Entropy, internal energy and temperature are all state functions: their value depends only on the current state of the system, not on the history that brought it there. Two gases in the same state (P,V,T,n)(P, V, T, n) have the same entropy, regardless of how they got there.

Why this is crucial

Even in an irreversible transformation, ΔSgas\Delta S_\text{gas} can be calculated with the formulas from this section, as if going from A to B along an imagined reversible path. The result is the same, because SS depends only on the endpoints A and B, not on the path.

This property is what makes the formulas for the gas, the solid and the thermostat universally applicable. Many real processes are violently irreversible — a gas exploding into a vacuum, two bodies at different temperatures suddenly brought into contact — and for them there is no well-defined “path” in the PP-VV diagram: they pass through non-equilibrium states that cannot even be drawn. And yet, since the initial state A and the final state B are well-defined equilibrium states, we can imagine a fictitious reversible path connecting them and calculate ΔS\Delta S along it. The value obtained is the true entropy change of the real process.

A useful analogy is with gravitational potential energy: the difference in altitude between two points on a mountain does not depend on the path chosen to climb it. In the same way, ΔS\Delta S between two states does not depend on the transformation chosen to connect them.

There is, however, a fundamental difference from energy. The internal energy of the gas does not change depending on whether the process is reversible or irreversible: it is always a “neutral” state function. The entropy of the gas is also a state function, but the total entropy (gas plus surroundings) clearly distinguishes the two cases: it stays unchanged only in reversible processes, and increases in irreversible ones. It is precisely this distinction that is the content of the second law, the subject of the next section.

Topics: Entropy and the second law Concepts: Entropy · Internal energy · Temperature

Related exercises: Heat from hot to cold: proof · T ratio · Melting 1 kg of ice: ΔS