Step 1: First Law for Isobaric Process. For a process at constant pressure (isobaric), the heat supplied \(\Delta Q\) is related to the internal energy change \(\Delta U\) and work done \(W\) by the equation \(\Delta Q = \Delta U + W\).
Step 2: Defining the Molar Heat Capacities. For a diatomic gas:
1. Molar heat capacity at constant volume \(C_v = \frac{5}{2}R\). 2. Molar heat capacity at constant pressure \(C_p = C_v + R = \frac{7}{2}R\).
Step 3: Expressing Thermodynamic Quantities. 1. \(\Delta Q = n C_p \Delta T = n(\frac{7}{2}R)\Delta T\). 2. \(\Delta U = n C_v \Delta T = n(\frac{5}{2}R)\Delta T\). 3. \(W = P \Delta V = n R \Delta T\).
Step 4: Calculating the Ratio. The ratio \(\Delta Q : \Delta U : W\) is:
\[\frac{7}{2}nR\Delta T : \frac{5}{2}nR\Delta T : nR\Delta T\]
Dividing by \(nR\Delta T\) and multiplying by 2, we get 7 : 5 : 2.

One mole each of \(A_2(g)\) and \(B_2(g)\) are taken in a 1 L closed flask and allowed to establish the equilibrium at 500 K: \(A_{2}(g)+B_{2}(g) \rightleftharpoons 2AB(g)\). The value of x (missing enthalpy of \(B_2\) or related parameter) is ______ . (Nearest integer)}