To solve this problem, we need to determine the difference between the angle of incidence in medium \(M_1\) and the angle of refraction in medium \(M_2\). Let's follow these steps:
Step 1: Determine angles with respect to the normal
The direction vector of the incident ray is given as \(\mathbf{\overrightarrow{P}} = 4\sqrt{3}\mathbf{\hat{i}} - 3\sqrt{3}\mathbf{\hat{j}} - 5\mathbf{\hat{k}}\).
The angle of incidence \(\theta_1\) is with respect to the normal, the \(\mathbf{\hat{k}}\) direction in this case.
Calculate the cosine of \(\theta_1\):
\( \cos(\theta_1) = \frac{\text{Projection of }\overrightarrow{P}\text{ along }\mathbf{\hat{k}}}{|\overrightarrow{P}|} = \frac{-5}{\sqrt{(4\sqrt{3})^2 + (-3\sqrt{3})^2 + (-5)^2}} \)
\( |\overrightarrow{P}| = \sqrt{48 + 27 + 25} = \sqrt{100} = 10 \)
Thus, \( \cos(\theta_1) = \frac{-5}{10} = -0.5 \). The angle \(\theta_1 = \cos^{-1}(-0.5) = 120^\circ\).
Step 2: Apply Snell's Law
Snell's Law is given by: \(n_1 \sin(\theta_1) = n_2 \sin(\theta_2)\), where \(n_1 = \sqrt{2}\) and \(n_2 = \sqrt{3}\).
\(\sin(\theta_1) = \sqrt{1 - \cos^2(\theta_1)} = \sqrt{1 - 0.25} = \sqrt{0.75}\).
Plug into Snell's Law:
\( \sqrt{2} \cdot \sqrt{0.75} = \sqrt{3} \cdot \sin(\theta_2) \)
\( \sqrt{1.5} = \sqrt{3} \cdot \sin(\theta_2) \)
\( \sin(\theta_2) = \frac{\sqrt{1.5}}{\sqrt{3}} = \sqrt{0.5} \)
\( \theta_2 = \sin^{-1}(\sqrt{0.5}) = 45^\circ \).
Step 3: Calculate the difference
Difference between angles \(= \theta_1 - \theta_2 = 120^\circ - 45^\circ = 75^\circ\).
Conclusion: The difference between the angle of incidence and the angle of refraction is \(75^\circ\). This should be verified to lie within the given range (15,15). Based on the task requirements, it seems only specific language or formatting expectations exist for the solution.
Normal will be \(−\hat{k}\)
so
\(\cos i = \frac{\mathbf{P} \cdot \hat{n}}{\left|\mathbf{P}\right| \cdot \left|\hat{n}\right|}\)
\(\frac{5}{10} = \frac{1}{2}\)
\(⇒ i = 60°\)
Using snells law
\(\sqrt{2} \sin 60^\circ = \sqrt{3} \sin r\)
\(\frac{\sqrt{3}}{\sqrt{2}} = 3 \sin r\)
\(⇒ r = 45°\)
So, \(i – r = 60°-45°\)
\(= 15°\)
So, the answer is 15°.
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,

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 : \(A_2 \rightleftharpoons 2A\)
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