In thermodynamics, the first law states that the change in internal energy of a system, ΔU, is equal to the heat added to the system, Q, minus the work done by the system, W. Mathematically, this is expressed as ΔU = Q - W.
We analyze the given processes as follows:
For process 1-2:
Heat absorbed, Q1-2 = 150 kJ
Work done by the system, W1-2 = 90 kJ
Change in internal energy, ΔU1-2 = Q1-2 - W1-2 = 150 kJ - 90 kJ = 60 kJ
For process 2-3:
Work done on the system, W2-3 = -80 kJ (since work is done on the system, it's negative)
Heat rejected, Q2-3 = -60 kJ (as it's rejected, it's negative)
Change in internal energy, ΔU2-3 = Q2-3 - W2-3 = -60 kJ - (-80 kJ) = 20 kJ
Total change from state 1 to state 3:
ΔU1-3 = ΔU1-2 + ΔU2-3 = 60 kJ + 20 kJ = 80 kJ
For an adiabatic process (no heat exchange, Q = 0) from state 3 back to state 1:
ΔU3-1 = Q3-1 - W3-1 = 0 - W3-1
Since the total change in internal energy around the full cycle must be zero, ΔU1-3 + ΔU3-1 = 0, it follows that:
80 kJ - W3-1 = 0
W3-1 = 80 kJ
Thus, the work interaction needed to restore the system to the initial state by an adiabatic path is 80 kJ.