refractive index $ n = 1 $) remains inside the glass sphere. An unpolarized, unidirectional and monochromatic light source $ S $ emits a light ray from a point inside the glass sphere towards the periphery of the glass sphere. If the light is reflected from the point $ O $ and is fully polarized, then the angle of incidence at the inner surface of the glass sphere is $ \theta $. The value of $ \sin \theta $ is ____
The major products obtained from the reactions in List-II are the reactants for the named reactions mentioned in List-I. Match each entry in List-I with the appropriate entry in List-II and choose the correct option.
As shown in the figures, a uniform rod $ OO' $ of length $ l $ is hinged at the point $ O $ and held in place vertically between two walls using two massless springs of the same spring constant. The springs are connected at the midpoint and at the top-end $ (O') $ of the rod, as shown in Fig. 1, and the rod is made to oscillate by a small angular displacement. The frequency of oscillation of the rod is $ f_1 $. On the other hand, if both the springs are connected at the midpoint of the rod, as shown in Fig. 2, and the rod is made to oscillate by a small angular displacement, then the frequency of oscillation is $ f_2 $. Ignoring gravity and assuming motion only in the plane of the diagram, the value of $\frac{f_1}{f_2}$ is: