To solve this problem, we'll use the First Law of Thermodynamics, which is given by:
\Delta U = Q - W
where:
Let's analyze each step of the process given in the question:
The work done on the gas during this constant pressure compression is calculated as:
W = P \cdot \Delta V = P \cdot (V_{\text{final}} - V_{\text{initial}})
Substitute the given values:
W = 100 \, N/m^2 \times (1 \, m^3 - 2 \, m^3) = 100 \times (-1) = -100 \, J
Here, the work done is negative because the volume decreases, meaning work is done on the gas.
Thus, the heat added to the gas Q = 150 \, J.
Substitute Q and W into the First Law of Thermodynamics:
\Delta U = Q - W = 150 \, J - (-100 \, J)
\Delta U = 150 \, J + 100 \, J = 250 \, J
Therefore, the internal energy of the gas increases by 250 \, J.
Conclusion: The correct answer is that the internal energy of the gas increases by 250 J.
A real gas within a closed chamber at \( 27^\circ \text{C} \) undergoes the cyclic process as shown in the figure. The gas obeys the equation \( PV^3 = RT \) for the path A to B. The net work done in the complete cycle is (assuming \( R = 8 \, \text{J/molK} \)):
