A heat engine is a device that, by repeating a cycle, continuously converts heat into useful work. Its operation always requires two sources at different temperatures: it absorbs heat QHQ_H from a hot source at temperature THT_H, converts part of it into mechanical work LL, and releases the rest QCQ_C to a cold source at temperature TCT_C.

The physical intuition is that heat never converts entirely into work: part of it must always “slide” towards the cold. It is this spontaneous flow from hot to cold that the engine intercepts and partly diverts in the form of work, just as a water wheel intercepts water falling from a height.

Diagram of a heat engine: it absorbs heat QHQ_H from the hot source, produces work LL and releases QCQ_C to the cold source.

The efficiency η\eta measures what fraction of the absorbed heat is actually converted into work. Since over a full cycle the internal energy returns to its initial value, the first law imposes Lnetto=QHQCL_\text{netto} = Q_H - |Q_C|: everything that goes in and does not come out as released heat becomes work.

Principle — Efficiency

η=LnettoQH=1QCQH\ev{\eta = \frac{L_\text{netto}}{Q_H} = 1 - \frac{|Q_C|}{Q_H}}

Efficiency is therefore always less than 11: it would equal 11 only if QC=0Q_C = 0, i.e. if the engine released nothing to the cold. But this is precisely what the second law forbids.

Topics: Macchine termiche Concepts: Rendimento Objects: Macchina termica

Related exercises: Problema — Dimostrazione del rendimento di Carnot · Problema — Ciclo di Carnot monoatomico (400-250 K) · Problema — Ranking di quattro macchine di Carnot