Analysing a thermodynamic cycle can seem complicated, but it becomes mechanical if a systematic method in four steps is followed. The underlying idea is to separate two levels: first the states (the vertices of the cycle) are fixed, then the processes (the segments connecting the vertices) are studied.

  1. Identify the processes. Recognise the type of each transformation (isothermal, isochoric, isobaric, adiabatic, …): establish which are reversible and which constraints hold on each segment (for example constant TT, or Q=0Q = 0).
  2. Table of states. For each vertex of the cycle compute the triplet PP, VV, TT using the ideal gas law PV=nRTPV = nRT and the specific relations of the process leading to that vertex.
  3. Table of processes. For each segment compute the four exchange quantities: heat QQ, work done by the gas LgasL_\text{gas}, change in internal energy ΔEint\Delta E_\text{int} and change in entropy ΔSgas\Delta S_\text{gas}.
  4. Checks. Verify the consistency of the calculations by closing the cycle.

Cycle-closure checks

Over a complete cycle the state functions return to their initial value, so: ΔEint,ciclo=0ΔSgas,ciclo=0Lnetto=QHQC\begin{aligned} \Delta E_\text{int,ciclo} &= 0 \\ \Delta S_\text{gas,ciclo} &= 0 \\ L_\text{netto} &= Q_H - |Q_C| \end{aligned} If one of these three relations does not hold, there is an error in a row of the table: they are a powerful automatic check on the calculations.

The first law guarantees that ΔEint=0\Delta E_\text{int} = 0 over every closed cycle, because internal energy is a state function; for the same reason the entropy of the gas also returns to its starting value. The net work, on the other hand, is not zero: it is the difference between the heat absorbed and that released, and in the PP-VV plane it coincides with the area enclosed by the cycle.

Topics: Macchine termiche Concepts: Primo principio della termodinamica Skills: Risoluzione di un ciclo termodinamico Methods: Diagramma P-V e ln P - ln V

Related exercises: Problema — Frigo con la porta aperta · Problema — Rendimento di una macchina reale (4000-3000 J) · Problema — Bilanci di un ciclo