
Given: \( \sin 60^\circ = \frac{4}{3} \sin r \)
Then:
\( \sin r = \frac{3}{4} \times \frac{\sqrt{3}}{2} = \frac{3\sqrt{3}}{8} \qquad (i) \)
\( \cos r = \sqrt{1 - \frac{27}{64}} = \sqrt{\frac{37}{64}} = \frac{\sqrt{37}}{8} \approx 0.75 \)
\( \tan r = \sqrt{\frac{27}{37}} \)
\( \frac{x}{1.5} = 0.85 \)
\( x = 0.85 \times 1.5 = 1.275 \text{ m} \)
\( \tan 30^\circ = \frac{y}{2.15 - 1.275} = 0.50 \)
\( y = \frac{0.875}{1.732} = 0.50 \)
So, the length of the pole above the water surface = \( \mathbf{0.50 \text{ m} = 50 \text{ cm}} \).
Snell’s Law relates the angle of incidence (\(i\)) and angle of refraction (\(r\)) for light passing through two different media with refractive indices \(n_1\) and \(n_2\):
\( n_1 \sin i = n_2 \sin r \)
In this case: - \( n_1 = 1 \) (air), - \( i = 60^\circ \) (since the angle with the surface is 30°), - \( n_2 = \frac{4}{3} \) (water).
Using Snell’s law:
\( \sin 60^\circ = \frac{4}{3} \sin r \)
Solving for \( \sin r \):
\( \sin r = \frac{3}{4} \sin 60^\circ = \frac{3}{4} \times \frac{\sqrt{3}}{2} = \frac{3\sqrt{3}}{8} \)
We first find \( \cos r \):
\( \cos r = \sqrt{1 - \sin^2 r} = \sqrt{1 - \left(\frac{3\sqrt{3}}{8}\right)^2} = \sqrt{1 - \frac{27}{64}} = \sqrt{\frac{37}{64}} = \frac{\sqrt{37}}{8} \)
Now we calculate \( \tan r \):
\( \tan r = \frac{\sin r}{\cos r} = \frac{3\sqrt{3}/8}{\sqrt{37}/8} = \frac{3\sqrt{3}}{\sqrt{37}} \approx 0.85 \)
Let \( x \) be the horizontal length of the shadow. We have \( \tan r = \frac{x}{1.5 \, \text{m}} \), where 1.5 m is the depth of the water.
Thus:
\( x = 1.5 \times \tan r = 1.5 \times 0.85 = 1.275 \, \text{m} \)
Since the total length of the shadow is 2.15 m, the horizontal distance from the pole to the point where light enters the water is:
\( 2.15 - 1.275 = 0.875 \, \text{m} \)
Let \( y \) be the height of the pole above the water. Since the angle of incidence is 30° with the water surface, we have:
\( \tan 30^\circ = \frac{y}{0.875} \)
Solving for \( y \):
\( y = 0.875 \times \tan 30^\circ = 0.875 \times \frac{1}{\sqrt{3}} \approx 0.875 \times 0.577 = 0.50 \, \text{m} = 50 \, \text{cm} \)
The height of the pole above the water surface is \( \mathbf{50 \, \text{cm}} \).
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,


A convex mirror of radius of curvature 30 cm forms an image that is half the size of the object. The object distance is:
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 : \(A_2 \rightleftharpoons 2A\)