




Look at the flow sketch first: water leaves the condenser at 1, gets pushed to higher pressure by the pump at 2, is warmed further by steam bled from the turbine until it reaches 3, is boiled and heated fully at 4, and expands through the turbine down to 5 before returning to the condenser. Two of these five steps are meant to be frictionless and reversible: the pump (1 to 2) and the turbine (4 to 5). On a temperature versus entropy plot, a reversible pump or turbine shows up as a straight vertical line because entropy cannot change during that step.
Since the ideal cycle needs both the pump and turbine legs to stand vertical while still showing a separate heating step from 2 to 3, option A is the one that fits.
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 \( R = 8 \, \text{J/molK} \)):
