5.2.2(d)-(f) - Free energy, feasibility and kinetic limits

5.2.2(d)-(f) - Free energy, feasibility and kinetic limits

Some chemical changes are favoured by energy being released, some by entropy increasing, and many by a balance between the two. This lesson teaches how OCR links those ideas using Gibbs free energy, ΔG\Delta G, so that you can calculate whether a process is thermodynamically feasible at a stated temperature. You will also learn the key limitation: a feasible reaction may still be too slow to observe.

The Gibbs balance

Feasibility is about whether a process is thermodynamically allowed under the stated conditions. OCR uses the sign of the free energy change, ΔG\Delta G, to make that judgement.

Free energy change

The free energy change, ΔG\Delta G, combines the enthalpy change of the system, ΔH\Delta H, with the temperature-weighted entropy change of the system, TΔST\Delta S.

Gibbs equation

ΔG=ΔH−TΔS\Delta G = \Delta H - T\Delta S

A process is feasible when ΔG\Delta G has a negative value. If ΔG\Delta G is positive, the process is not thermodynamically feasible under those stated conditions. If ΔG=0\Delta G = 0, the process is at the boundary where feasibility changes.

The terms in the equation have to be in compatible units:

quantityusual unit in OCR calculationsnote
ΔH\Delta H kJ mol−1\,\mathrm{kJ} \,\mathrm{mol}^{-1}enthalpy change of the system
TTK\mathrm Ktemperature must be in kelvin
ΔS\Delta S J K−1\,\mathrm{J} \,\mathrm{K}^{-1}  mol−1\,\mathrm{mol}^{-1} or  kJ K−1\,\mathrm{kJ} \,\mathrm{K}^{-1}  mol−1\,\mathrm{mol}^{-1}convert if needed
ΔG\Delta G kJ mol−1\,\mathrm{kJ} \,\mathrm{mol}^{-1}if ΔH\Delta H is in  kJ mol−1\,\mathrm{kJ} \,\mathrm{mol}^{-1}

The most common method is to convert ΔS\Delta S from  J K−1\,\mathrm{J} \,\mathrm{K}^{-1}  mol−1\,\mathrm{mol}^{-1} to  kJ K−1\,\mathrm{kJ} \,\mathrm{K}^{-1}  mol−1\,\mathrm{mol}^{-1} by dividing by 1000. Then TΔST\Delta S has units of  kJ mol−1\,\mathrm{kJ} \,\mathrm{mol}^{-1}, matching ΔH\Delta H.

Do not read "feasible" as "fast". Negative ΔG\Delta G means the energy balance favours the process; it does not yet say whether particles can get over the activation-energy barrier.

Calculating free energy change

A free energy calculation is usually a careful substitution exercise. The chemistry is in the signs and units.

Worked example:

A reaction has:

  • ΔH=−74.8 kJ mol−1\Delta H = -74.8\ \mathrm{kJ\ mol^{-1}}
  • ΔS=−80.7 J K−1 mol−1\Delta S = -80.7\ \mathrm{J\ K^{-1}\ mol^{-1}}
  • T=298 KT = 298\ \mathrm{K}

Calculate ΔG\Delta G and state whether the reaction is feasible at 298 K\mathrm K.

First convert entropy into  kJ K−1\,\mathrm{kJ} \,\mathrm{K}^{-1}  mol−1\,\mathrm{mol}^{-1}:

ΔS=−80.71000=−0.0807 kJ K−1 mol−1\Delta S = \frac{-80.7}{1000} = -0.0807\ \mathrm{kJ\ K^{-1}\ mol^{-1}}

Now substitute into the Gibbs equation:

ΔG=ΔH−TΔS\Delta G = \Delta H - T\Delta S ΔG=−74.8−(298×−0.0807)\Delta G = -74.8 - (298 \times -0.0807)

Estimate before pressing on: 300×0.08≈24300 \times 0.08 \approx 24, so the entropy term will add about +24 kJ mol−1+24\ \mathrm{kJ\ mol^{-1}} because subtracting a negative gives a positive contribution.

ΔG=−74.8+24.0=−50.8 kJ mol−1\Delta G = -74.8 + 24.0 = -50.8\ \mathrm{kJ\ mol^{-1}}

The value is negative, so the reaction is feasible at 298 K\mathrm K.

If a question gives entropies of individual substances instead of ΔS\Delta S, use the previous entropy method first:

ΔS=∑S(products)−∑S(reactants)\Delta S = \sum S(\text{products}) - \sum S(\text{reactants})

Then use the resulting ΔS\Delta S in the Gibbs equation. Coefficients in the balanced equation still matter when calculating ΔS\Delta S.

Temperature and sign reasoning

The term TΔST\Delta S explains why temperature can change feasibility. As temperature increases, the entropy term has a bigger effect on ΔG\Delta G.

[DIAGRAM: asset_name: Lesson 5.2.2d-f: Free energy, feasibility and kinetic limits - diagram 01; asset_slug: 05_02_02b_free_energy_feasibility_and_kinetic_limits__diagram_01; recommended_method: drawn_chem; description: Deterministic sign map for Delta H and Delta S combinations, showing always feasible, never feasible, high-temperature feasible and low-temperature feasible cases under the Gibbs equation.]
Diagram

The sign of ΔH\Delta H tells you whether the enthalpy term helps or opposes feasibility. A negative ΔH\Delta H helps make ΔG\Delta G negative; a positive ΔH\Delta H makes ΔG\Delta G more positive.

The sign of ΔS\Delta S has to be read through the term −TΔS-T\Delta S:

  • if ΔS\Delta S is positive, −TΔS-T\Delta S is negative, so increasing temperature helps feasibility
  • if ΔS\Delta S is negative, −TΔS-T\Delta S is positive, so increasing temperature works against feasibility

This gives four useful cases:

ΔH\Delta HΔS\Delta Seffect on feasibility
negativepositivefeasible at all temperatures
positivenegativenot feasible at any temperature
positivepositivefeasible only at high enough temperature
negativenegativefeasible only at low enough temperature

These patterns assume ΔH\Delta H and ΔS\Delta S are approximately constant over the temperature range considered. They are not a replacement for calculation. If numbers are given, calculate ΔG\Delta G.

Worked example:

A reaction has ΔH=+85.0 kJ mol−1\Delta H = +85.0\ \mathrm{kJ\ mol^{-1}} and ΔS=+170 J K−1 mol−1\Delta S = +170\ \mathrm{J\ K^{-1}\ mol^{-1}}. Both signs are positive, so the reaction is only feasible at high enough temperature.

Convert entropy:

ΔS=+0.170 kJ K−1 mol−1\Delta S = +0.170\ \mathrm{kJ\ K^{-1}\ mol^{-1}}

At the feasibility boundary, ΔG=0\Delta G = 0:

0=ΔH−TΔS0 = \Delta H - T\Delta S

Rearrange:

T=ΔHΔST = \frac{\Delta H}{\Delta S}

Substitute:

T=85.00.170=500 KT = \frac{85.0}{0.170} = 500\ \mathrm{K}

Because ΔH\Delta H and ΔS\Delta S are both positive, higher temperature makes −TΔS-T\Delta S more negative. The reaction becomes feasible above 500 K\mathrm K.

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