18-Env-A2 Hydrology and Municipal Hydraulics Engineering · December 2016
Question 4 of 7
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Exams — December 2016 — 04-Env-A2 Hydrology and Municipal Hydraulics Engineering (3 hours, closed book with an 8½×11 candidate aid-sheet). Instructions state any five (5) of the seven problems constitute a complete paper (100 marks); all seven are solved in full below for completeness.
Reference texts: Linsley, Kohler & Paulhus, Hydrology for Engineers; Chow, Open-Channel Hydraulics; Walski et al., Advanced Water Distribution Modeling and Management; Davis & Cornwell, Introduction to Environmental Engineering.
(i) Recession curve, base flow and direct runoff (6 marks)
Fig. 3 — Labelled schematic of a typical runoff hydrograph.
Direct runoff is the "excess" rainfall component that reaches the stream quickly — via overland flow and shallow interflow — during and shortly after a storm; it produces the sharp rising limb and peak of the hydrograph. Base flow is the sustained, slowly varying component of streamflow sourced from groundwater discharge into the channel; it persists between storms and is what keeps a stream flowing during dry weather. The recession curve is the falling limb of the hydrograph after the peak, and specifically its tail once direct runoff has essentially drained away, represents the depletion of bank/aquifer storage discharging back to the stream; it typically follows an exponential decay ($Q_t = Q_0 e^{-kt}$) and its shape (the recession constant $k$) is itself a useful indicator of the basin's groundwater storage characteristics. Hydrograph separation techniques use the recession curve, extrapolated backward under the storm peak, to split total streamflow into its base-flow and direct-runoff components.
(ii) Two main factors affecting hydrograph shape (6 marks)
Watershed physiographic characteristics (size, shape, slope and drainage density). A small, steep, compact watershed with a dense drainage network concentrates runoff quickly, producing a short time-to-peak, a high sharp peak and a rapid recession; a large, flat, elongated watershed spreads the runoff contribution over a much longer travel time, producing a lower, broader, more delayed peak. This directly affects hydrograph analysis because the unit hydrograph's time base and peak must be scaled (or an entirely different unit hydrograph derived) for basins of different physiographic character — a unit hydrograph is not transferable between dissimilar watersheds without adjustment.
Storm characteristics (rainfall intensity, duration and spatial/temporal distribution over the basin, including storm movement direction). A high-intensity, short-duration storm produces a sharply peaked hydrograph, while a low-intensity, long-duration storm produces a flatter, more prolonged response; a storm cell moving in the downstream direction of the drainage network increases the peak discharge (successive sub-basin contributions arrive in closer succession) compared with the same storm moving upstream. This matters for hydrograph analysis because the same total rainfall volume can produce very different peak flows and timing depending on how the storm is distributed, so a single design storm hyetograph must be chosen carefully (and storm movement considered) when deriving a design hydrograph.
(iii) Pump total dynamic head and brake horse power (8 marks)
Fig. 4 — Pump configuration: intake screen, pump and PVC discharge pipe with static lift ΔElev = 31 m.
Given.
Quantity
Value
Static elevation lift, $\Delta\text{Elev}$
31 m
Pipe length, $L$ (PVC)
1500 m
Friction factor, $f$ (Darcy)
0.014
Pipe diameter, $D$
295 mm
Flow rate, $Q$
102 L/s $= 0.102\ \text{m}^3/\text{s}$
Pump efficiency, $E_{pump}$
0.70
Find. Total dynamic head (TDH) and brake horse power (BHP), with all losses other than pipe friction and static lift taken as negligible (as stated).
Approach. $\text{TDH} = \Delta\text{Elev} + H_f$ (Darcy–Weisbach friction loss added to the static lift), then the hydraulic (water) power $\rho g Q\,\text{TDH}$ is divided by pump efficiency to obtain the shaft (brake) power.
Velocity in the pipe. $A = \dfrac{\pi}{4}D^2 = \dfrac{\pi}{4}(0.295)^2 = 0.06835\ \text{m}^2$.
$$V = \frac{Q}{A} = \frac{0.102}{0.06835} = 1.49\ \text{m/s}$$
Friction head loss (Darcy–Weisbach).
$$H_f = f\,\frac{L}{D}\,\frac{V^2}{2g} = 0.014\times\frac{1500}{0.295}\times\frac{1.49^2}{2(9.81)} = 8.08\ \text{m}$$
Total dynamic head. With velocity head and minor losses stated negligible,
$$\text{TDH} = \Delta\text{Elev} + H_f = 31 + 8.08 = \boxed{39.1\ \text{m}}$$
Brake horse power. Hydraulic power delivered to the water,
$$P_{hyd} = \rho g Q\,\text{TDH} = 1000\times9.81\times0.102\times39.1 = 39{,}100\ \text{W} = 39.1\ \text{kW}$$
Dividing by pump efficiency for the required shaft input,
$$\text{BHP} = \frac{P_{hyd}}{E_{pump}} = \frac{39.1}{0.70} = \boxed{55.9\ \text{kW} \approx 74.9\ \text{hp}}$$