Concept:
According to the First Law of Thermodynamics for a closed system undergoing a non-cyclic process, the net heat interactions ($Q$) equal the sum of the change in internal energy ($\Delta U$) and the work performed ($W$):
\[
Q = \Delta U + W
\]
For a quasi-static displacement process operating under constant pressure conditions (isobaric process), the boundary work output ($W$) is given by the integral of pressure over volume:
\[
W = \int P \, dV = P(V_2 - V_1)
\]
By evaluating the boundary work and employing the first law, we can isolate the net internal energy alteration.
Step 1: Extract parameters and equalize metric prefixes to standard SI base units.
The parameters given in the problem statement are:
• Constant Pressure, \(P = 1 \text{ MPa} = 1 \times 10^6 \text{ N/m}^2\)
• Initial Volume, \(V_1 = 0.03 \text{ m}^3\)
• Final Volume, \(V_2 = 0.06 \text{ m}^3\)
• Heat absorbed by the system, \(Q = +84 \text{ kJ} = 84 \times 10^3 \text{ J}\)
Step 2: Calculate the boundary work performed during expansion.
Using the constant-pressure work equation:
\[
W = P \times (V_2 - V_1)
\]
Substitute the values:
\[
W = (1 \times 10^6 \text{ Pa}) \times (0.06 \text{ m}^3 - 0.03 \text{ m}^3)
\]
\[
W = 1 \times 10^6 \times 0.03 = 30000 \text{ J}
\]
Converting Joules to kilojoules gives:
\[
W = \frac{30000}{1000} \text{ kJ} = 30 \text{ kJ}
\]
Step 3: Solve for the change in internal energy (\(\Delta U\)) via the First Law.
Rearranging the first law equation to solve for $\Delta U$:
\[
\Delta U = Q - W
\]
Substituting our calculated heat interaction and boundary work values:
\[
\Delta U = 84 \text{ kJ} - 30 \text{ kJ} = 54 \text{ kJ}
\]
Thus, the change in internal energy of the gas mixture is equal to 54 kJ, corresponding to Option (B).