Given:
- Process 1–2: Heat absorbed \( Q_{1-2} = 150 \, {kJ} \), Work done \( W_{1-2} = 90 \, {kJ} \)
- Process 2–3: Work done on system \( W_{2-3} = -80 \, {kJ} \), Heat rejected \( Q_{2-3} = -60 \, {kJ} \)
- Process 3–1: Adiabatic process (no heat exchange)
From the first law of thermodynamics:
\[
\Delta U = Q - W
\]
For process 1–2:
\[
\Delta U_{1-2} = 150 - 90 = 60 \, {kJ}
\]
For process 2–3:
\[
\Delta U_{2-3} = -60 - (-80) = 20 \, {kJ}
\]
Now, the total change in internal energy from state 1 to state 3 is:
\[
\Delta U_{{total}} = \Delta U_{1-2} + \Delta U_{2-3} = 60 + 20 = 80 \, {kJ}
\]
Since the process 3–1 is adiabatic, \( Q = 0 \), so the work interaction is equal to the negative of the change in internal energy:
\[
W_{3-1} = - \Delta U_{{total}} = -80 \, {kJ}
\]
Thus, the work interaction in the adiabatic process is \( 80 \, {kJ} \).