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16-Civ-A3 Elementary Environmental Engineering · May 2018

Question 4 of 7: Material Balances, Reaction Kinetics and Microbiology

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

Notes on this paper

Paper format. National Exams, May 2018 — 16-Civ-A3 Elementary Environmental Engineering. Three hours; closed book with one candidate-prepared 8½ × 11 double-sided aid sheet; approved Casio or Sharp calculator only. Seven problems are printed, each worth 20 marks, and any five constitute a complete paper (maximum 100 marks). All seven are solved here, because the set is intended as a study resource rather than an exam script. Section marks are shown in brackets at the left margin of each question and are reproduced from the final-page Marking Scheme.

Reference texts.

Check: Problem 4(ii) quotes a rate constant as “20 dm6/mol2” with no time unit, and states the fundamental reaction 2A + B ⇌ C. It is solved as a forward-rate second-in-A/first-in-B rate law with $k=20\ \text{dm}^{6}\,\text{mol}^{-2}\,\text{s}^{-1}$ (the only reading that makes $-r_A=k\,C_A^{2}C_B$ dimensionally a rate); the time unit is taken as seconds per NOTE 1. Because no feed flow rate is supplied, the well-posed deliverable is the flow-independent space-time $\tau$ (with $V=\tau\,v_0$ for any stated feed basis), not an absolute volume.

Question 4: Material Balances, Reaction Kinetics and Microbiology (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.

Part (i) — Lead emission from a 2000 MW coal plant (6 marks)

Given. A coal-fired power plant is defined by the following data.

Given data — Problem 4(i)
QuantitySymbolValue
Net electrical outputPe2000 MW = 2.0 × 109 W
Overall (thermal) efficiencyη0.50
Higher heating value of coalHHV30 × 106 J/kg
Lead content of coalwPb0.1 µg/g = 0.1 × 10−6 kg/kg

Find. The mass of lead emitted per year (kg/yr), on a worst-case mass balance in which all lead in the fuel leaves with the flue gas (no capture in a precipitator or scrubber).

Approach. An energy balance converts electrical output to a coal-burning rate; a species mass balance on lead then follows the Pb from fuel to stack, and the rate is annualised.

  1. Energy balance → thermal input. Fuel heat is released at rate $\dot Q_{\text{in}}$, of which the fraction $\eta$ becomes electricity: $$\dot Q_{\text{in}}=\frac{P_e}{\eta}=\frac{2000}{0.50}=4000\ \text{MW}=4.0\times10^{9}\ \text{W}.$$
  2. Coal-burning rate. Dividing the heat rate by the heating value gives the fuel mass rate: $$\dot m_{\text{coal}}=\frac{\dot Q_{\text{in}}}{\text{HHV}}=\frac{4.0\times10^{9}\ \text{W}}{30\times10^{6}\ \text{J/kg}}=133.3\ \text{kg/s}.$$
  3. Lead mass balance. With a fuel lead fraction $w_{\text{Pb}}=0.1\times10^{-6}$ and all of it partitioning to the gas stream, $$\dot m_{\text{Pb}}=\dot m_{\text{coal}}\,w_{\text{Pb}}=133.3\times0.1\times10^{-6}=1.333\times10^{-5}\ \text{kg/s}.$$
  4. Annualise. Multiplying by the seconds in a year $(3.154\times10^{7}\ \text{s/yr})$: $$\boxed{\dot m_{\text{Pb}}=1.333\times10^{-5}\times3.154\times10^{7}\approx 4.2\times10^{2}\ \text{kg/yr}\;(\approx 420\ \text{kg/yr}).}$$
Check: This is the uncontrolled emission — it assumes every gram of fuel lead reaches the stack. In practice most lead condenses onto fly ash and is captured by an electrostatic precipitator or fabric filter (typically 90–99%), so the actual stack emission is roughly 4–40 kg/yr. The mass balance sizes the challenge to the control device rather than the release to atmosphere.

Part (ii) — CSTR for the gas-phase reaction 2A + B ⇌ C (6 marks)

Given. A constant-T, constant-P gas-phase CSTR with a variable number of moles.

Given data — Problem 4(ii)
QuantitySymbolValue
Reaction / rate law—2A + B ⇌ C,   $-r_A=k\,C_A^{2}C_B$
Temperature / pressureT, P500 K, 15 atm
Rate constantk20 dm6 mol−2 s−1
Feed compositionyA0, yB00.60 A, 0.40 B
Target conversionX0.99

Find. The CSTR volume (as the flow-independent space-time $\tau$, with $V=\tau v_0$) for 99% conversion of A.

Approach. Because total moles change, express $C_A$ and $C_B$ in terms of conversion with a mole-change factor $\varepsilon$, evaluate the rate at the exit composition (a CSTR operates at exit conditions), then apply the CSTR design equation.

  1. Mole-change factor. On a per-mole-A basis the reaction is $A+\tfrac12 B\rightarrow \tfrac12 C$, so $\delta=\tfrac12-1-\tfrac12=-1$ and $$\varepsilon=y_{A0}\,\delta=0.60\times(-1)=-0.60.$$
  2. Inlet concentrations. From the ideal-gas law with $R=0.082057\ \text{dm}^3\text{atm}\,\text{mol}^{-1}\text{K}^{-1}$: $$C_{T0}=\frac{P}{RT}=\frac{15}{0.082057\times500}=0.3656\ \tfrac{\text{mol}}{\text{dm}^3},\qquad C_{A0}=y_{A0}C_{T0}=0.2193\ \tfrac{\text{mol}}{\text{dm}^3}.$$ The feed ratio is $\theta_B=y_{B0}/y_{A0}=0.6667$.
  3. Exit concentrations at X = 0.99. With $C_A=C_{A0}\dfrac{1-X}{1+\varepsilon X}$ and $C_B=C_{A0}\dfrac{\theta_B-\tfrac12 X}{1+\varepsilon X}$, and denominator $1+\varepsilon X = 1-0.594 = 0.406$: $$C_A=0.2193\times\frac{0.01}{0.406}=5.40\times10^{-3}\ \tfrac{\text{mol}}{\text{dm}^3},\qquad C_B=0.2193\times\frac{0.6667-0.495}{0.406}=9.28\times10^{-2}\ \tfrac{\text{mol}}{\text{dm}^3}.$$
  4. Rate at the exit. $$-r_A=k\,C_A^{2}C_B=20\times(5.40\times10^{-3})^{2}\times9.28\times10^{-2}=5.41\times10^{-5}\ \tfrac{\text{mol}}{\text{dm}^3\text{s}}.$$
  5. CSTR design equation (space-time). With $\tau=V/v_0$ and $C_{A0}X=(-r_A)\tau$, $$\boxed{\tau=\frac{C_{A0}\,X}{-r_A}=\frac{0.2193\times0.99}{5.41\times10^{-5}}\approx 4.0\times10^{3}\ \text{s}\;(\approx 67\ \text{min}),\qquad V=\tau\,v_0\approx 4.0\ \text{m}^3\ \text{per (dm}^3\text{/s) of feed.}}$$
Check: No feed flow rate is given, so an absolute volume cannot be stated; the space-time $\tau\approx4.0\times10^{3}$ s is the flow-independent result, and $V=\tau v_0$ (e.g. $\approx4.0\ \text{m}^3$ for a 1 dm3/s feed). The large $\tau$ is expected: a CSTR runs entirely at the low exit concentration where a second-order-in-A rate is slowest, so it needs far more volume than a plug-flow reactor for the same 99% conversion.

Part (iii) — UV disinfection: resistance order and 99.9% doses (8 marks)

A UV dose–response (fluence–response) curve plots log inactivation against UV dose; the steeper the curve, the less resistant the organism, because a smaller dose achieves the same log kill. Reading the four series in the figure at the 99.9% (3-log) level gives the ranking and doses below. The figure is reconstructed as an inline plot from the described data.

99.9% (3-log) level 0 1 2 3 4 5 6 0 20 40 60 80 100 UV Dose (mJ/cm²) Log Inactivation E. coli Total coliform (ww) Rotavirus B. subtilis spores
UV dose–response curves. The dashed line marks 3-log (99.9%) inactivation; where each curve crosses it gives the required dose.

Order of resistance (highest to lowest): B. subtilis spores > Rotavirus > Total coliform (wastewater) > E. coli. Spores and viruses are far more UV-resistant than vegetative bacteria; the bacterial spore is the most resistant of the four. The reads at the 99.9% (3-log) level are collected below.

Approximate UV dose for 99.9% (3-log) inactivation
MicroorganismRelative resistanceUV dose for 3-log (mJ/cm²)
B. subtilis sporesHighest≈ 70–75
RotavirusHigh≈ 30
Total coliform (wastewater)Moderate (tails)≈ 13
E. coliLowest≈ 9
Check: Doses are read graphically from the described curve and are approximate. The total-coliform curve tails (approaches a plateau near 4.5–5 log), so pushing beyond 3-log for that population needs disproportionately more dose — a practical caution when a wastewater UV system must meet a strict effluent limit.