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21-Mat-A1 Thermodynamics · May 2015

Question 3 of 7: Temperature Dependence of ΔS° — CO Oxidation at 500 K

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

National Exams — May 2015 — 10-Met-A1 Metallurgical Thermodynamics. Three-hour, closed-book exam using an approved (Casio or Sharp) calculator; candidates were told to state any interpretive assumptions. Any five of the seven questions constitute a complete paper — all seven are solved below for completeness. All questions are of equal value (20 marks each out of 100).

Reference texts: Gaskell, D. R., Introduction to the Thermodynamics of Materials (2nd–5th ed.) — the exam's own Ellingham diagram (Fig. 9-3) is reproduced from this text, which also supplies the standard-state enthalpy/entropy data used below; supporting 298 K entropies for the elements, CO, CO₂, H₂, H₂O(g) and Cu₂O/Cr₂O₃/TiO₂/SiO₂ from the NIST–JANAF Thermochemical Tables.

Question 3: Temperature Dependence of ΔS° — CO Oxidation at 500 K (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

QuantityCO(g)CO₂(g)O₂(g)
$S^\circ_{298}$ (J/K·mol)197.7213.7205.1
$C_p(T)$ (J/K·mol)$31.1-1.5\times10^{-2}T+3.1\times10^{-5}T^2-1.5\times10^{-8}T^3$$18.9+7.9\times10^{-2}T-6.8\times10^{-5}T^2+2.4\times10^{-8}T^3$$30.8-1.2\times10^{-2}T+2.4\times10^{-5}T^2$

Find. $\Delta S^\circ_R$ at $T=500$ K for $\text{CO(g)}+\tfrac12\text{O}_2\text{(g)}=\text{CO}_2\text{(g)}$.

Approach. Compute $\Delta S^\circ_{298}$ from the tabulated standard entropies, then apply the Kirchhoff-type correction $\Delta S^\circ(500)=\Delta S^\circ(298)+\int_{298}^{500}\dfrac{\Delta C_p(T)}{T}dT$ using $\Delta C_p(T)=C_p(\text{CO}_2)-C_p(\text{CO})-\tfrac12C_p(\text{O}_2)$.

  1. $\Delta S^\circ_{298}$. $$\Delta S^\circ_{298}=S^\circ(\text{CO}_2)-S^\circ(\text{CO})-\tfrac12S^\circ(\text{O}_2)=213.7-197.7-\tfrac12(205.1)=\boxed{-86.55\ \text{J}\,\text{K}^{-1}\text{mol}^{-1}}.$$
  2. Assemble $\Delta C_p(T)$. Collecting the constant, $T$, $T^2$ and $T^3$ coefficients of $C_p(\text{CO}_2)-C_p(\text{CO})-\tfrac12C_p(\text{O}_2)$ term by term: $$\Delta C_p(T)=-27.6+0.100\,T-1.11\times10^{-4}T^2+3.9\times10^{-8}T^3\ \ \text{J}\,\text{K}^{-1}\text{mol}^{-1}.$$
  3. Integrate $\Delta C_p/T$ from 298 to 500 K. Term by term, $\int(a/T+b+cT+dT^2)\,dT=a\ln T+bT+\tfrac{c}{2}T^2+\tfrac{d}{3}T^3$, evaluated between the limits: $$\Delta S_{corr}=-27.6\ln\!\frac{500}{298}+0.100(500-298)-5.55\times10^{-5}(500^2-298^2)+1.3\times10^{-8}(500^3-298^3)=\boxed{-1.75\ \text{J}\,\text{K}^{-1}\text{mol}^{-1}}.$$
  4. $\Delta S^\circ_{500}$. $$\Delta S^\circ_{500}=\Delta S^\circ_{298}+\Delta S_{corr}=-86.55-1.75=\boxed{-88.3\ \text{J}\,\text{K}^{-1}\text{mol}^{-1}}.$$ The entropy decrease is expected: 1.5 mol of gas (CO + ½O₂) becomes 1 mol of gas (CO₂), so the moles of gas fall — the dominant driver of $\Delta S^\circ<0$ here — and the small extra correction from 298 to 500 K barely changes that.
QuantityValue
$\Delta S^\circ_{298}$−86.55 J/K·mol
Kirchhoff correction (298→500 K)−1.75 J/K·mol
$\Delta S^\circ_{500}$−88.3 J/K·mol