Chemical equilibrium · five routes to K
One reaction.
Several routes to equilibrium.
Compare equilibrium constants from Gibbs energies, formation properties, enthalpy and entropy, a reference K, and equilibrium activities. Keep the reaction basis, temperature and standard states consistent.
Compare thermodynamic K
Direct and formation Gibbs energies apply only at their supplied temperature. Scroll the table horizontally on narrow screens. Energy values are per reaction as written.
Teal: constant ΔH° approximation. Amber: constant ΔCp° correction. Solid lines use Kref; dashed lines use ΔH° and ΔS°. Supplied Gibbs-energy data appear as points only. Matching curves can overlap.
Formation-energy sum
Observed activities: Q or inferred K
From K to equilibrium composition
Five routes, one standard-state convention
2. ΔrG° = ΣᵢνᵢΔfGᵢ°
3. ΔrG°(T) = ΔrH°(T) − TΔrS°(T)
4. ln[K(T)/Kref] = ΔrH°ref/R (1/Tref − 1/T)
5. K = Πᵢaᵢ^νᵢ only at equilibrium
Reaction coefficients are positive for products and negative for reactants. Reversing a reaction gives Knew=1/K; multiplying all coefficients by c gives Knew=K^c. Reaction-level energies and entropies must be transformed on the same basis. The app does not silently reconcile conflicting independent inputs.
For gases aᵢ=φᵢyᵢP/p°. For solutes on the supplied molarity standard aᵢ=γᵢcᵢ/c°. A liquid solution uses aᵢ=γᵢxᵢ relative to the pure-liquid standard. Unit activities for pure solids and liquids require their presence. The composition panel admits one gas phase and one liquid-solution phase; omitted mole fractions can represent nonreacting components.
All formation and reaction properties must use the same species phases and standard states. No automatic conversion of molarity, molality, pure-liquid or gas standards is performed. Individual-ion activity coefficients are convention dependent; no electrolyte model is supplied.
Heat-capacity correction Constant reaction ΔCp° over the declared interval
ΔS°(T) = ΔS°ref + ΔCp° ln(T/Tref)
ln[K(T)/Kref] = ΔH°ref/R (1/Tref − 1/T)
+ ΔCp°/R [ln(T/Tref) + Tref/T − 1]
The two corrected routes agree only if Kref and the reference ΔH°/ΔS° are mutually consistent. A point value of ΔG° does not provide a temperature law. No polynomial Cp, phase-transition correction or external property database is assumed.
ln K is retained when exponentiating would overflow or underflow; such K values are labeled rather than replaced by zero or infinity. A finite ln K does not guarantee that a nearly depleted equilibrium composition can be resolved in floating-point arithmetic.
Ideal-gas extent and validation
nᵢ=nᵢ,0+νᵢξ defines the feasible extent interval. The solver brackets ln Q(ξ)−ln K at fixed T and total pressure, then independently checks atom conservation. For the admitted single neutral ideal-gas reaction, Gibbs energy is convex along ξ, so the resolved stationary state is the global minimum within that model. The reported relative total Gibbs energy divided by RT has units of mol.
Pressure changes the composition even though standard K depends only on temperature for the fixed standard-state convention. Inert gas affects this fixed-pressure calculation by dilution. This is not the same constraint as adding inert gas to a rigid ideal-gas vessel.
No multireaction minimizer, charged-gas solver, nonideal EOS, reaction–phase equilibrium or electrochemical cell is included. Electrochemistry is the next lab.