The key here is remembering that enthalpy of an ideal gas ties only to temperature, so any statement mixing in pressure needs to be checked against that fact.
The direct consequence of sharing an isotherm is $h_2 = h_3$, option A.
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 \( R = 8 \, \text{J/molK} \)):
