The collision frequency (\( Z \)) is given by:
\( Z = n \pi d^2 v_{avg} \)
where \( n \) is the number of molecules per unit volume, \( d \) is the diameter of the molecules, and \( v_{avg} \) is the average speed.
Let \( Z_1 \) and \( Z_2 \) be the collision frequencies before and after the increase in the number of molecules, respectively. Let \( n_1 \) and \( n_2 \) be the corresponding number densities. Since the diameter and average speed of the molecules remain constant, we can write:
\( \frac{Z_1}{Z_2} = \frac{n_1 \pi d^2 v_{avg}}{n_2 \pi d^2 v_{avg}} = \frac{n_1}{n_2} \)
Given \( n_1 = 3 \times 10^{19} \) and \( n_2 = 12 \times 10^{19} \):
\( \frac{Z_1}{Z_2} = \frac{3 \times 10^{19}}{12 \times 10^{19}} = \frac{3}{12} = \frac{1}{4} = 0.25 \)
The ratio of collision frequencies before and after the increase is 0.25 (Option 1).
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 \( 4.606 \times 10^{-2} \text{ s}^{-1} \).