To find the width of the slit in a single slit diffraction pattern, we can use the formula for the position of minima: \(a \sin \theta = n\lambda\), where \(a\) is the slit width, \(\theta\) is the diffraction angle, \(n\) is the order of the minima, and \(\lambda\) is the wavelength of light. For small angles, \(\sin \theta \approx \tan \theta = \frac{y}{D}\), where \(y\) is the distance of the minima from the central maximum on the screen, and \(D\) is the distance from the slit to the screen.
The distance between the first (\(n=1\)) and third (\(n=3\)) minima is given as 3 mm. Using the positions of the minima: \(y_1 = \frac{\lambda D}{a}\) and \(y_3 = \frac{3\lambda D}{a}\).
The difference is: \(y_3 - y_1 = \frac{3\lambda D}{a} - \frac{\lambda D}{a} = \frac{2\lambda D}{a}\).
Equating this to the given distance: \(\frac{2\lambda D}{a} = 3 \, \text{mm} = 0.003 \, \text{m}\).
Substitute \( \lambda = 6000 \, \text{Å} = 6000 \times 10^{-10} \, \text{m}\) and \(D = 50 \, \text{cm} = 0.5 \, \text{m}\):
\(a = \frac{2 \cdot 6000 \times 10^{-10} \cdot 0.5}{0.003}\).
\(a = \frac{6000 \times 10^{-10}}{0.003} = 2 \times 10^{-4} \, \text{m}\).
Thus, the width of the slit is \(2 \times 10^{-4} \, \text{m}\), fitting well within the specified range [2,2].
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 : \(A_2 \rightleftharpoons 2A\)