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Thermodynamics and Energetics — Diagnostic Tests

Unit Tests

UT-1: Born-Haber Cycle for an Ionic Compound

Question:

Construct a Born-Haber cycle for magnesium oxide (MgO\text{MgO}) and calculate the lattice energy. Use the following data:

QuantityValue / kJ mol1\text{kJ mol}^{-1}
Enthalpy of atomisation of Mg+148+148
Enthalpy of atomisation of O (12O2\frac{1}{2}\text{O}_2)+249+249
First ionisation energy of Mg+738+738
Second ionisation energy of Mg+1451+1451
First electron affinity of O141-141
Second electron affinity of O+798+798
Standard enthalpy of formation of MgO602-602

Solution:

Born-Haber cycle (all values in kJ mol1\text{kJ mol}^{-1}):

Mg(s)+12O2(g)ΔHf=602Mg2+O2(s)\text{Mg}(s) + \tfrac{1}{2}\text{O}_2(g) \xrightarrow{\Delta H_f = -602} \text{Mg}^{2+}\text{O}^{2-}(s)

Two routes from elements to ionic solid:

Route 1 (direct): ΔHf=602\Delta H_f = -602

Route 2 (indirect via gaseous ions):

  1. Atomisation of Mg: +148+148
  2. Atomisation of 12O2\frac{1}{2}\text{O}_2: +249+249
  3. First ionisation of Mg: +738+738
  4. Second ionisation of Mg: +1451+1451
  5. First electron affinity of O: 141-141
  6. Second electron affinity of O: +798+798
  7. Lattice energy (LE): ΔHlatt\Delta H_{\text{latt}}

By Hess's law: Route 1 = Route 2

602=148+249+738+1451141+798+ΔHlatt-602 = 148 + 249 + 738 + 1451 - 141 + 798 + \Delta H_{\text{latt}}

602=3243+ΔHlatt-602 = 3243 + \Delta H_{\text{latt}}

ΔHlatt=6023243=3845kJ mol1\Delta H_{\text{latt}} = -602 - 3243 = -3845\,\text{kJ mol}^{-1}

The lattice energy of MgO is 3845kJ mol1-3845\,\text{kJ mol}^{-1}.

Note: The large magnitude reflects the very strong electrostatic attraction between Mg2+\text{Mg}^{2+} and O2\text{O}^{2-} (high charges, small ions). The second electron affinity of oxygen is endothermic because adding an electron to a negatively charged O\text{O}^- ion requires energy to overcome repulsion.


UT-2: Hess's Law with Indirect Enthalpy Determination

Question:

The standard enthalpy change of combustion of ethanol is 1367kJ mol1-1367\,\text{kJ mol}^{-1}. The standard enthalpy change of combustion of carbon is 394kJ mol1-394\,\text{kJ mol}^{-1}, and the standard enthalpy change of combustion of hydrogen is 286kJ mol1-286\,\text{kJ mol}^{-1}.

(a) Use Hess's law to calculate the standard enthalpy change of formation of ethanol, C2H5OH(l)\text{C}_2\text{H}_5\text{OH}(l).

(b) The experimental value is 277kJ mol1-277\,\text{kJ mol}^{-1}. Suggest a reason why the calculated value might differ from the experimental value.

Solution:

(a) Target equation: 2C(s)+3H2(g)+12O2(g)C2H5OH(l)2\text{C}(s) + 3\text{H}_2(g) + \tfrac{1}{2}\text{O}_2(g) \to \text{C}_2\text{H}_5\text{OH}(l)

Using the combustion data and Hess's law (elements to products via combustion products):

Formation = Sum of combustion of elements - Combustion of compound

ΔHf(C2H5OH)=2×ΔHc(C)+3×ΔHc(H2)ΔHc(C2H5OH)\Delta H_f(\text{C}_2\text{H}_5\text{OH}) = 2 \times \Delta H_c(\text{C}) + 3 \times \Delta H_c(\text{H}_2) - \Delta H_c(\text{C}_2\text{H}_5\text{OH})

=2×(394)+3×(286)(1367)= 2 \times (-394) + 3 \times (-286) - (-1367)

=788858+1367= -788 - 858 + 1367

=1646+1367=279kJ mol1= -1646 + 1367 = -279\,\text{kJ mol}^{-1}

(b) The calculated value (279kJ mol1-279\,\text{kJ mol}^{-1}) is close to but not identical to the experimental value (277kJ mol1-277\,\text{kJ mol}^{-1}). Small differences arise from:

  • Experimental uncertainties in the combustion data used (each measurement has some error, which propagates through the calculation).
  • Incomplete combustion in the experiments determining combustion enthalpies.
  • State differences: The standard state of ethanol at 298K298\,\text{K} may not be exactly matched in the combustion experiment (e.g., trace water vapour vs liquid).
  • Heat losses from the calorimeter during combustion measurements.

UT-3: Gibbs Free Energy and Spontaneity

Question:

For the decomposition of calcium carbonate:

CaCO3(s)CaO(s)+CO2(g)\text{CaCO}_3(s) \to \text{CaO}(s) + \text{CO}_2(g)

ΔH=+178kJ mol1\Delta H^\circ = +178\,\text{kJ mol}^{-1}, ΔS=+161J K1 mol1\Delta S^\circ = +161\,\text{J K}^{-1}\text{ mol}^{-1}.

(a) Calculate ΔG\Delta G^\circ at 298K298\,\text{K} and state whether the reaction is spontaneous at this temperature.

(b) Calculate the minimum temperature at which the reaction becomes thermodynamically feasible.

(c) Explain why the entropy change is positive for this reaction, even though a solid is being converted to another solid and a gas.

Solution:

(a)

ΔG=ΔHTΔS\Delta G^\circ = \Delta H^\circ - T\Delta S^\circ

ΔG=178000298×161=17800047978=+130022J mol1=+130kJ mol1\Delta G^\circ = 178000 - 298 \times 161 = 178000 - 47978 = +130022\,\text{J mol}^{-1} = +130\,\text{kJ mol}^{-1}

ΔG>0\Delta G^\circ \gt 0, so the reaction is not spontaneous at 298K298\,\text{K}.

(b) The reaction becomes feasible when ΔG0\Delta G^\circ \leq 0:

ΔHTΔS0\Delta H^\circ - T\Delta S^\circ \leq 0

TLBΔHRB◆◆LBΔSRB=178000161=1106KT \geq \frac◆LB◆\Delta H^\circ◆RB◆◆LB◆\Delta S^\circ◆RB◆ = \frac{178000}{161} = 1106\,\text{K}

The minimum temperature is approximately 1106K1106\,\text{K} (833C833\,^\circ\text{C}).

(c) The entropy change is positive because a gas is produced from a solid. Gases have much higher entropy than solids (gas molecules have many more possible arrangements due to their freedom of movement). The gain in entropy from creating 1 mol of CO2(g)\text{CO}_2(g) more than compensates for the fact that one solid (CaCO3\text{CaCO}_3) is replaced by another solid (CaO\text{CaO}). The overall effect is an increase in disorder:

ΔS=S(CaO)+S(CO2)S(CaCO3)\Delta S^\circ = S^\circ(\text{CaO}) + S^\circ(\text{CO}_2) - S^\circ(\text{CaCO}_3)

The large positive entropy of CO2(g)\text{CO}_2(g) (approximately 214J K1 mol1214\,\text{J K}^{-1}\text{ mol}^{-1}) compared to the solids drives the overall entropy change positive.

Integration Tests

IT-1: Thermodynamic Feasibility of Industrial Processes (with Equilibrium)

Question:

The Contact process involves the oxidation of sulfur dioxide:

2SO2(g)+O2(g)2SO3(g)2\text{SO}_2(g) + \text{O}_2(g) \rightleftharpoons 2\text{SO}_3(g)

ΔH=198kJ mol1\Delta H^\circ = -198\,\text{kJ mol}^{-1}, ΔS=190J K1 mol1\Delta S^\circ = -190\,\text{J K}^{-1}\text{ mol}^{-1}.

(a) Calculate the temperature above which the reaction is no longer thermodynamically feasible.

(b) Given that industrial conditions use 400400--450C450\,^\circ\text{C}, explain why this temperature range is chosen despite the thermodynamic considerations.

(c) Calculate ΔG\Delta G^\circ at 700K700\,\text{K} and hence calculate KpK_p at this temperature.

Solution:

(a) The reaction ceases to be feasible when ΔG>0\Delta G^\circ \gt 0:

T>LBΔHRB◆◆LBΔSRB=198000190=1042KT \gt \frac◆LB◆\Delta H^\circ◆RB◆◆LB◆\Delta S^\circ◆RB◆ = \frac{-198000}{-190} = 1042\,\text{K}

Above 1042K1042\,\text{K} (769C769\,^\circ\text{C}), the reaction is no longer thermodynamically spontaneous. The negative ΔS\Delta S^\circ (3 mol gas \to 2 mol gas) means that at high temperatures, the TΔS-T\Delta S^\circ term dominates and makes ΔG\Delta G^\circ positive.

(b) At 400400--450C450\,^\circ\text{C} (673673--723K723\,\text{K}), the reaction is thermodynamically feasible (ΔG<0\Delta G^\circ \lt 0 since T<1042KT \lt 1042\,\text{K}). Although lower temperatures give a more negative ΔG\Delta G^\circ (higher equilibrium yield), the rate of reaction would be impractically slow. 400400--450C450\,^\circ\text{C} represents a compromise between thermodynamic yield and kinetic rate. A vanadium(V) oxide catalyst is used to further increase the rate at these temperatures.

(c) At 700K700\,\text{K}:

ΔG=198000700×(190)=198000+133000=65000J mol1\Delta G^\circ = -198000 - 700 \times (-190) = -198000 + 133000 = -65000\,\text{J mol}^{-1}

Using ΔG=RTlnKp\Delta G^\circ = -RT\ln K_p:

65000=8.31×700×lnKp-65000 = -8.31 \times 700 \times \ln K_p

lnKp=650005817=11.17\ln K_p = \frac{65000}{5817} = 11.17

Kp=e11.17=7.08×104atm1K_p = e^{11.17} = 7.08 \times 10^4\,\text{atm}^{-1}


IT-2: Entropy Changes in Dissolution (with Bonding and Acids/Bases)

Question:

(a) Explain why the dissolution of NaCl\text{NaCl} in water has a small positive entropy change, while the dissolution of CaCO3\text{CaCO}_3 in water is not thermodynamically feasible.

(b) The dissolution of ammonium nitrate in water is endothermic yet spontaneous. Use thermodynamic arguments to explain this.

(c) Calculate the entropy change when 2.00mol2.00\,\text{mol} of ice melts at 0C0\,^\circ\text{C}. The standard enthalpy of fusion of ice is +6.01kJ mol1+6.01\,\text{kJ mol}^{-1}.

Solution:

(a) For NaCl\text{NaCl} dissolving: NaCl(s)Na+(aq)+Cl(aq)\text{NaCl}(s) \to \text{Na}^+(aq) + \text{Cl}^-(aq)

The entropy change involves competing factors:

  • Positive contribution: The ordered ionic lattice breaks down, and ions become dispersed in solution (increased disorder)
  • Negative contribution: Water molecules become more ordered around the hydrated ions (water molecules orient their partial charges towards the ions, restricting their freedom)

For NaCl\text{NaCl}, the lattice breakdown slightly outweighs the ordering of water, giving a small positive ΔS\Delta S.

For CaCO3\text{CaCO}_3: CaCO3(s)Ca2+(aq)+CO32(aq)\text{CaCO}_3(s) \to \text{Ca}^{2+}(aq) + \text{CO}_3^{2-}(aq)

The doubly-charged ions cause much more ordering of water molecules around them (stronger ion-dipole interactions, more structured hydration shells). The negative contribution from water ordering outweighs the positive contribution from lattice breakdown, giving a negative ΔS\Delta S. Combined with the endothermic lattice breaking, ΔG\Delta G is positive, making dissolution non-spontaneous.

(b) For NH4NO3(s)NH4+(aq)+NO3(aq)\text{NH}_4\text{NO}_3(s) \to \text{NH}_4^+(aq) + \text{NO}_3^-(aq):

The process is endothermic (ΔH>0\Delta H \gt 0), but the entropy change is strongly positive because:

  • The ionic lattice breaks down completely
  • Both ions are large and singly charged, so they cause relatively little ordering of water
  • The ammonium ion can form hydrogen bonds but retains rotational freedom

The large positive ΔS\Delta S makes TΔS-T\Delta S more negative than ΔH\Delta H is positive, giving ΔG<0\Delta G \lt 0 (spontaneous). This demonstrates that enthalpy alone does not determine spontaneity.

(c) At the melting point, ΔG=0\Delta G = 0, so ΔS=ΔH/T\Delta S = \Delta H/T:

ΔS=6010273=22.0J K1 mol1\Delta S = \frac{6010}{273} = 22.0\,\text{J K}^{-1}\text{ mol}^{-1}

For 2.00mol2.00\,\text{mol}:

ΔStotal=2.00×22.0=44.0J K1\Delta S_{\text{total}} = 2.00 \times 22.0 = 44.0\,\text{J K}^{-1}

The positive entropy change reflects the increased disorder as water molecules in the rigid ice lattice gain freedom of movement in liquid water.


IT-3: Enthalpy Changes and Bond Energies (with Kinetics)

Question:

The hydrogenation of ethene is:

C2H4(g)+H2(g)C2H6(g)ΔH=137kJ mol1\text{C}_2\text{H}_4(g) + \text{H}_2(g) \to \text{C}_2\text{H}_6(g) \quad \Delta H = -137\,\text{kJ mol}^{-1}

Bond enthalpies: C==C =612= 612, C--C =348= 348, C--H =412= 412, H--H =436= 436 (all in kJ mol1\text{kJ mol}^{-1}).

(a) Use bond enthalpies to estimate ΔH\Delta H for this reaction and explain why it differs from the given value.

(b) Draw an enthalpy profile diagram for this reaction, labelling the activation energy EaE_a and the enthalpy change ΔH\Delta H.

(c) Explain why this reaction requires a catalyst despite being exothermic.

Solution:

(a) Bonds broken:

  • 1 ×\times C==C: 612612
  • 4 ×\times C--H (in C2H4\text{C}_2\text{H}_4): 4×412=16484 \times 412 = 1648
  • 1 ×\times H--H: 436436

Total bonds broken: 612+1648+436=2696kJ mol1612 + 1648 + 436 = 2696\,\text{kJ mol}^{-1}

Bonds formed:

  • 1 ×\times C--C: 348348
  • 6 ×\times C--H (in C2H6\text{C}_2\text{H}_6): 6×412=24726 \times 412 = 2472

Total bonds formed: 348+2472=2820kJ mol1348 + 2472 = 2820\,\text{kJ mol}^{-1}

ΔH=26962820=124kJ mol1\Delta H = 2696 - 2820 = -124\,\text{kJ mol}^{-1}

This differs from the experimental value of 137kJ mol1-137\,\text{kJ mol}^{-1} because bond enthalpies are average values taken from many different molecules. The actual C==C bond in ethene and C--C bond in ethane may differ from the average values. Bond enthalpies apply to gaseous species only and do not account for variations in bond strength due to the molecular environment.

(b) The enthalpy profile shows:

  • Reactants (C2H4+H2\text{C}_2\text{H}_4 + \text{H}_2) at a higher energy level
  • Products (C2H6\text{C}_2\text{H}_6) at a lower energy level (exothermic, ΔH=137kJ mol1\Delta H = -137\,\text{kJ mol}^{-1})
  • A peak (transition state) above the reactants, with EaE_a being the difference between the peak and the reactant energy level
  • ΔH\Delta H is the vertical difference between products and reactants

(c) Despite being exothermic (ΔH<0\Delta H \lt 0), the reaction has a significant activation energy (EaE_a). The H--H bond (436kJ mol1436\,\text{kJ mol}^{-1}) and the C==C π\pi-bond (part of the 612kJ mol1612\,\text{kJ mol}^{-1}) must be broken before new bonds can form. At room temperature, very few molecules have sufficient kinetic energy (Ea\geq E_a) to overcome this barrier. A metal catalyst (e.g., Ni, Pd, or Pt) provides an alternative pathway by adsorbing both H2\text{H}_2 and C2H4\text{C}_2\text{H}_4 onto its surface, weakening the H--H bond and lowering the activation energy.


Additional Practice Problems

UT-4: Hess's Law with Combustion Data

Question: Use the following standard enthalpies of combustion to calculate the standard enthalpy change for the hydrogenation of propene to propane:

C3H6(g)+H2(g)C3H8(g)\mathrm{C}_3\mathrm{H}_6(g) + \mathrm{H}_2(g) \to \mathrm{C}_3\mathrm{H}_8(g)

ΔHc(C3H6)=2058kJmol1\Delta H_c^\circ(\mathrm{C}_3\mathrm{H}_6) = -2058\,\mathrm{kJ\,mol^{-1}}

ΔHc(C3H8)=2220kJmol1\Delta H_c^\circ(\mathrm{C}_3\mathrm{H}_8) = -2220\,\mathrm{kJ\,mol^{-1}}

ΔHc(H2)=286kJmol1\Delta H_c^\circ(\mathrm{H}_2) = -286\,\mathrm{kJ\,mol^{-1}}

Solution:

Hess's Law cycle:

Reactants \to Products \to Combustion products (CO2+H2O\mathrm{CO}_2 + \mathrm{H}_2\mathrm{O})

Path 1 (indirect): Reactants \to combustion products: ΔHc(C3H6)+ΔHc(H2)=2058+(286)=2344kJmol1\Delta H_c(\mathrm{C}_3\mathrm{H}_6) + \Delta H_c(\mathrm{H}_2) = -2058 + (-286) = -2344\,\mathrm{kJ\,mol^{-1}}

Path 2 (via products): Products \to combustion products: ΔHc(C3H8)=2220kJmol1\Delta H_c(\mathrm{C}_3\mathrm{H}_8) = -2220\,\mathrm{kJ\,mol^{-1}}

ΔH=Path 1Path 2=2344(2220)=124kJmol1\Delta H^\circ = \text{Path 1} - \text{Path 2} = -2344 - (-2220) = -124\,\mathrm{kJ\,mol^{-1}} (2 marks).

The hydrogenation is exothermic, as expected for converting a C=C double bond to two C--H single bonds.

IT-4: Born-Haber and Entropy Combined

Question: Calculate the lattice energy of CaF2\mathrm{CaF}_2 using a Born-Haber cycle and the following data:

QuantityValue (kJ mol1^{-1})
ΔHf(CaF2)\Delta H_f^\circ(\mathrm{CaF}_2)1220-1220
ΔHatom(Ca)\Delta H_{\text{atom}}(\mathrm{Ca})+178+178
ΔHatom(F2)\Delta H_{\text{atom}}(\mathrm{F}_2) (per 12F2\frac{1}{2}\mathrm{F}_2)+79+79
First IE of Ca+590+590
Second IE of Ca+1145+1145
Electron affinity of F328-328

Solution:

Born-Haber cycle for CaF2\mathrm{CaF}_2:

ΔHf=ΔHatom(Ca)+ΔHatom(F2)×2+IE1+IE2+EA×2+Lattice Energy\Delta H_f^\circ = \Delta H_{\text{atom}}(\mathrm{Ca}) + \Delta H_{\text{atom}}(\mathrm{F}_2) \times 2 + \text{IE}_1 + \text{IE}_2 + \text{EA} \times 2 + \text{Lattice Energy}

1220=178+79×2+590+1145+(328)×2+LE-1220 = 178 + 79 \times 2 + 590 + 1145 + (-328) \times 2 + \text{LE}

1220=178+158+590+1145656+LE-1220 = 178 + 158 + 590 + 1145 - 656 + \text{LE}

1220=1415+LE-1220 = 1415 + \text{LE}

LE=12201415=2635kJmol1\text{LE} = -1220 - 1415 = -2635\,\mathrm{kJ\,mol^{-1}} (2 marks).

The large (negative) lattice energy reflects the high charges on Ca2+\mathrm{Ca}^{2+} and F\mathrm{F}^- and the small ionic radii, both of which increase the electrostatic attraction in the lattice (1 mark).