Chemistry of Solutions 202-SN2-RE • CEGEP, Montreal

Revision sheet: chemical thermodynamics (202-SN2-RE)

Thermodynamics says what is POSSIBLE, never what is fast. Two quantities are enough, enthalpy and entropy, and their combination ΔG=ΔH−TΔS\Delta G=\Delta H-T\Delta S settles the question of spontaneity. Temperature acts as the referee, which explains why the same reaction can be impossible when cold and easy when hot.

This sheet gives the table of the four cases, the way to predict the sign of ΔS\Delta S without calculation, the relation between free energy and the equilibrium constant, and the list of unit mistakes that cost the most. It is written for CEGEP students in Chemistry of Solutions, 202-SN2-RE (formerly 202-NYB).

Mark this sheet as read or add it to your favourites: a free account, no password, keeps your read sheets and favourites from one visit to the next, tells you which chapter to tackle next and lets you ask for the method or exercise you are missing. Create your space, an email is enough.

The thread of the chapter

ΔH\Delta H is in kilojoules per mole and ΔS\Delta S in joules per mole per kelvin. Subtracting the two without converting gives a ΔG\Delta G a thousand times too large, and this is by far the most frequent mistake of the chapter.

This chapter is part of 202-SN2-RE, Chemistry of Solutions

The essentials

The three quantities and their units

  • • ΔHr∘=∑nΔHf∘(products)−∑nΔHf∘(reactants)\Delta H^{\circ}_{r}=\sum n\Delta H^{\circ}_{f}(\text{products})-\sum n\Delta H^{\circ}_{f}(\text{reactants}), in kJ/mol. Zero for an element in its standard state.
  • • ΔSr∘=∑nS∘(products)−∑nS∘(reactants)\Delta S^{\circ}_{r}=\sum nS^{\circ}(\text{products})-\sum nS^{\circ}(\text{reactants}), in J/(mol·K). S∘S^{\circ} is TABULATED and always POSITIVE, even for an element.
  • • ΔG=ΔH−TΔS\Delta G=\Delta H-T\Delta S, with TT in KELVINS and both terms in the SAME unit.
  • • Spontaneous if ΔG<0\Delta G<0; at equilibrium if ΔG=0\Delta G=0; nonspontaneous if ΔG>0\Delta G>0.
  • • Link with equilibrium: ΔG∘=−RTln⁡K\Delta G^{\circ}=-RT\ln K, and away from standard conditions ΔG=ΔG∘+RTln⁡Q\Delta G=\Delta G^{\circ}+RT\ln Q.

The two tables differ in nature: the enthalpy of FORMATION is zero for an element and can be negative; ABSOLUTE entropy never is, by virtue of the third law.

Predicting the sign of ΔS\Delta S without calculation

  • • What decides first is the change in the NUMBER OF MOLES OF GAS. More gas on the right: ΔS>0\Delta S>0.
  • • Increasing order of disorder: solid << liquid << gas. A change of state toward the right of this list increases entropy.
  • • Dissolving an ionic solid generally increases entropy; dissolving a gas DECREASES it, since free molecules are being trapped.
  • • With an equal number of moles of gas, compare the complexity of the molecules: the more atoms a molecule has, the higher its entropy.
  • • Heating always increases the entropy of a substance, without changing the sign of ΔS\Delta S for the reaction.
solidliquidgasincreasing disorder and entropy
Solid, liquid, gas: disorder, and so entropy, grows in this order, and the change to gas is by far the biggest jump.

A reaction that consumes gases to give a solid necessarily has ΔS<0\Delta S<0: this is the case for solid ammonium chloride formed from gaseous NH3NH_{3} and HClHCl. The Haber process, for its part, produces a gas: its ΔS\Delta S is negative because four moles of gas give two.

The four cases, and the crossover temperature

  • • ΔH<0\Delta H<0 and ΔS>0\Delta S>0: spontaneous at EVERY temperature. The most favourable case.
  • • ΔH>0\Delta H>0 and ΔS<0\Delta S<0: NEVER spontaneous, at any temperature.
  • • ΔH<0\Delta H<0 and ΔS<0\Delta S<0: spontaneous at LOW temperature, the term −TΔS-T\Delta S eventually winning as the temperature rises.
  • • ΔH>0\Delta H>0 and ΔS>0\Delta S>0: spontaneous at HIGH temperature, which is the case for most decompositions.
  • • Crossover temperature: T=ΔHΔST=\dfrac{\Delta H}{\Delta S}, the one where ΔG=0\Delta G=0. It exists ONLY in the last two cases, those where the two signs are identical.
ΔH < 0ΔH > 0ΔS < 0ΔS > 0low Tneveralwayshigh TΔG = ΔH − TΔS
Only the two cells of the DIAGONAL, where the two signs coincide, have a crossover temperature. The other two are settled in advance, whatever the temperature.

In the first two cases, the calculation ΔHΔS\dfrac{\Delta H}{\Delta S} gives a negative number, hence an impossible absolute temperature: this is how arithmetic signals that there is no crossover.

The mistakes that cost marks

These are the errors I correct most often in session. Each one costs marks on a paper, even when the reasoning behind it is right.

1. Subtracting joules from kilojoules in ΔG=ΔH−TΔS\Delta G=\Delta H-T\Delta S

the whole question, 6 points, and a reversed conclusion

What not to write

“ΔG=178.3−298×160.6=−47,680\Delta G=178.3-298\times 160.6=-47{,}680 kJ/mol.”

What to write

“ΔS\Delta S is in J/(mol·K): it must be converted to kJ. ΔG=178.3−298.15×0.1606=+130.4\Delta G=178.3-298.15\times 0.1606=+130.4 kJ/mol, and the reaction is NOT spontaneous.”

Why: The factor of a thousand changes not only the value but the SIGN of ΔG\Delta G, and so the conclusion about spontaneity. This is the costliest mistake of the chapter.

2. Setting the standard entropy of an element to zero

the whole question, 5 points

What not to write

“S∘(O2)=0S^{\circ}(O_{2})=0, like its enthalpy of formation.”

What to write

“S∘(O2)=205.0S^{\circ}(O_{2})=205.0 J/(mol·K). Standard entropy is ABSOLUTE and always positive: only ΔHf∘\Delta H^{\circ}_{f} is zero for an element.”

ΔH°f (kJ/mol)CaCO₃−1206.9CaO−635.1CO₂−393.5O₂0S° (J/(mol·K))92.9CaCO₃39.8CaO213.7CO₂205O₂S°(O₂) = 0:wrong
The enthalpy of formation of O2O_{2} is zero, its standard entropy is 205.0205.0 J/(mol·K): in the table of S∘S^{\circ}, no bar is at zero.

Why: The two tables do not measure the same thing: one is a difference relative to the elements, the other an absolute value referred to absolute zero, where every entropy vanishes.

3. Leaving the temperature in degrees Celsius

3 points, and a ΔG\Delta G too large by 4444 kJ/mol here

What not to write

“At 2525 °C: ΔG=178.3−25×0.1606=174.3\Delta G=178.3-25\times 0.1606=174.3 kJ/mol.”

What to write

“TT in KELVINS: ΔG=178.3−298.15×0.1606=130.4\Delta G=178.3-298.15\times 0.1606=130.4 kJ/mol.”

50100150200250300350400100110120130140150160170180190T = 25: 174.3298.15 K: 130.4T (K)ΔG (kJ/mol)
On the same line, T=25T=25 reads the red point, almost at ΔH\Delta H; the true temperature, 298.15298.15 K, gives the green point, 4444 kJ/mol lower.

Why: Entropy is defined on an absolute scale. Using degrees Celsius would give a ΔG\Delta G equal to ΔH\Delta H at 00 °C, which makes no physical sense.

4. Confusing spontaneous and fast

4 points on the reasoning question

What not to write

“ΔG∘\Delta G^{\circ} is very negative, so the reaction is fast.”

What to write

“ΔG∘<0\Delta G^{\circ}<0 only says that the reaction is POSSIBLE. The rate depends on the activation energy, which appears nowhere in thermodynamics.”

energyreaction progressdiamond + O₂CO₂high barrierΔG° verynegative
The products are much lower, ΔG∘\Delta G^{\circ} very negative, but the barrier is high: thermodynamics says where the reaction would go, kinetics says whether it goes there.

Why: The combustion of diamond has a very negative ΔG∘\Delta G^{\circ} at room temperature and yet never happens spontaneously: its kinetic barrier cannot be crossed without heating.

5. Looking for a crossover temperature where there is none

3 points, and the direction of the conclusion reversed

What not to write

“ΔH=−92\Delta H=-92 kJ/mol and ΔS=−198\Delta S=-198 J/(mol·K): the crossover temperature is −92,000−198=465\dfrac{-92{,}000}{-198}=465 K, and beyond it the reaction becomes spontaneous.”

What to write

“The two signs are identical, so the crossover does exist, but in the OTHER direction: the reaction is spontaneous BELOW 465465 K and stops being so above.”

200400600800100012001400−120−80−404080120160200465 K1110 KHaber: spontaneous BELOW 465 Klimestone: spontaneous ABOVE 1110 KT (K)ΔG (kJ/mol)
Same formula T=ΔHΔST=\dfrac{\Delta H}{\Delta S}, opposite directions: the Haber line RISES and is negative only below 465465 K; the limestone line goes down and is negative only above 11101110 K.

Why: The formula gives the temperature of the switch, not the direction of the switch. That is read off the signs: ΔH<0\Delta H<0 means that the reaction is favoured when cold.

6. Using ΔG∘\Delta G^{\circ} away from standard conditions

the whole question, 5 points

What not to write

“ΔG∘=+130\Delta G^{\circ}=+130 kJ/mol at 2525 °C, so the decomposition cannot happen at any pressure.”

What to write

“ΔG=ΔG∘+RTln⁡Q\Delta G=\Delta G^{\circ}+RT\ln Q: by sweeping away the carbon dioxide, we lower QQ, hence ΔG\Delta G, and the decomposition becomes possible sooner.”

200400600800100012001400−100−50501001502001110 K897 KP(CO₂) = 1 barP(CO₂) = 0.010 barT (K)ΔG (kJ/mol)
The same reaction, the same enthalpy and the same entropy: only the pressure of the product gas changes, and the temperature needed drops by more than two hundred degrees.

Why: The small circle means “all species at 11 mol/L or 11 bar”. As soon as a partial pressure departs from this value, the ln⁡Q\ln Q term must be added, and the industrial effect is considerable.

7. Counting total moles to predict the sign of ΔS\Delta S

2 points, but the question on the sign comes up every time

What not to write

“CaCO3(s)→CaO(s)+CO2(g)CaCO_{3}(s)\rightarrow CaO(s)+CO_{2}(g): one mole becomes two, so ΔS\Delta S increases a little.”

What to write

“What counts is the number of moles of GAS: we go from ZERO to ONE. That is a considerable jump, and ΔS=+160.6\Delta S=+160.6 J/(mol·K).”

CaCO₃(s)CaO(s) + CO₂(g)0 mol of gas1 mol of gas
Two solids count for almost nothing: it is the appearance of the gas, from zero to one mole, that makes the entropy jump.

Why: The entropy of a gas is about twice that of the corresponding solid. Two solids count for almost nothing in the balance; it is the appearance of a gas that wins.

8. Believing that a negative system entropy forbids the reaction

4 points on the reasoning question

What not to write

“ΔSsystem<0\Delta S_{system}<0, so the reaction violates the second law and is impossible.”

What to write

“It is the entropy of the UNIVERSE that must increase: ΔSuniverse=ΔSsystem+−ΔHT\Delta S_{universe}=\Delta S_{system}+\dfrac{-\Delta H}{T}. An exothermic reaction increases the entropy of the surroundings, which can compensate.”

−198 J/Ksystem+308.6 J/Ksurroundings+110.6 J/Kuniverse
Synthesis of ammonia at 298298 K: the system loses 198198 J/K, but the heat given up makes the surroundings gain 309309, and the entropy of the universe increases.

Why: The criterion ΔG<0\Delta G<0 is nothing other than ΔSuniverse>0\Delta S_{universe}>0 multiplied by −T-T. This is why an ordering reaction, such as the formation of a crystal, remains possible if it releases enough heat.

9. Confusing a spontaneous reaction with a complete one

3 points

What not to write

“ΔG∘<0\Delta G^{\circ}<0, so the reaction goes to completion and no reactant is left.”

What to write

“ΔG∘<0\Delta G^{\circ}<0 only means K>1K>1. A ΔG∘\Delta G^{\circ} of −2-2 kJ/mol gives K=2.2K=2.2, so an equilibrium where a lot of reactant remains.”

Why: The link is logarithmic: about −6-6 kJ/mol is needed for a KK of 1010, and −34-34 kJ/mol for a KK of 10610^{6}. A weakly spontaneous reaction is not a complete reaction.

10. Forgetting to multiply by the coefficients in an entropy balance

3 points

What not to write

“ΔS∘=S∘(NH3)−S∘(N2)−S∘(H2)\Delta S^{\circ}=S^{\circ}(NH_{3})-S^{\circ}(N_{2})-S^{\circ}(H_{2}) for N2+3H2→2NH3N_{2}+3H_{2}\rightarrow 2NH_{3}.”

What to write

“Each term carries its coefficient: ΔS∘=2S∘(NH3)−S∘(N2)−3S∘(H2)\Delta S^{\circ}=2S^{\circ}(NH_{3})-S^{\circ}(N_{2})-3S^{\circ}(H_{2}).”

Why: The tabulated quantities are molar: they refer to one mole of the species. The reaction balance consumes or produces several, so each term is weighted.

11. Getting the sign wrong in the relation between ΔG∘\Delta G^{\circ} and KK

3 points, and a reversed conclusion

What not to write

“ΔG∘=RTln⁡K\Delta G^{\circ}=RT\ln K, so a negative ΔG∘\Delta G^{\circ} gives a KK below 11.”

What to write

“ΔG∘=−RTln⁡K\Delta G^{\circ}=-RT\ln K: a NEGATIVE ΔG∘\Delta G^{\circ} gives a KK ABOVE 11, which is consistent with a favoured reaction.”

correct:wrong: ΔG° = RT ln KΔG° < 0: K > 1ΔG° (kJ/mol)ln KΔG° = −RT ln K
With the minus sign, a negative ΔG∘\Delta G^{\circ} gives ln⁡K>0\ln K>0, so K>1K>1: the green line. The red line would pair a favoured reaction with K<1K<1.

Why: The minus sign is what makes the two criteria agree: spontaneous means both ΔG∘<0\Delta G^{\circ}<0 and K>1K>1. Without it, the two would systematically contradict each other.

Which method to choose

Is the reaction spontaneous?

The signs of ΔH\Delta H and ΔS\Delta S, before any calculation

ΔH < 0, ΔS > 0: alwaysΔH > 0, ΔS < 0: neverΔH < 0, ΔS < 0: at low TΔH > 0, ΔS > 0: at high TT (K)ΔG (kJ/mol)
Each case is a line with intercept ΔH\Delta H and slope −ΔS-\Delta S: only the two that change sign have a crossover temperature.
  • If ΔH<0\Delta H<0 and ΔS>0\Delta S>0 → spontaneous at EVERY temperature, no calculation needed

    Example: combustion of a hydrocarbon producing more gas

  • If ΔH>0\Delta H>0 and ΔS<0\Delta S<0 → NEVER spontaneous, whatever the temperature

    Example: the formation of ozone from oxygen

  • If ΔH<0\Delta H<0 and ΔS<0\Delta S<0 → spontaneous BELOW T=ΔHΔST=\dfrac{\Delta H}{\Delta S}

    Example: the Haber process, favoured when cold but too slow

  • If ΔH>0\Delta H>0 and ΔS>0\Delta S>0 → spontaneous ABOVE T=ΔHΔST=\dfrac{\Delta H}{\Delta S}

    Example: the decomposition of limestone, above 837837 °C

  • If the conditions are NOT standard → ΔG=ΔG∘+RTln⁡Q\Delta G=\Delta G^{\circ}+RT\ln Q, which can change the conclusion

    sweeping away a gaseous product lowers QQ and makes the reaction possible much sooner

The table of the four cases is remembered by its diagonal: where the two signs coincide, temperature is the referee; where they are opposite, the answer is the same at every temperature.

Which quantity to calculate, depending on the question

What the problem asks

  • If “is the reaction spontaneous at such a temperature” → ΔG=ΔH−TΔS\Delta G=\Delta H-T\Delta S, after converting the units

    Example: +130.4+130.4 kJ/mol at 298298 K: nonspontaneous

  • If “from what temperature” → T=ΔHΔST=\dfrac{\Delta H}{\Delta S}, in consistent units, then interpret the direction from the signs

    Example: 178,300160.6=1110\dfrac{178{,}300}{160.6}=1110 K

  • If “what is the equilibrium constant” → K=e−ΔG∘/RTK=e^{-\Delta G^{\circ}/RT}, with ΔG∘\Delta G^{\circ} IN JOULES

    Example: ΔG∘=+130\Delta G^{\circ}=+130 kJ/mol gives K≈10−23K\approx 10^{-23}

  • If the problem gives pressures or concentrations that are not unity → ΔG=ΔG∘+RTln⁡Q\Delta G=\Delta G^{\circ}+RT\ln Q

    Example: sweeping away the product gas lowers the required temperature by two hundred degrees

  • If the problem gives several equations → Hess's law on ΔH\Delta H, on ΔS\Delta S and on ΔG\Delta G: all three are state functions

    reversing changes the sign, multiplying multiplies, adding adds

The three quantities combine through Hess's law in exactly the same way. This is what makes it possible to make an impossible reaction spontaneous by COUPLING it to another, very favourable one, in an industrial process.

How the answer is expected to be written

A marker ticks steps. Here they are in order, with the concluding sentence expected word for word.

Calculating spontaneity and the crossover temperature

When to use it: The problem gives an equation, a table of enthalpies of formation and standard entropies, and asks whether the reaction is spontaneous.

  1. 1 Calculate ΔHr∘\Delta H^{\circ}_{r} in kJ/mol, products minus reactants, each term multiplied by its coefficient.
  2. 2 Calculate ΔSr∘\Delta S^{\circ}_{r} in J/(mol·K), in the same way, remembering that elements have a NONZERO entropy.
  3. 3 CONVERT ΔS\Delta S to kJ/(mol·K) by dividing by one thousand, on a visible line, then write ΔG=ΔH−TΔS\Delta G=\Delta H-T\Delta S with TT in kelvins.
  4. 4 Conclude on spontaneity at the requested temperature, and check consistency with the signs in the table of the four cases.
  5. 5 If the two signs coincide, calculate T=ΔHΔST=\dfrac{\Delta H}{\Delta S} and state whether spontaneity is obtained above or below it.

Concluding sentence

“With ΔH∘=+178.3\Delta H^{\circ}=+178.3 kJ/mol and ΔS∘=+160.6\Delta S^{\circ}=+160.6 J/(mol·K), we obtain ΔG∘=178.3−298.15×0.1606=+130.4\Delta G^{\circ}=178.3-298.15\times 0.1606=+130.4 kJ/mol: the reaction is not spontaneous at 2525 °C, but it becomes so above T=178,300160.6=1110T=\dfrac{178{,}300}{160.6}=1110 K.”

The trap: Forgetting to convert ΔS\Delta S. Writing the division by one thousand explicitly on its own line is the only reliable way not to skip it under exam pressure.

Marking: Typically 2 points for ΔH\Delta H, 2 for ΔS\Delta S, 1 for the conversion, 2 for ΔG\Delta G and the conclusion, 2 for the crossover temperature and its direction.

Handling nonstandard conditions

When to use it: The problem imposes a partial pressure or a concentration different from the standard value, or asks for the effect of sweeping away a gas.

  1. 1 First calculate ΔG∘\Delta G^{\circ} under standard conditions, as usual.
  2. 2 Write QQ as for an equilibrium, including only the gases and the dissolved species.
  3. 3 Apply ΔG=ΔG∘+RTln⁡Q\Delta G=\Delta G^{\circ}+RT\ln Q, with RR in J/(mol·K) and ΔG∘\Delta G^{\circ} converted to joules.
  4. 4 If the temperature that makes the reaction possible is wanted, set ΔG=0\Delta G=0 and solve for TT, keeping the ln⁡Q\ln Q term.
  5. 5 Comment on the gap from the standard temperature: this is usually the real point of the question.

Concluding sentence

“By keeping the pressure of carbon dioxide at 0.0100.010 bar, the condition ΔG=0\Delta G=0 is written 178,300=T(160.6−8.314ln⁡0.010)178{,}300=T(160.6-8.314\ln 0.010), so T=897T=897 K, that is 623623 °C instead of 837837 °C.”

The trap: Mixing ΔG∘\Delta G^{\circ} in kilojoules and RTln⁡QRT\ln Q in joules. The whole calculation must be done in a single unit, and the safest is to convert everything to joules before adding.

Check before you hand in

Five minutes of checking recover more marks than one more problem started in a hurry.

The typical problem, taken apart

The lime kiln, and why it works well below the predicted temperature

The decomposition of limestone is written CaCO3(s)→CaO(s)+CO2(g)CaCO_{3}(s)\rightarrow CaO(s)+CO_{2}(g).

Calculate ΔH∘\Delta H^{\circ}, ΔS∘\Delta S^{\circ} and ΔG∘\Delta G^{\circ} at 2525 °C, then the crossover temperature. Then determine the equilibrium constant at 2525 °C, and finally the temperature required if the kiln is swept so as to keep the pressure of carbon dioxide at 0.0100.010 bar.

Data in kJ/mol for ΔHf∘\Delta H^{\circ}_{f}: CaCO3=−1206.9CaCO_{3}=-1206.9, CaO=−635.1CaO=-635.1, CO2=−393.5CO_{2}=-393.5. In J/(mol·K) for S∘S^{\circ}: CaCO3=92.9CaCO_{3}=92.9, CaO=39.8CaO=39.8, CO2=213.7CO_{2}=213.7. R=8.314R=8.314 J/(mol·K).

CaCO₃(s)furnace at T?airair + CO₂P(CO₂) held at 0.010 bar
The kiln is swept by a stream of air: the carbon dioxide is carried away as it forms and its pressure stays at 0.0100.010 bar.

Step 1

ΔH∘=[(−635.1)+(−393.5)]−(−1206.9)=−1028.6+1206.9=+178.3\Delta H^{\circ}=[(-635.1)+(-393.5)]-(-1206.9)=-1028.6+1206.9=+178.3 kJ/mol.

Why

The result is POSITIVE: the decomposition absorbs heat, which is consistent with the fact that a lime kiln has to be heated continuously.

Step 2

ΔS∘=(39.8+213.7)−92.9=+160.6\Delta S^{\circ}=(39.8+213.7)-92.9=+160.6 J/(mol·K).

Why

The entropy of limestone is not zero even though it appears alone on the left: it is an ABSOLUTE entropy, not an entropy of formation. The gain comes from the appearance of a gas.

Step 3

ΔG∘=ΔH∘−TΔS∘=178.3−298.15×160.61000=178.3−47.9=+130.4\Delta G^{\circ}=\Delta H^{\circ}-T\Delta S^{\circ}=178.3-298.15\times\dfrac{160.6}{1000}=178.3-47.9=+130.4 kJ/mol.

Why

The division by one thousand is written on the line itself: it is the only gesture that prevents the costliest mistake of the chapter, the one that changes the sign of the conclusion.

Step 4

ΔG∘>0\Delta G^{\circ}>0: at 2525 °C, the decomposition is NOT spontaneous. The signs ΔH>0\Delta H>0 and ΔS>0\Delta S>0 announce a reaction favoured at HIGH temperature.

Why

The table of the four cases gives the answer even before the calculation: the only remaining question is from what temperature, which is the object of the next step.

Step 5

Crossover temperature: T=ΔH∘ΔS∘=178,300160.6=1110T=\dfrac{\Delta H^{\circ}}{\Delta S^{\circ}}=\dfrac{178{,}300}{160.6}=1110 K, that is 837837 °C.

Why

Both quantities are brought to joules so that the ratio gives kelvins. The direction of the switch is read off the signs: ABOVE this temperature, the reaction goes.

Step 6

Constant at 2525 °C: ln⁡K=−ΔG∘RT=−130,4008.314×298.15=−52.6\ln K=-\dfrac{\Delta G^{\circ}}{RT}=-\dfrac{130{,}400}{8.314\times 298.15}=-52.6, so K≈1.4×10−23K\approx 1.4\times 10^{-23}.

Why

This value means that at room temperature the equilibrium pressure of carbon dioxide is of the order of 10−2310^{-23} bar: in other words, nothing decomposes.

Step 7

With sweeping: ΔG=ΔG∘+RTln⁡Q\Delta G=\Delta G^{\circ}+RT\ln Q with Q=PCO2=0.010Q=P_{CO_{2}}=0.010. The condition ΔG=0\Delta G=0 gives 178,300=T(160.6−8.314ln⁡0.010)=T(160.6+38.3)=198.9 T178{,}300=T\left(160.6-8.314\ln 0.010\right)=T(160.6+38.3)=198.9\,T.

Why

The logarithm of a number below one is negative, so the term −Rln⁡Q-R\ln Q ADDS to the entropy: it is as if the reaction gained 3838 units of effective entropy.

Step 8

T=178,300198.9=897T=\dfrac{178{,}300}{198.9}=897 K, that is 623623 °C, against 837837 °C under standard conditions.

Why

Two hundred and fourteen degrees saved by a single change to the process: this is exactly the reason why industrial kilns are ventilated continuously.

Step 9

Check: at 11101110 K and under standard conditions, ΔG∘=178.3−1110×0.1606=0.0\Delta G^{\circ}=178.3-1110\times 0.1606=0.0 kJ/mol, so K=1K=1 and the equilibrium pressure of the gas is indeed 11 bar.

Why

This check ties the three results together: the crossover temperature is exactly the one where the constant equals one, which validates both the calculation of ΔG∘\Delta G^{\circ} and that of TT at the same time.

The conclusion, written out

“The decomposition of limestone absorbs 178.3178.3 kJ/mol and gains 160.6160.6 J/(mol·K) of entropy: it is not spontaneous at 2525 °C, where ΔG∘\Delta G^{\circ} is +130.4+130.4 kJ/mol and KK about 10−2310^{-23}, but it becomes so above 837837 °C. By sweeping the kiln to keep the carbon dioxide at 0.0100.010 bar, this temperature falls to 623623 °C.”

The classic mistake on this problem: Writing ΔG∘=178.3−298.15×160.6\Delta G^{\circ}=178.3-298.15\times 160.6 and finding a very negative number, hence concluding that limestone decomposes spontaneously at room temperature. The world would then have no limestone cliffs, which is enough to reject the result.

Learn by heart

  • • ΔH\Delta H in kJ/mol, ΔS\Delta S in J/(mol·K): CONVERT before subtracting.
  • • ΔG=ΔH−TΔS\Delta G=\Delta H-T\Delta S, with TT in KELVINS. Spontaneous if ΔG<0\Delta G<0.
  • • S∘S^{\circ} is absolute and always POSITIVE, even for an element; only ΔHf∘\Delta H^{\circ}_{f} is zero there.
  • • The sign of ΔS\Delta S is read first off the change in the number of moles of GAS.
  • • Four cases: two opposite signs give an answer valid at every temperature; two identical signs give a crossover temperature T=ΔHΔST=\dfrac{\Delta H}{\Delta S}.
  • • ΔG∘=−RTln⁡K\Delta G^{\circ}=-RT\ln K: the MINUS sign makes ΔG∘<0\Delta G^{\circ}<0 equivalent to K>1K>1.
  • • Away from standard conditions: ΔG=ΔG∘+RTln⁡Q\Delta G=\Delta G^{\circ}+RT\ln Q.
  • • Spontaneous does not mean fast, nor complete.

Frequently asked questions

Why must entropy be converted before calculating free energy?

Because enthalpies are tabulated in kilojoules per mole and entropies in joules per mole per kelvin. Subtracting directly amounts to mixing two units that differ by a factor of one thousand, which changes not only the value but the sign of the result, and so the conclusion about spontaneity.

Is the standard entropy of an element zero?

No, never. It is the enthalpy of formation of an element that is zero, by convention. Standard entropy is an absolute value measured from absolute zero, where every entropy vanishes. Gaseous oxygen, for example, has a standard entropy above two hundred joules per mole per kelvin.

How can the sign of the entropy change be predicted without calculation?

First look at the change in the number of moles of gas. If there is more gas on the product side, entropy increases. Solids and liquids weigh much less in the balance. With an equal number of gas moles, compare the complexity of the molecules: the more atoms a molecule has, the greater its entropy.

Is a spontaneous reaction fast?

Not at all. Thermodynamics only says that a reaction is possible, never how fast it happens. The combustion of diamond is very favourable at room temperature and yet never happens spontaneously, for lack of enough energy to cross the activation barrier. The rate belongs to kinetics.

When does a crossover temperature exist?

Only when the enthalpy and the entropy of reaction have the same sign. If the enthalpy is negative and the entropy positive, the reaction is spontaneous at every temperature; in the opposite case, it never is. The ratio then gives a negative number, which is how arithmetic signals that there is no crossover.

Why does a lime kiln work below the calculated temperature?

Because the calculated temperature assumes a carbon dioxide pressure of one bar, which corresponds to standard conditions. By ventilating the kiln, the gas is removed as it forms, which lowers the reaction quotient and the free energy with it. The decomposition becomes possible a couple of hundred degrees sooner.

Practise it

Corrected exercises: Chemical thermodynamics, 202-SN2-RE

A method is proved on a paper, not on a sheet. The set for the same chapter takes each of these traps into a problem, with the solution written out step by step.

  • 10 corrected exercises
  • 100 points
  • 150 minutes
Do the exercises
Something missing from this sheet? A method, a trap, an exercise to practise it, a mistake you spotted: tell me, I read every request.

Sending goes through your free space: that is how I can answer you and tell you when the exercise is added. An email is enough, no password. Create your space. Rather not create an account? Write to me directly.

What is it about?
I read every request myself, nobody else sees it. No need to write your name or your school.
When your request is dealt with, you hear about it by email and in your space.

By sending, you agree that I read your request to answer it. It is kept with your account, erased with it, and never published: privacy policy.

Previous sheet Redox and electrochemistry Next sheet Solutions and colligative properties

© Ahmed Squalli Houssaini. Revision sheet published at www.letuteurscientifique.ca/en/fiches/cegep-chem-sn2-thermodynamics. Free for personal and classroom use; republishing it elsewhere requires written permission (legal notice).

See also

Looking for a 202-SN2-RE tutor in Montreal?

Get in touch for a first session. In thermodynamics, we first install the unit discipline and the table of the four cases: the rest of the chapter follows from them.

Site by Studio Squalli