To solve this question, we need to find the ratio of the refractive indices of the two media given the critical angle of incidence. The critical angle (\( \theta_c \)) for a pair of optical media is the angle of incidence in the denser medium for which the angle of refraction is \( 90^\circ \) in the rarer medium. Using Snell's Law, which states:
\(n_1 \sin \theta_c = n_2 \sin 90^\circ\)
Where:
Given that the critical angle \( \theta_c = 45^\circ \), and \(\sin 90^\circ = 1\), the equation becomes:
\(n_1 \sin 45^\circ = n_2\)
We know \(\sin 45^\circ = \frac{\sqrt{2}}{2}\). Therefore:
\(n_1 \frac{\sqrt{2}}{2} = n_2\)
Rearrange to find the ratio of refractive indices:
\(\frac{n_1}{n_2} = \sqrt{2}\)
Hence, the refractive indices ratio is \( \sqrt{2} : 1 \). This matches the correct given option \(\sqrt{2} : 1\).
Let's analyze why the other options are incorrect:
The critical angle is given by:
\[ \sin C = \frac{n_2}{n_1}. \]
At \( C = 45^\circ \):
\[ \sin 45^\circ = \frac{1}{\sqrt{2}} = \frac{n_2}{n_1}. \]
Thus:
\[ \frac{n_1}{n_2} = \sqrt{2} : 1. \]
Final Answer: \(\sqrt{2} : 1\).
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

In an experiment to measure the focal length (f) of a convex lens, the magnitude of object distance (x) and the image distance (y) are measured with reference to the focal point of the lens. The y-x plot is shown in figure.
The focal length of the lens is_____cm.

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)