The relationship between \(K_p\) and \(K_c\) is given by:
\[ K_p = K_c \cdot (RT)^{\Delta n_g} \]
For the reaction \( \text{N}_2\text{O}_4(g) \leftrightharpoons 2\text{NO}_2(g) \), the change in the number of moles of gas (\(\Delta n_g\)) is calculated as:
\[ \Delta n_g = 2 - 1 = 1 \]
Rearranging the formula to solve for \(K_c\) and substituting the given values:
\[ K_c = \frac{K_p}{RT} = \frac{0.492}{0.082 \times 300} = 2 \times 10^{-2} \]
Thus, \(K_c\) is $2 \times 10^{-2}$.
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?
