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23-Chem-A3 Heat and Mass Transfer · December 2017

Question 4 of 6: Part B: Vapour–Liquid Equilibrium of Benzene–Toluene

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

Notes on this paper

National Exams — December 2017 — 16-Chem-A3 Heat and Mass Transfer. Three-hour, open-book exam (one textbook of the candidate’s choice; any non-communicating calculator). Format: two parts — Part A — Heat Transfer (Q1–Q3) and Part B — Mass Transfer (Q4–Q6). All problems are worth 25 points; the rubric requires at least two problems attempted from each part and marks only the first two per part, so a complete paper is four questions (100 points). All six problems are solved below for completeness. Property data are quoted as stated in each problem; where a value applies to a film condition it is used at the stated film temperature.

Reference texts: F. P. Incropera & D. P. DeWitt, Fundamentals of Heat and Mass Transfer (Wiley) — free/forced convection correlations, conduction shape factors, the heat–mass-transfer analogy; J. P. Holman, Heat Transfer (McGraw-Hill) — natural-convection constants $C,m$ and cylinder conduction; R. E. Treybal, Mass-Transfer Operations (McGraw-Hill) — wetted-wall $k_G$, gas absorption and the Chilton–Colburn analogy; R. B. Bird, W. E. Stewart & E. N. Lightfoot, Transport Phenomena (Wiley); supporting property data from Perry’s Chemical Engineers’ Handbook (9th ed.).

Question 4 — Part B: Vapour–Liquid Equilibrium of Benzene–Toluene (25 points)

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.

Given. Benzene (1) and toluene (2) form a nearly ideal solution, so Raoult’s law applies: $P = x_1 P_1^{\text{sat}} + (1-x_1)P_2^{\text{sat}}$ and $y_1 = x_1 P_1^{\text{sat}}/P$, with the total pressure fixed at $P=101.32$ kPa. Pure-component vapour pressures are tabulated versus temperature (benzene boils at 80.0 °C, toluene at 110.1 °C, where each pure vapour pressure equals 101.32 kPa).

Find. (a) the equilibrium pairs $(x_1,y_1)$ at each temperature; (b) an empirical $y_1$–$x_1$ relation (relative volatility form).

0.00.20.40.60.81.080859095100105110mole fraction benzene, x or yTemperature, °Cbubble (liquid, x)dew (vapor, y)
Figure 4 — Boiling-point (T–x–y) diagram for benzene–toluene at 101.32 kPa, computed below. The lower (blue) curve is the bubble line $T$ vs. liquid $x_1$; the upper (red) curve is the dew line $T$ vs. vapour $y_1$; benzene is the more volatile component.

Approach. At each tabulated temperature the total pressure must equal 101.32 kPa; a lever on the two pure vapour pressures gives the liquid composition $x_1=(P-P_2^{\text{sat}})/(P_1^{\text{sat}}-P_2^{\text{sat}})$, and Raoult’s law then gives $y_1$. Averaging the ratio $\alpha=P_1^{\text{sat}}/P_2^{\text{sat}}$ across the range yields a single-parameter $y$–$x$ curve.

  1. Bubble-point lever for the liquid composition. Because $P=x_1P_1^{\text{sat}}+(1-x_1)P_2^{\text{sat}}=101.32$ kPa at every equilibrium temperature, $$x_1 = \frac{P - P_2^{\text{sat}}}{P_1^{\text{sat}} - P_2^{\text{sat}}}.$$ For example at 92.9... (worked point) $T=93.3$ °C: $x_1=(101.32-60.26)/(149.72-60.26)=0.459$.
  2. Raoult’s law for the vapour composition. The vapour benzene fraction is $$y_1 = \frac{x_1 P_1^{\text{sat}}}{P}.$$ At $T=93.3$ °C, $y_1 = (0.459)(149.72)/101.32 = 0.678$. Repeating at every temperature gives the full VLE table:
T (°C)$P_1^{\text{sat}}$ (kPa)$P_2^{\text{sat}}$ (kPa)$x_1$ (benzene)$y_1$ (benzene)
80.0101.32—1.0001.000
82.9108.1241.860.8970.958
85.0117.6046.000.7730.897
87.0127.6050.400.6600.831
90.5138.2555.200.5550.758
93.3149.7260.260.4590.678
96.1161.8565.860.3690.590
99.0174.6571.730.2880.496
101.6188.2578.000.2120.393
104.5202.6584.660.1410.282
107.2216.6591.860.0760.162
110.0234.1199.590.0130.030
110.1—101.320.0000.000
  1. Empirical relation via average relative volatility. The relative volatility $\alpha=P_1^{\text{sat}}/P_2^{\text{sat}}$ varies only mildly (2.58 at 82.9 °C down to 2.35 at 110 °C); its mean is $\bar\alpha=2.46$. The constant-$\alpha$ equilibrium curve then compactly represents the whole table: $$\boxed{y_1 = \frac{\bar\alpha\,x_1}{1+(\bar\alpha-1)x_1} = \frac{2.46\,x_1}{1+1.46\,x_1}}.$$ As a check at $x_1=0.5$ this gives $y_1=0.71$, matching the tabulated trend. That is part (b).
QuantityResult
(a) VLE data at 101.32 kPa13-point $(x_1,y_1)$ table above (T–x–y in Fig. 4)
Average relative volatility $\bar\alpha$2.46
(b) Empirical relation$y_1 = 2.46\,x_1/(1+1.46\,x_1)$