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: \(\sqrt{2} : 1\).
The strain-stress plot for materials A, B, C and D is shown in the figure. Which material has the largest Young's modulus? 
MX is a sparingly soluble salt that follows the given solubility equilibrium at 298 K.
MX(s) $\rightleftharpoons M^{+(aq) }+ X^{-}(aq)$; $K_{sp} = 10^{-10}$
If the standard reduction potential for $M^{+}(aq) + e^{-} \rightarrow M(s)$ is $(E^{\circ}_{M^{+}/M}) = 0.79$ V, then the value of the standard reduction potential for the metal/metal insoluble salt electrode $E^{\circ}_{X^{-}/MX(s)/M}$ is ____________ mV. (nearest integer)
[Given : $\frac{2.303 RT}{F} = 0.059$ V]
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :
