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Chemistry · Ch 6 — Equilibrium

Relationship between Equilibrium Constant K, Reaction Quotient Q and Gibbs Energy G

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Relationship between Equilibrium Constant K, Reaction Quotient Q and Gibbs Energy G

The Thermodynamic Link Between KK, QQ, and ΔG\Delta G

The equilibrium constant KcK_c for a reaction is a number that tells you where equilibrium lies, but it is not a kinetic quantity — it does not depend on how fast the reaction gets there. Instead, KcK_c is rooted in thermodynamics, specifically in the Gibbs energy change ΔG\Delta G of the reaction. This connection is what lets us predict the direction of a reaction from a single measurement of concentrations.

The sign of ΔG\Delta G tells you the story of the reaction's spontaneity:

  • If ΔG\Delta G is negative, the forward reaction is spontaneous — it will proceed on its own.
  • If ΔG\Delta G is positive, the forward reaction is non-spontaneous. But the reverse reaction then has a negative ΔG\Delta G, so the products will convert back into reactants.
  • If ΔG\Delta G is zero, the system is at equilibrium. No net free energy remains to drive the reaction in either direction.

This thermodynamic view is captured in a single equation that relates ΔG\Delta G to the reaction quotient QQ:

ΔG=ΔG∘+RTln⁡Q(6.21)\Delta G = \Delta G^\circ + RT \ln Q \qquad(6.21)

Here ΔG∘\Delta G^\circ is the standard Gibbs energy change (when all reactants and products are in their standard states, typically 1 bar pressure for gases and 1 M concentration for solutions), RR is the gas constant (8.314 J mol−1K−18.314\ \text{J mol}^{-1}\text{K}^{-1}), and TT is the absolute temperature in Kelvin.

The Equilibrium Condition: Deriving ΔG∘=−RTln⁡K\Delta G^\circ = -RT \ln K

At equilibrium, the system has no net driving force — ΔG=0\Delta G = 0. At that same point, the reaction quotient QQ equals the equilibrium constant KK (whether KcK_c or KpK_p, depending on the units). Substituting these two conditions into equation (6.21) gives:

0=ΔG∘+RTln⁡K0 = \Delta G^\circ + RT \ln K

Rearranging:

ΔG∘=−RTln⁡K(6.22)\Delta G^\circ = -RT \ln K \qquad(6.22)

This is the master equation that links thermodynamics and equilibrium. It can also be written as:

ln⁡K=−ΔG∘RT\ln K = -\frac{\Delta G^\circ}{RT}

Or, exponentiating both sides:

K=e−ΔG∘/RTK = e^{-\Delta G^\circ / RT}

Important

Equation (6.22) is the bridge between two worlds: the thermodynamic quantity ΔG∘\Delta G^\circ (which you can look up in tables of standard Gibbs energies of formation) and the equilibrium constant KK (which you measure experimentally). A single value of ΔG∘\Delta G^\circ determines KK uniquely at a given temperature.

What This Equation Tells Us About KK

The relationship K=e−ΔG∘/RTK = e^{-\Delta G^\circ / RT} reveals three clear regimes:

Sign of ΔG∘\Delta G^\circValue of KKMeaning
Negative (ΔG∘<0\Delta G^\circ < 0)K>1K > 1Products are favoured at equilibrium; the equilibrium lies to the right.
Zero (ΔG∘=0\Delta G^\circ = 0)K=1K = 1Reactants and products are equally favoured at equilibrium.
Positive (ΔG∘>0\Delta G^\circ > 0)0<K<10 < K < 1Reactants are favoured at equilibrium; the equilibrium lies to the left.
Watch out

Do not confuse ΔG\Delta G with ΔG∘\Delta G^\circ. ΔG∘\Delta G^\circ is a fixed value for a given reaction at a given temperature — it determines KK. ΔG\Delta G depends on the actual concentrations (or pressures) of reactants and products through QQ, and it tells you whether the reaction will proceed forward or backward from those conditions. A reaction with ΔG∘>0\Delta G^\circ > 0 (and therefore K<1K < 1) can still have ΔG<0\Delta G < 0 if the initial concentrations are far from equilibrium — for example, if you start with no products at all.

Using QQ and KK to Predict Direction

The equation ΔG=ΔG∘+RTln⁡Q\Delta G = \Delta G^\circ + RT \ln Q can be combined with ΔG∘=−RTln⁡K\Delta G^\circ = -RT \ln K to give a direct comparison: …