Reaction:
\[ A(g) \rightleftharpoons B(g) + \frac{1}{2} C(g) \]
Step 1: Initial Moles
Initial moles: \[ n_A = n, \quad n_B = 0, \quad n_C = 0 \]
Step 2: Equilibrium Moles
Equilibrium moles: \[ n_A = n(1 - \alpha), \quad n_B = n\alpha, \quad n_C = \frac{n\alpha}{2} \]
Step 3: Total Moles at Equilibrium
Total moles: \[ n_{\text{total}} = n\left(1 + \alpha\right)/2 \]
Step 4: Equilibrium Partial Pressures
Partial pressure of each component at equilibrium: \[ P_A = \frac{(1 - \alpha)P}{1 + \alpha/2}, \quad P_B = \frac{\alpha P}{1 + \alpha/2}, \quad P_C = \frac{(\alpha/2) P}{1 + \alpha/2} \]
Step 5: Equilibrium Constant \( K_p \) Expression
The equilibrium constant \( K_p \) is defined as: \[ K_p = \frac{P_B \cdot P_C^{1/2}}{P_A} = \frac{\alpha P}{1 + \alpha/2} \times \left( \frac{(\alpha/2) P}{1 + \alpha/2} \right)^{1/2} \]
Step 6: Simplification of \( K_p \) Expression
Simplified expression for \( K_p \): \[ K_p = \frac{\alpha P}{1 + \alpha/2} \times \left( \frac{\alpha P^{1/2}}{2^{1/2} (1 + \alpha/2)^{1/2}} \right) = \frac{\alpha^{3/2} P^{3/2}}{2^{1/2} (1 + \alpha/2)^{3/2}} \]
Final Expression for \( K_p \):
The final simplified expression for \( K_p \) is: \[ K_p = \frac{\alpha^{3/2} P^{1/2}}{(2 + \alpha)^{1/2} (1 - \alpha)} \]
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?
