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18-Env-A2 Hydrology and Municipal Hydraulics Engineering · Undated paper

Question 4 of 7

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

Notes on this paper

National Exams — May 2019 — 18-Env-A2 / Hydrology and Municipal Hydraulics Engineering. 3 hours duration; closed book with an 8.5×11 in double-sided aid sheet; Casio or Sharp approved calculator only. Any five questions constitute a complete paper (only the first five answers in the work book are marked); all seven Problems are solved below for completeness. Each question is worth 20 marks.

Reference texts. Linsley, Kohler & Paulhus, Hydrology for Engineers (3rd ed.); Chow, Open-Channel Hydraulics; Walski et al., Advanced Water Distribution Modeling and Management; Metcalf & Eddy, Wastewater Engineering: Treatment and Resource Recovery (5th ed.); Davis & Cornwell, Introduction to Environmental Engineering (6th ed.); Guidelines for Canadian Drinking Water Quality (Health Canada); Canadian Council of Ministers of the Environment (CCME) water-quality guidelines.

Problem 4 (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) Steel pipe: flow rate, Reynolds number, head loss (7 marks)

Given.

QuantityValue
Length, $L$2000 m
Diameter, $D$400 mm = 0.400 m
Full-flow velocity, $V$4 m/s
Manning's $n$ (steel, as given)0.015
Kinematic viscosity, $\nu$ (water)$1.0\times10^{-6}\ \text{m}^2/\text{s}$

Find. (a) $Q$; (b) $Re$ and flow type; (c) $H_f$ in m.

Approach. $Q$ from continuity; classify with $Re$; since a Manning's $n$ is given (rather than a roughness height), back out the slope implied by Manning's equation at this $V$ and $D$, then convert to head loss over the pipe length.

  1. Part (a) — flow rate.$$A=\frac{\pi D^2}{4}=0.1257\ \text{m}^2\qquad Q=VA=(4)(0.1257)=\boxed{0.5027\ \text{m}^3/\text{s}}=30.16\ \text{m}^3/\text{min}$$
  2. Part (b) — Reynolds number.$$Re=\frac{VD}{\nu}=\frac{(4)(0.400)}{1.0\times10^{-6}}=\boxed{1.60\times10^{6}}$$Since $Re\gg4000$, the flow is turbulent.
  3. Part (c) — friction head loss via Manning's equation. For full flow $R=D/4$; solve Manning's equation for the slope consistent with the given $n$, $D$ and $V$, then $H_f=SL$:$$S=\left(\frac{Vn}{R^{2/3}}\right)^2=\left(\frac{(4)(0.015)}{(0.100)^{2/3}}\right)^2=0.07756\ (=7.756\%)$$$$H_f=SL=(0.07756)(2000)=\boxed{155.1\ \text{m}}$$
QuantityValue
Flow rate, $Q$0.5027 m³/s (30.16 m³/min)
Reynolds number, $Re$1.60×10&sup6; (turbulent)
Implied pipe slope7.756%
Friction head loss, $H_f$155.1 m
Check: sustaining $V=4$ m/s in a 400 mm steel pipe at the given $n=0.015$ (unusually rough for steel, more typical of an old, tuberculated main than new steel pipe) requires a steep 7.76% implied grade, so the 2000 m run loses 155.1 m of head — solved exactly from the data given rather than substituted with a more typical smooth-steel $n\approx0.011$–0.013.

(ii) Three main functions/design aspects of distribution systems (6 marks)

(1) Conveyance and pressure maintenance (transmission/distribution mains). The pipe network's primary function is delivering treated water from the source/treatment plant to every service connection while maintaining a minimum positive pressure everywhere in the system at all times (typically ≥140–350 kPa depending on jurisdiction) — the governing design/operation constraint, since a pressure loss anywhere risks pathogen intrusion through leaking joints and cross-connections.

(2) Storage and demand equalization (reservoirs/elevated tanks). Storage facilities buffer the mismatch between a relatively constant treatment/pumping rate and highly variable diurnal demand, and provide the emergency and fire-flow reserve that would otherwise require oversizing every pipe and pump in the network; their operational aspect is water age — poor turnover in an oversized or poorly-mixed tank lets disinfectant residual decay and can promote nitrification, so tank sizing/turnover is a direct water-quality decision.

(3) Pressure boosting and zoning (pumping stations and pressure zones). Pumping stations supply the energy to overcome elevation change and friction loss across the service area; in areas with large elevation differences, the system is divided into separate pressure zones (each with its own hydraulic grade line, connected by pressure-reducing valves or booster pumps) so that no zone experiences either sub-minimum pressure (at high elevation) or excessive, main-damaging pressure (at low elevation) — a core design aspect governing both reliability and pipe-material/pressure-class selection.

(iii) Conceptual model for predicting runoff: use and limitations (7 marks)

A widely used conceptual model for predicting runoff is the SCS (NRCS) Curve Number method combined with a synthetic unit hydrograph: rainfall excess is computed from a lumped Curve Number (CN, representing the watershed's hydrologic soil group, land cover and antecedent moisture condition) via the SCS runoff equation, and that excess rainfall is convolved with a dimensionless synthetic unit hydrograph to produce the full runoff hydrograph, including its peak and volume. Its use is to allow reasonable design-storm runoff estimates on ungauged or sparsely-gauged watersheds, where a full physically-based distributed model cannot be calibrated for lack of data, using only readily available soil-survey and land-cover information.

Limitation 1 — lumped, non-physical parameterization. Curve Number and the unit-hydrograph time parameters are empirically-fitted lumped representations, not physically measured quantities, so the model can reproduce an observed peak flow for the "wrong" physical reason (e.g., over-estimating infiltration loss while compensating with an error in the timing parameter); this limits its reliability when extrapolated well beyond the conditions (soil groups, storm sizes, land uses) under which the original SCS curve-number tables were developed.

Limitation 2 — no explicit treatment of antecedent conditions or storm pattern. The standard SCS method assumes a single antecedent-moisture class and a fixed (Type II, etc.) design rainfall temporal pattern; it does not dynamically track soil moisture between storms or respond to a real, irregular rainfall hyetograph the way a continuous physically-based model would, so it is poorly suited to continuous simulation (e.g., a multi-storm wet season) or to watersheds whose antecedent-moisture behaviour differs materially from the standard assumption (e.g., strongly seasonal frozen-ground conditions).