\(K_2\) = \(\frac{1}{K_1}\)
K2 = \(K^2_1\)
K2 = \(K^1_2\)
K2 = \(\frac{1}{K^2_1}\)
To solve the problem of determining the relationship between the equilibrium constants \(K_1\) and \(K_2\) for the given chemical equilibria, we need to understand how these constants relate to each other based on the provided reactions.
The first equilibrium is given by:
NO_{(g)} + \bigg(\frac{1}{2}\bigg)O_{2(g)} \rightleftharpoons NO_{2(g)}\quad \text{with equilibrium constant}\, K_1
The second equilibrium is given by:
2NO_{2(g)} \rightleftharpoons 2NO_{(g)} + O_{2(g)} \quad \text{with equilibrium constant}\, K_2
To find the relationship between \(K_1\) and \(K_2\), we need to analyze how the second reaction is related to the first one. Notice that the second reaction is essentially the reverse of the first reaction, but with coefficients multiplied by 2:
The reverse of the first reaction with doubled coefficients is:
2NO_{2(g)} \rightleftharpoons 2NO_{(g)} + O_{2(g)}\quad \text{which is the same as the second reaction given}
The relationship between the equilibrium constants for the reverse reactions is:
(K_1)^{-1} when reversed and squared when doubled (as coefficients are doubled):
K_2 = \frac{1}{K_1^2}
Thus, the relationship is established as:
K_2 = \frac{1}{K_1^2}
This aligns with the given correct answer.
An ideal massless spring \( S \) can be compressed \( 1 \) m by a force of \( 100 \) N in equilibrium. The same spring is placed at the bottom of a frictionless inclined plane inclined at \( 30^\circ \) to the horizontal. A \( 10 \) kg block \( M \) is released from rest at the top of the incline and is brought to rest momentarily after compressing the spring by \( 2 \) m. If \( g = 10 \) m/s\( ^2 \), what is the speed of the mass just before it touches the spring?
