Gibbs Free Energy

A2 · 12 min

Whether a reaction can happen on its own depends on two things: the enthalpy change (energy released to or taken from the surroundings) and the entropy change of the system. The Gibbs free energy change, ΔG\Delta G, combines them into one number whose sign tells you whether a reaction is feasible. Paper 4 regularly asks you to calculate ΔG⊖\Delta G^{\ominus}, decide feasibility, and find the temperature at which a reaction becomes feasible, usually as part of a longer question on thermal decomposition or industrial processes.

The Gibbs equation

Key result
ΔG⊖=ΔH⊖−TΔS⊖\Delta G^{\ominus} = \Delta H^{\ominus} - T\Delta S^{\ominus}
  • ΔG⊖\Delta G^{\ominus} and ΔH⊖\Delta H^{\ominus} in kJ mol−1\text{kJ mol}^{-1}
  • TT in kelvin (T/K=θ/∘C+273T/\text{K} = \theta/^\circ\text{C} + 273)
  • ΔS⊖\Delta S^{\ominus} must be converted to kJ K−1 mol−1\text{kJ K}^{-1}\ \text{mol}^{-1} (divide by 1000) before substituting
Definition

A reaction or process is feasible if ΔG\Delta G is negative. If ΔG\Delta G is positive, the reaction is not feasible under those conditions (the reverse reaction is feasible). When ΔG=0\Delta G = 0, the system is at the boundary between feasible and not feasible.

Where the equation comes from

You do not need to derive it, but the idea makes it easier to use. The total entropy change of the universe must be positive for a process to happen spontaneously. The surroundings gain entropy when they absorb heat released by the reaction: ΔSsurr=−ΔH/T\Delta S_{\text{surr}} = -\Delta H/T. Adding the system and surroundings and multiplying by −T-T gives

−TΔStotal=ΔH−TΔSsystem=ΔG-T\Delta S_{\text{total}} = \Delta H - T\Delta S_{\text{system}} = \Delta G

So a negative ΔG\Delta G is the same as a positive total entropy change. The ΔH\Delta H term accounts for the surroundings; the TΔST\Delta S term accounts for the system.

The four combinations

Because TT is always positive, the signs of ΔH\Delta H and ΔS\Delta S decide how feasibility depends on temperature.

Feasibility and temperature
ΔH\Delta HΔS\Delta SΔG=ΔH−TΔS\Delta G = \Delta H - T\Delta SFeasible?
negativepositivealways negativeat all temperatures
positivenegativealways positiveat no temperature
negativenegativenegative at low TT, positive at high TTonly below T=ΔH/ΔST = \Delta H/\Delta S
positivepositivepositive at low TT, negative at high TTonly above T=ΔH/ΔST = \Delta H/\Delta S

The temperature at which feasibility changes is found by setting ΔG=0\Delta G = 0:

T=ΔH⊖ΔS⊖T = \frac{\Delta H^{\ominus}}{\Delta S^{\ominus}}

with ΔS\Delta S in kJ K−1 mol−1\text{kJ K}^{-1}\ \text{mol}^{-1} so that the units cancel to give kelvin.

Seeing it on a graph

Since ΔH\Delta H and ΔS\Delta S change only slightly with temperature, a graph of ΔG\Delta G against TT is approximately a straight line with intercept ΔH\Delta H (at T=0T = 0) and gradient −ΔS-\Delta S.

The first graph is for the decomposition of calcium carbonate (ΔH⊖=+178 kJ mol−1\Delta H^{\ominus} = +178\ \text{kJ mol}^{-1}, ΔS⊖=+160.4 J K−1 mol−1\Delta S^{\ominus} = +160.4\ \text{J K}^{-1}\ \text{mol}^{-1}), plotted as ΔG\Delta G in kJ mol⁻¹ against TT in K. The line falls and crosses zero at about 1110 K: above this, decomposition is feasible.

y = 178 - 0.1604x (1110, -100) -- (1110, 200)

The second graph is for the Haber process (ΔH⊖=−92 kJ mol−1\Delta H^{\ominus} = -92\ \text{kJ mol}^{-1}, ΔS⊖=−198.8 J K−1 mol−1\Delta S^{\ominus} = -198.8\ \text{J K}^{-1}\ \text{mol}^{-1}). The line rises and crosses zero at about 463 K: the forward reaction is feasible only below this temperature.

y = -92 + 0.1988x (463, -100) -- (463, 100)

A positive gradient means ΔS\Delta S is negative; a negative gradient means ΔS\Delta S is positive. Exam questions sometimes give you the graph and ask you to read off ΔH\Delta H (intercept) or ΔS\Delta S (minus the gradient).

Feasible does not mean fast

ΔG\Delta G tells you whether a reaction is thermodynamically possible. It says nothing about the rate. A reaction with a very negative ΔG\Delta G may be immeasurably slow at room temperature if its activation energy is high.

  • The conversion of diamond into graphite has ΔG⊖≈−3 kJ mol−1\Delta G^{\ominus} \approx -3\ \text{kJ mol}^{-1} at 298 K, but diamonds do not turn into graphite, because breaking the strong covalent network has an enormous activation energy.
  • Methane and oxygen can be mixed safely (ΔG⊖\Delta G^{\ominus} about −818 kJ mol−1-818\ \text{kJ mol}^{-1}) until a spark supplies the activation energy.

Such systems are described as kinetically stable (or kinetically inert) but thermodynamically unstable.

Watch out

Never write "the reaction happens quickly because ΔG\Delta G is negative". A negative ΔG\Delta G means the reaction is feasible; whether it is observed depends on the activation energy and the rate.

Gibbs calculations
  1. If not given, calculate ΔH⊖\Delta H^{\ominus} (for example from enthalpies of formation) and ΔS⊖\Delta S^{\ominus} (from standard entropies).
  2. Convert ΔS⊖\Delta S^{\ominus} from J K⁻¹ mol⁻¹ to kJ K⁻¹ mol⁻¹ by dividing by 1000.
  3. Convert the temperature to kelvin.
  4. Substitute into ΔG⊖=ΔH⊖−TΔS⊖\Delta G^{\ominus} = \Delta H^{\ominus} - T\Delta S^{\ominus} and state the sign and units.
  5. For a minimum or maximum temperature, set ΔG=0\Delta G = 0 and calculate T=ΔH/ΔST = \Delta H/\Delta S. State whether the reaction is feasible above or below it, using the signs.

Worked examples

Decomposition of calcium carbonate

For CaCOX3(s)→CaO(s)+COX2(g)\ce{CaCO3(s) -> CaO(s) + CO2(g)}, ΔH⊖=+178 kJ mol−1\Delta H^{\ominus} = +178\ \text{kJ mol}^{-1} and ΔS⊖=+160.4 J K−1 mol−1\Delta S^{\ominus} = +160.4\ \text{J K}^{-1}\ \text{mol}^{-1}.

(a) Calculate ΔG⊖\Delta G^{\ominus} at 298 K and comment. (b) Calculate the minimum temperature at which the decomposition becomes feasible.

Solution

(a)

ΔG⊖=178−298×0.1604=178−47.8=+130 kJ mol−1\Delta G^{\ominus} = 178 - 298 \times 0.1604 = 178 - 47.8 = +130\ \text{kJ mol}^{-1}

Positive, so not feasible at room temperature: limestone is stable.

(b)

T=ΔH⊖ΔS⊖=1780.1604=1110 KT = \frac{\Delta H^{\ominus}}{\Delta S^{\ominus}} = \frac{178}{0.1604} = 1110\ \text{K}

Since ΔS\Delta S is positive, −TΔS-T\Delta S becomes more negative as TT rises, so the reaction is feasible above 1110 K (about 837 ∘C837\ ^\circ\text{C}). Lime kilns operate above this temperature.

The Haber process

For NX2(g)+3 HX2(g)→2 NHX3(g)\ce{N2(g) + 3H2(g) -> 2NH3(g)}, ΔH⊖=−92 kJ mol−1\Delta H^{\ominus} = -92\ \text{kJ mol}^{-1} and ΔS⊖=−198.8 J K−1 mol−1\Delta S^{\ominus} = -198.8\ \text{J K}^{-1}\ \text{mol}^{-1}.

(a) Show that the reaction is feasible at 298 K. (b) Calculate the temperature above which it is no longer feasible. (c) Suggest why the industrial process operates at about 700 K anyway.

Solution

(a)

ΔG⊖=−92−298×(−0.1988)=−92+59.2=−32.8 kJ mol−1\Delta G^{\ominus} = -92 - 298 \times (-0.1988) = -92 + 59.2 = -32.8\ \text{kJ mol}^{-1}

Negative, so feasible.

(b)

T=−92−0.1988=463 KT = \frac{-92}{-0.1988} = 463\ \text{K}

Above 463 K, −TΔS-T\Delta S (which is positive) outweighs ΔH\Delta H, so ΔG⊖\Delta G^{\ominus} is positive.

(c) At low temperature the rate is far too slow, even with a catalyst. A compromise temperature gives an acceptable rate. (Feasibility under standard conditions is not the whole story: high pressure and removal of ammonia shift the position of equilibrium in favour of ammonia, so a useful yield is still obtained.)

Melting ice

For HX2O(s)→HX2O(l)\ce{H2O(s) -> H2O(l)}, ΔH⊖=+6.01 kJ mol−1\Delta H^{\ominus} = +6.01\ \text{kJ mol}^{-1} and ΔS⊖=+22.0 J K−1 mol−1\Delta S^{\ominus} = +22.0\ \text{J K}^{-1}\ \text{mol}^{-1}. Calculate ΔG\Delta G at 263 K and at 283 K, and the temperature at which ΔG=0\Delta G = 0.

SolutionΔG263=6.01−263×0.0220=6.01−5.786=+0.22 kJ mol−1\Delta G_{263} = 6.01 - 263 \times 0.0220 = 6.01 - 5.786 = +0.22\ \text{kJ mol}^{-1}ΔG283=6.01−283×0.0220=6.01−6.226=−0.22 kJ mol−1\Delta G_{283} = 6.01 - 283 \times 0.0220 = 6.01 - 6.226 = -0.22\ \text{kJ mol}^{-1}T=6.010.0220=273 KT = \frac{6.01}{0.0220} = 273\ \text{K}

Ice does not melt at −10 ∘C-10\ ^\circ\text{C} but does at +10 ∘C+10\ ^\circ\text{C}. At 273 K, ΔG=0\Delta G = 0: ice and water coexist in equilibrium at the melting point.

From enthalpies of formation and entropies

Sodium hydrogencarbonate decomposes on heating:

2 NaHCOX3(s)→NaX2COX3(s)+HX2O(g)+COX2(g)\ce{2NaHCO3(s) -> Na2CO3(s) + H2O(g) + CO2(g)}
SubstanceΔHf⊖\Delta H^{\ominus}_{\text{f}} / kJ mol⁻¹S⊖S^{\ominus} / J K⁻¹ mol⁻¹
NaHCOX3(s)\ce{NaHCO3(s)}–950.8101.7
NaX2COX3(s)\ce{Na2CO3(s)}–1130.7135.0
HX2O(g)\ce{H2O(g)}–241.8188.7
COX2(g)\ce{CO2(g)}–393.5213.6

Calculate the minimum temperature for decomposition.

SolutionΔH⊖=[−1130.7+(−241.8)+(−393.5)]−2(−950.8)=−1766.0+1901.6=+135.6 kJ mol−1\Delta H^{\ominus} = [-1130.7 + (-241.8) + (-393.5)] - 2(-950.8) = -1766.0 + 1901.6 = +135.6\ \text{kJ mol}^{-1}ΔS⊖=(135.0+188.7+213.6)−2(101.7)=+333.9 J K−1 mol−1\Delta S^{\ominus} = (135.0 + 188.7 + 213.6) - 2(101.7) = +333.9\ \text{J K}^{-1}\ \text{mol}^{-1}T=135.60.3339=406 KT = \frac{135.6}{0.3339} = 406\ \text{K}

Both ΔH\Delta H and ΔS\Delta S are positive, so decomposition is feasible above 406 K (about 133 ∘C133\ ^\circ\text{C}). This is why baking powder releases carbon dioxide in a hot oven.

Extracting ΔH and ΔS from two values of ΔG (exam-hard)

For a reaction, ΔG=+20.0 kJ mol−1\Delta G = +20.0\ \text{kJ mol}^{-1} at 300 K and −4.0 kJ mol−1-4.0\ \text{kJ mol}^{-1} at 500 K. Assuming ΔH\Delta H and ΔS\Delta S do not change with temperature, calculate ΔH\Delta H, ΔS\Delta S and the temperature at which the reaction becomes feasible.

Solution

Write the Gibbs equation at each temperature:

20.0=ΔH−300ΔS−4.0=ΔH−500ΔS20.0 = \Delta H - 300\Delta S \qquad -4.0 = \Delta H - 500\Delta S

Subtract the second from the first:

24.0=200ΔS⇒ΔS=0.120 kJ K−1 mol−1=+120 J K−1 mol−124.0 = 200\Delta S \quad\Rightarrow\quad \Delta S = 0.120\ \text{kJ K}^{-1}\ \text{mol}^{-1} = +120\ \text{J K}^{-1}\ \text{mol}^{-1}ΔH=20.0+300×0.120=+56.0 kJ mol−1\Delta H = 20.0 + 300 \times 0.120 = +56.0\ \text{kJ mol}^{-1}T=56.00.120=467 KT = \frac{56.0}{0.120} = 467\ \text{K}

Feasible above 467 K. (This is the graph method in algebra: the gradient between the two points is −ΔS-\Delta S.)

Common mistakes
  • Unit mismatch. Substituting ΔS=160.4\Delta S = 160.4 (in J) with ΔH=178\Delta H = 178 (in kJ). Always divide ΔS\Delta S by 1000.
  • Celsius. TT must be in kelvin.
  • Wrong direction. Saying the Haber process is feasible "above 463 K". Check the signs: negative ΔS\Delta S means higher temperatures make ΔG\Delta G more positive.
  • Confusing feasibility with rate. A feasible reaction may not occur at a measurable rate.
  • Losing signs when ΔS\Delta S is negative. −T×(−0.1988)-T \times (-0.1988) is +0.1988T+0.1988T. Use brackets.

Exam technique

Exam tip
  • "State whether the reaction is feasible" needs a reason: "ΔG\Delta G is negative (or positive), so it is (or is not) feasible".
  • When asked to "predict the effect of temperature on feasibility", refer to the sign of ΔS\Delta S and the size of the TΔST\Delta S term compared with ΔH\Delta H.
  • When calculating TT at which a reaction becomes feasible, state "above" or "below" it. Without this the final mark is usually lost.
  • Assumptions examiners like: "ΔH\Delta H and ΔS\Delta S do not vary with temperature" and "the reaction occurs under standard conditions".
  • If a reaction is feasible but does not occur, the expected explanation is a high activation energy, so the rate is very slow.

Summary

Summary
  • ΔG⊖=ΔH⊖−TΔS⊖\Delta G^{\ominus} = \Delta H^{\ominus} - T\Delta S^{\ominus}, with ΔS\Delta S in kJ K⁻¹ mol⁻¹ and TT in K.
  • A reaction is feasible when ΔG\Delta G is negative.
  • ΔH<0\Delta H < 0, ΔS>0\Delta S > 0: always feasible. ΔH>0\Delta H > 0, ΔS<0\Delta S < 0: never feasible.
  • When ΔH\Delta H and ΔS\Delta S have the same sign, feasibility switches at T=ΔH/ΔST = \Delta H / \Delta S: positive ΔS\Delta S means feasible above it; negative ΔS\Delta S means feasible below it.
  • ΔG\Delta G against TT is a straight line with intercept ΔH\Delta H and gradient −ΔS-\Delta S.
  • Feasibility says nothing about rate; high activation energy can make a feasible reaction too slow to observe.

Practice questions

Question
  1. State the Gibbs equation and the units of each term.
  2. For a reaction, ΔH⊖=−46 kJ mol−1\Delta H^{\ominus} = -46\ \text{kJ mol}^{-1} and ΔS⊖=−99 J K−1 mol−1\Delta S^{\ominus} = -99\ \text{J K}^{-1}\ \text{mol}^{-1}. Calculate ΔG⊖\Delta G^{\ominus} at 298 K and state whether the reaction is feasible.
  3. For the decomposition of magnesium carbonate, ΔH⊖=+117 kJ mol−1\Delta H^{\ominus} = +117\ \text{kJ mol}^{-1} and ΔS⊖=+175 J K−1 mol−1\Delta S^{\ominus} = +175\ \text{J K}^{-1}\ \text{mol}^{-1}. Calculate the minimum temperature for decomposition.
  4. Explain why a reaction with ΔH\Delta H positive and ΔS\Delta S negative can never be feasible.
  5. For 2 SOX2(g)+OX2(g)→2 SOX3(g)\ce{2SO2(g) + O2(g) -> 2SO3(g)}, ΔH⊖=−197.8 kJ mol−1\Delta H^{\ominus} = -197.8\ \text{kJ mol}^{-1} and ΔS⊖=−187.8 J K−1 mol−1\Delta S^{\ominus} = -187.8\ \text{J K}^{-1}\ \text{mol}^{-1}. Calculate ΔG⊖\Delta G^{\ominus} at 298 K and the temperature above which the reaction is not feasible.
  6. Ammonium nitrate dissolves with ΔH⊖=+25.7 kJ mol−1\Delta H^{\ominus} = +25.7\ \text{kJ mol}^{-1} and ΔS⊖=+108.7 J K−1 mol−1\Delta S^{\ominus} = +108.7\ \text{J K}^{-1}\ \text{mol}^{-1}. Show that dissolving is feasible at 298 K.
  7. The conversion of diamond to graphite has a negative ΔG⊖\Delta G^{\ominus} at 298 K. Explain why diamonds do not change into graphite.
  8. A graph of ΔG\Delta G against TT for a reaction is a straight line passing through (0 K,+80 kJ mol−1)(0\ \text{K}, +80\ \text{kJ mol}^{-1}) and (800 K,−16 kJ mol−1)(800\ \text{K}, -16\ \text{kJ mol}^{-1}). Find ΔH\Delta H and ΔS\Delta S.
  9. Iron(III) oxide is reduced by carbon: FeX2OX3(s)+3 C(s)→2 Fe(s)+3 CO(g)\ce{Fe2O3(s) + 3C(s) -> 2Fe(s) + 3CO(g)}. Data: ΔHf⊖\Delta H^{\ominus}_{\text{f}} / kJ mol⁻¹: FeX2OX3\ce{Fe2O3} –824.2, CO\ce{CO} –110.5. S⊖S^{\ominus} / J K⁻¹ mol⁻¹: FeX2OX3\ce{Fe2O3} 87.4, C 5.7, Fe 27.3, CO 197.7. Calculate the minimum temperature at which the reduction is feasible.
  10. For a reaction, ΔG=+20.0 kJ mol−1\Delta G = +20.0\ \text{kJ mol}^{-1} at 300 K and −4.0 kJ mol−1-4.0\ \text{kJ mol}^{-1} at 500 K. Without calculating, explain how you can tell the sign of ΔS\Delta S, and then state whether ΔH\Delta H must be positive or negative.
Answers
  1. ΔG⊖=ΔH⊖−TΔS⊖\Delta G^{\ominus} = \Delta H^{\ominus} - T\Delta S^{\ominus}; ΔG\Delta G and ΔH\Delta H in kJ mol⁻¹, TT in K, ΔS\Delta S in kJ K⁻¹ mol⁻¹ (data are usually given in J K⁻¹ mol⁻¹ and must be divided by 1000).

  2. ΔG⊖=−46−298(−0.099)=−46+29.5=−16.5 kJ mol−1\Delta G^{\ominus} = -46 - 298(-0.099) = -46 + 29.5 = -16.5\ \text{kJ mol}^{-1}. Negative, so feasible.

  3. T=117/0.175=669 KT = 117 / 0.175 = 669\ \text{K}. ΔS\Delta S is positive, so decomposition is feasible above 669 K.

  4. ΔH\Delta H is positive and −TΔS-T\Delta S is also positive (since ΔS\Delta S is negative and TT is positive), so ΔG\Delta G is positive at every temperature.

  5. ΔG⊖=−197.8+298(0.1878)=−197.8+56.0=−141.8 kJ mol−1\Delta G^{\ominus} = -197.8 + 298(0.1878) = -197.8 + 56.0 = -141.8\ \text{kJ mol}^{-1} (feasible). T=197.8/0.1878=1053 KT = 197.8/0.1878 = 1053\ \text{K}; above this the reaction is not feasible.

  6. ΔG⊖=25.7−298(0.1087)=25.7−32.4=−6.7 kJ mol−1\Delta G^{\ominus} = 25.7 - 298(0.1087) = 25.7 - 32.4 = -6.7\ \text{kJ mol}^{-1}. Negative, so feasible: the large entropy increase outweighs the endothermic enthalpy change.

  7. The reaction has a very high activation energy because many strong covalent bonds in the giant diamond lattice must be broken. The rate at room temperature is negligible, so diamond is kinetically stable even though it is thermodynamically unstable relative to graphite.

  8. Intercept: ΔH=+80 kJ mol−1\Delta H = +80\ \text{kJ mol}^{-1}. Gradient =(−16−80)/800=−0.120 kJ K−1 mol−1=−ΔS= (-16 - 80)/800 = -0.120\ \text{kJ K}^{-1}\ \text{mol}^{-1} = -\Delta S, so ΔS=+0.120 kJ K−1 mol−1=+120 J K−1 mol−1\Delta S = +0.120\ \text{kJ K}^{-1}\ \text{mol}^{-1} = +120\ \text{J K}^{-1}\ \text{mol}^{-1}.

  9. ΔH⊖=3(−110.5)−(−824.2)=−331.5+824.2=+492.7 kJ mol−1\Delta H^{\ominus} = 3(-110.5) - (-824.2) = -331.5 + 824.2 = +492.7\ \text{kJ mol}^{-1}. ΔS⊖=[2(27.3)+3(197.7)]−[87.4+3(5.7)]=647.7−104.5=+543.2 J K−1 mol−1\Delta S^{\ominus} = [2(27.3) + 3(197.7)] - [87.4 + 3(5.7)] = 647.7 - 104.5 = +543.2\ \text{J K}^{-1}\ \text{mol}^{-1}. T=492.7/0.5432=907 KT = 492.7 / 0.5432 = 907\ \text{K}; reduction is feasible above about 907 K.

  10. ΔG\Delta G becomes more negative as TT increases, so −TΔS-T\Delta S must be becoming more negative: ΔS\Delta S is positive. At 300 K, ΔG\Delta G is positive even though −TΔS-T\Delta S is negative, so ΔH\Delta H must be positive (and larger than 300ΔS300\Delta S).

How well do you know this?

Builds on

Console

Search notes, courses and tools, or run an action