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18-Env-A1 Principles of Environmental Engineering · December 2016

Question 7 of 7: Particle Characteristics, Chemistry of Solutions and Thermal Pollution

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

Notes on this paper

National Exams — December 2016 — 04-Env-A1 / Principles of Environmental Engineering. 3 hours duration; closed book with a candidate-prepared 8.5×11 in double-sided aid sheet; Casio or Sharp approved calculator only. Any five questions constitute a complete paper (first five answers marked); all seven are solved below for completeness. Each question is worth 20 marks.

Reference texts. Davis & Cornwell, Introduction to Environmental Engineering (6th ed.); Metcalf & Eddy, Wastewater Engineering: Treatment and Resource Recovery (5th ed.); MWH’s Water Treatment: Principles and Design (3rd ed.); Sawyer, McCarty & Parkin, Chemistry for Environmental Engineering and Science; Guidelines for Canadian Drinking Water Quality (Health Canada); Canadian Council of Ministers of the Environment (CCME) water-quality and municipal solid-waste guidelines; Canadian Environmental Protection Act, 1999 (CEPA) and Canadian Environmental Assessment Act (CEAA 2012); ISO 14040/14044 (Life Cycle Assessment); Bies & Hansen, Engineering Noise Control; Andrews, Canadian Professional Engineering and Geoscience (professional ethics).

Question 7: Particle Characteristics, Chemistry of Solutions and Thermal Pollution (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.

(i) Coagulation and Flocculation in Water/Wastewater Treatment

Coagulation is the chemical destabilization of colloidal particles: a coagulant (e.g., alum, ferric chloride, or a cationic polymer) is dosed and rapidly, intensely mixed into the water so it neutralizes the negative surface charge that normally keeps colloidal particles apart (charge neutralization) and/or compresses the electrical double layer surrounding each particle, removing the electrostatic repulsion that otherwise prevents particles from approaching one another. Flocculation is the subsequent physical process of gentle, prolonged mixing (low velocity gradient $G$, longer detention time than the rapid-mix step) that promotes particle–particle collisions among the now-destabilized colloids, allowing them to aggregate into larger, denser flocs. Together, coagulation removes the repulsive barrier and flocculation supplies the collision opportunity for aggregation, converting turbidity-causing colloidal particles — which are individually far too small and too slow-settling to remove by gravity alone — into flocs large and dense enough to be removed efficiently by downstream sedimentation and/or filtration. This coagulation–flocculation–sedimentation–filtration sequence is the core physicochemical pretreatment train in conventional water treatment, and an analogous chemically-enhanced coagulation step is also used in wastewater treatment to enhance phosphorus and solids removal.

(ii) Hardness of Lake Huron Water as CaCO₃

Given. Average ion concentrations near the salt quarry, with atomic weights Ca = 40, Mg = 24, Cu = 64, C = 12, O = 16 (so CaCO₃ molar mass = 100):

Given ion concentrations
IonConcentrationEquivalent weight (atomic wt. ÷ valence)
Ca²⁺100 mg/L40/2 = 20
Mg²⁺80 mg/L24/2 = 12
Cu²⁺50 mg/L64/2 = 32

Find. Total hardness in mg/L as CaCO₃, and the water's hardness classification.

Approach. Total hardness is conventionally defined (Standard Methods) as the sum of the Ca²⁺ and Mg²⁺ equivalents expressed as CaCO₃ — Cu²⁺ is not a hardness-forming cation under this definition (it is not one of the alkaline-earth divalent cations that hardness classically refers to) and is a decoy value in this dataset, not part of the hardness sum. Convert each hardness-causing ion's concentration to a CaCO₃-equivalent using the ratio of equivalent weights, then sum and compare to standard hardness classification bands.

  1. Convert Ca²⁺ to CaCO₃ equivalent. $$H_{Ca} = 100\ \text{mg/L} \times \frac{50}{20} = 250\ \text{mg/L as CaCO}_3.$$
  2. Convert Mg²⁺ to CaCO₃ equivalent. $$H_{Mg} = 80\ \text{mg/L} \times \frac{50}{12} = 333.3\ \text{mg/L as CaCO}_3.$$
  3. Sum for total hardness (Cu²⁺ excluded — not a hardness ion). $$\boxed{H_{total} = H_{Ca} + H_{Mg} = 250 + 333.3 = 583.3\ \text{mg/L as CaCO}_3.}$$
  4. Classify against standard hardness bands. Soft < 75, moderately hard 75–150, hard 150–300, very hard > 300 mg/L as CaCO₃. At 583.3 mg/L, the water is classified as very hard.
QuantityValue
Hardness from Ca²⁺250.0 mg/L as CaCO₃
Hardness from Mg²⁺333.3 mg/L as CaCO₃
Total hardness583.3 mg/L as CaCO₃
ClassificationVery hard (> 300 mg/L as CaCO₃)

(iii) Downstream River Temperature After Cooling-Tower Discharge

Given. A cooling-tower discharge mixes with the upstream river before the downstream measurement point.

Given data
QuantitySymbolValue
Cooling-tower discharge flow$Q_c$400 m³/s
Cooling-tower discharge temperature$T_c$70 °C
Upstream river temperature$T_s$20 °C
Total downstream flow$Q$500 m³/s
RiverConfluenceCooling-tower dischargeQc = 400 m3/s, Tc = 70 degCUpstream riverQs = 100 m3/s, Ts = 20 degCDownstream riverQ = 500 m3/s, T = ? degC
Cooling-tower discharge ($Q_c$, $T_c$) mixing with the upstream river ($Q_s = Q-Q_c$, $T_s$) to give the downstream temperature $T$.

Find. The downstream river temperature $T$ immediately after complete mixing.

Approach. The upstream river flow is the balance of the total downstream flow not accounted for by the cooling-tower discharge ($Q_s = Q - Q_c$); apply a steady-state thermal energy balance (equivalent to a flow-weighted average temperature, since density and specific heat are effectively constant over this range) across the mixing point.

  1. Find the upstream river flow rate by continuity. $$Q_s = Q - Q_c = 500 - 400 = 100\ \text{m}^3/\text{s}.$$
  2. Write the steady-state thermal energy balance at the mixing point. With constant $\rho$ and $c_p$, the energy balance reduces to a flow-weighted temperature average: $$QT = Q_cT_c + Q_sT_s.$$
  3. Solve for the downstream temperature. $$T = \frac{Q_cT_c + Q_sT_s}{Q} = \frac{(400)(70) + (100)(20)}{500} = \frac{28000+2000}{500} = \boxed{60\ ^\circ\text{C}}.$$
QuantityValue
Upstream river flow, $Q_s$100 m³/s
Downstream river temperature, $T$60 °C
Check
Assumes complete, instantaneous cross-sectional mixing at the confluence and negligible heat loss to the atmosphere between the discharge point and the downstream measurement location (a short mixing reach); density and specific heat of water are treated as constant over the 20–70 °C range for the energy balance.

A downstream temperature of 60 °C is far above any cold-water fishery tolerance (typically well under 20 °C for salmonids), so mitigation is required. Two engineering solutions: (1) reduce the discharge temperature at the source by adding a supplementary cooling stage (a wet or dry cooling tower cell, or an engineered cooling pond) so $T_c$ is lowered before the cooling water ever reaches the river, which is the most direct fix since it reduces the driving temperature difference itself; and (2) diffuse the discharge to increase effective initial dilution using a multi-port diffuser across the river cross-section instead of a single discharge point, which increases the effective mixing flow at the point of discharge and lowers the peak near-field temperature the fishery is exposed to, even though the far-field mixed temperature is governed by the same overall energy balance.

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