Given: - Wavelength of light: \( \lambda = 5000 \, \text{\AA} = 5000 \times 10^{-10} \, \text{m} \) - Distance between slits: \( d = 1.0 \, \text{mm} = 1.0 \times 10^{-3} \, \text{m} \) - Distance between the slits and the screen: \( D = 1.0 \, \text{m} \)
The fringe width \( \beta \) in Young’s double-slit experiment is given by:
\[ \beta = \frac{\lambda D}{d} \]
Substituting the given values:
\[ \beta = \frac{5000 \times 10^{-10} \times 1.0}{1.0 \times 10^{-3}} \, \text{m} \] \[ \beta = 5 \times 10^{-3} \, \text{m} = 5 \, \text{mm} \]
The intensity becomes half of the maximum intensity at the position of the first secondary maximum. The position \( y \) where this occurs is given by:
\[ y = \frac{\beta}{4} \]
Substituting the value of \( \beta \):
\[ y = \frac{5 \times 10^{-3}}{4} \, \text{m} \] \[ y = 1.25 \times 10^{-3} \, \text{m} = 125 \times 10^{-6} \, \text{m} \]
The distance from the centre of the screen where the intensity becomes half of the maximum intensity for the first time is \( 125 \times 10^{-6} \, \text{m} \).
Let \[ I(x) = \int \frac{dx}{(x-11)^{\frac{11}{13}} (x+15)^{\frac{15}{13}}} \] If \[ I(37) - I(24) = \frac{1}{4} \left( b^{\frac{1}{13}} - c^{\frac{1}{13}} \right) \] where \( b, c \in \mathbb{N} \), then \[ 3(b + c) \] is equal to:
For the thermal decomposition of \( N_2O_5(g) \) at constant volume, the following table can be formed, for the reaction mentioned below: \[ 2 N_2O_5(g) \rightarrow 2 N_2O_4(g) + O_2(g) \] Given: Rate constant for the reaction is \( 4.606 \times 10^{-2} \text{ s}^{-1} \).