18-Env-A2 Hydrology and Municipal Hydraulics Engineering · May 2017
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
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.
| Quantity | Value |
|---|---|
| Length, $L$ | 1200 m |
| Diameter, $d$ | 400 mm = 0.400 m |
| Full-flow velocity, $V$ | 2.5 m/s |
| Kinematic viscosity, $\nu$ (water, $\approx$20 °C) | $1.0\times10^{-6}\ \text{m}^2/\text{s}$ |
| Concrete roughness height, $\varepsilon$ (assumed, smooth-finished) | 0.3 mm |
Find. $Q$ in m³/min; $Re$ and flow type; head loss $H_f$.
Approach. Continuity gives $Q=VA$; $Re=Vd/\nu$ classifies the flow; the Darcy–Weisbach equation with a friction factor from the explicit Swamee–Jain fit (equivalent to reading the Moody chart at this $Re$ and relative roughness) gives $H_f$.
| Quantity | Value |
|---|---|
| Flow rate, $Q$ | 18.85 m³/min |
| Reynolds number, $Re$ | $1.00\times10^6$ (turbulent) |
| Friction factor, $f$ | 0.0188 |
| Head loss, $H_f$ | 17.97 m over 1200 m |
Waterhammer is the transient pressure surge generated when a moving column of water is suddenly decelerated, converting its momentum into a pressure wave that travels back and forth through the pipe at (near) the speed of sound in water. Two potential causes are: (1) rapid valve closure — a valve (including a check valve slamming shut) closed faster than the pipeline's critical closure time reflects the full momentum of the flowing column into a pressure spike; and (2) sudden pump trip/power failure — loss of power stops the pump essentially instantaneously while the water column in the discharge main continues moving under its own inertia, and the resulting flow reversal against a closing check valve produces a severe surge.
Two potential solutions are: (1) controlled (slow) valve operation and surge-anticipating/soft-closing check valves — extending the closure time beyond the pipeline's critical period (based on the pressure-wave travel time) allows the surge to dissipate gradually rather than reflect as a sharp spike; and (2) surge-control devices such as air/vacuum-relief valves, surge (relief) valves set to open above a threshold pressure, or a surge tank/standpipe/air chamber on the discharge main, which absorb or vent the transient energy before it can damage the pipe, joints or fittings.
Conceptual models of runoff represent a catchment's rainfall-runoff response as a simplified system of interconnected linear or non-linear storage elements (e.g., a cascade of linear reservoirs, or the widely used unit-hydrograph approach itself) whose parameters are calibrated against observed rainfall and streamflow records rather than derived purely from first-principles physics; they are used operationally for design-storm hydrograph generation, flood forecasting and reservoir/detention-pond routing because they are computationally simple and only need a modest calibration dataset. Two important differences from analytical (physically-based) models are: (1) basis of the governing equations — conceptual models use empirical storage–discharge relationships calibrated to fit observed behaviour, while analytical models solve the actual physical equations of motion (e.g., the kinematic-wave or full St. Venant equations for overland and channel flow) from first principles using measured physical parameters (slope, roughness, geometry); and (2) data and transferability — a conceptual model's calibrated parameters are specific to the gauged catchment they were fit to and transfer poorly to an ungauged basin, whereas an analytical model's physically-based parameters can, in principle, be estimated from maps and surveys and applied to an ungauged catchment, at the cost of much greater data and computational demand.