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 \( \Delta n = 2.8 \times 10^{-3} \).
A hemispherical vessel is completely filled with a liquid of refractive index \( \mu \). A small coin is kept at the lowest point \( O \) of the vessel as shown in the figure. The minimum value of the refractive index of the liquid so that a person can see the coin from point \( E \) (at the level of the vessel) is:
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.