Part of PC-04 — Chemical Thermodynamics

Feynman Note: Gibbs Free Energy — The "Useful Work" Concept

by Notetube Official246 words5 views

The Simple Idea

Gibbs free energy GG answers one question: "Can this reaction drive itself at constant temperature and pressure?"

Think of ΔG\Delta G as the "maximum useful work" a reaction can do (beyond PV work). When ΔG<0\Delta G < 0, the system has "free energy" to drive the reaction forward spontaneously.

Why G=HTSG = H - TS?

HH is the total energy content. But some energy is "locked up" in entropy — it is the thermal energy that must be there to maintain the level of disorder (TSTS). You cannot use this entropy-locked energy for work.

Useful energy = Total energy - Entropy tax G=HTSG = H - TS

The Driving Forces

  1. Enthalpy drive (ΔH<0\Delta H < 0): System wants to go downhill in energy (like a ball rolling down a hill)
  2. Entropy drive (TΔS>0T\Delta S > 0): System wants to maximize disorder (like a gas expanding to fill space)

When BOTH drives push the same direction → always spontaneous. When they oppose → the temperature determines which wins.

At Equilibrium

ΔG=0\Delta G = 0: no net driving force. The system has reached the lowest free energy state available. Forward and reverse rates are equal.

Intuition Check

  • Large KK (products favored) ↔ ΔG0\Delta G^\circ \ll 0 (reaction drives strongly to products)
  • Small KK (reactants favored) ↔ ΔG0\Delta G^\circ \gg 0 (system prefers reactants)
  • K=1K = 1ΔG=0\Delta G^\circ = 0 (no preference at equilibrium)

Like these notes? Save your own copy and start studying with NoteTube's AI tools.

Sign up free to clone these notes