Heat transfer in the constant-pressure expansion: Q1 = 654 Btu & Heat transfer in the isothermal compression: Q2 = -72 Btu
Process 1: Constant-Pressure Expansion
Work Done (W1):
For a constant-pressure process, work is calculated as: W1 = P(V2 - V1)
We need to find the pressure (P).
Use the steam tables to determine the specific volume (v1) at the initial state (350°F, 71.7 ft³).
v1 = 23.9 ft³/lb (from steam tables)
P = mRT/V1
= 3 lb * 0.5956 Btu/lb·°R * (350 + 460)°R / 71.7 ft³
= 45.5 psia
W1 = 45.5 psia * (85.38 ft³ - 71.7 ft³)
= 654 Btu
Heat Transfer (Q1):
Apply the first law of thermodynamics: Q1 - W1 = ΔU1
For an ideal gas, internal energy change (ΔU) depends only on temperature change. Since the process is isothermal, ΔU1 = 0.
Therefore, Q1 = W1 = 654 Btu
Process 2: Isothermal Compression
Heat Transfer (Q2):
For an isothermal process, ΔU2 = 0.
Applying the first law: Q2 - W2 = ΔU2
Q2 = W2 = -72 Btu (negative because work is done on the system)