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Gibbs Free Energy: Why ΔG = ΔH − TΔS Makes Sense

Derive the spontaneity criterion from the Second Law instead of memorising a four-case table.

Most students memorise the table of signs for ΔH and ΔS. You never need to — the result comes straight from the Second Law.

Start from the universe

A process is spontaneous when ΔSuniverse > 0. Split it: ΔSuniv = ΔSsys + ΔSsurr. At constant T and P, the surroundings absorb heat −ΔHsys, so ΔSsurr = −ΔH/T.

Multiply by −T

−TΔSuniv = ΔH − TΔSsys. That quantity is defined as ΔG. Since ΔSuniv > 0 means −TΔSuniv < 0, spontaneity becomes simply ΔG < 0.

Now the four cases read themselves

  • ΔH < 0, ΔS > 0 → always spontaneous.
  • ΔH > 0, ΔS < 0 → never spontaneous.
  • ΔH < 0, ΔS < 0 → spontaneous at low T.
  • ΔH > 0, ΔS > 0 → spontaneous at high T.
Note: the crossover temperature is T = ΔH/ΔS — a favourite one-line JEE numerical.

Link it to equilibrium with ΔG° = −RT ln K and to cells with ΔG = −nFE, and three chapters collapse into one idea.

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