At a given temperature and pressure, the equilibrium constant values for the equilibria are given below:
$ 3A_2 + B_2 \rightleftharpoons 2A_3B, \, K_1 $
$ A_3B \rightleftharpoons \frac{3}{2}A_2 + \frac{1}{2}B_2, \, K_2 $
The relation between $ K_1 $ and $ K_2 $ is:
To find the relation between the equilibrium constants \( K_1 \) and \( K_2 \), let's analyze the given equilibrium reactions.
The first equilibrium given is:
\(3A_2 + B_2 \rightleftharpoons 2A_3B, \, K_1\)
This means that for the above reaction, the equilibrium constant is \( K_1 \).
The second equilibrium is the reverse of this to some extent:
\(A_3B \rightleftharpoons \frac{3}{2}A_2 + \frac{1}{2}B_2, \, K_2\)
This reaction is essentially the reverse of the formation of \( A_3B \) with half of the quantities from the initial equilibrium.
To relate \( K_1 \) and \( K_2 \), let's write out their expressions:
Since the second reaction is the reverse half of the first, we calculate the relation using their inverses and powers:
The inverse of the first equilibrium (the reverse reaction) would have the constant \( \frac{1}{K_1} \). Since the coefficients are halved in the second reaction, the constants' relation involves a square root due to the balance of moles:
The correct relationship can be expressed as: \(K_2 = \frac{1}{\sqrt{K_1}}\)
Therefore, the correct option is: \(K_2 = \frac{1}{\sqrt{K_1}}\)
For the reaction A(g) $\rightleftharpoons$ 2B(g), the backward reaction rate constant is higher than the forward reaction rate constant by a factor of 2500, at 1000 K.
[Given: R = 0.0831 atm $mol^{–1} K^{–1}$]
$K_p$ for the reaction at 1000 K is: