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18-Env-A3 Geotechnical and Hydrogeological Engineering · May 2016

Question 4 of 6: Unconfined Aquifer Well Yield & Source-Water Protection Area

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

Notes on this paper

National Exams — May 2016 — 04-Env-A3 / Geotechnical & Hydrogeological Engineering. 3 hours duration; open book exam, any non-communicating calculator permitted. FIVE (5) questions constitute a complete exam paper (the first five as they appear in the answer book are marked, 20 marks each, 100 marks total); all six printed questions are solved below for completeness.

Reference texts. Braja M. Das, Principles of Geotechnical Engineering (9th ed.) — weight–volume relations, USCS classification, seepage/flow nets, consolidation and bearing-capacity chapters; Craig & Knappett, Craig's Soil Mechanics (8th ed.) — cross-reference for seepage and flow-net theory; Freeze & Cherry, Groundwater (1979) — Darcy's law, the Dupuit–Thiem equation for an unconfined well, and wellhead time-of-travel capture zones.

Question 4: Unconfined Aquifer Well Yield & Source-Water Protection Area (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.

Given.

Given data
QuantitySymbolValue
Well diameter$2r_w$20 cm ($r_w=0.10$ m)
Aquifer porosity$n$0.25
Saturated hydraulic conductivity$K$10 m/day
Undisturbed saturated thickness$h_0$15 m
Max. allowable drawdown at the well$s_w$7.5 m
Underlying clay till conductivity—$10^{-6}$ cm/s (aquitard)

[Figure not reproduced: Figure 3 — unconfined aquifer with a single pumping well (schematic, redrawn from the source figure's setup; not to numeric scale). The underlying clay till (k ≈ 8.6×10 -4 m/day, five orders of magnitude below the sand) acts as the aquifer's effectively impermeable base. See the official exam paper.]

Find. (a) maximum sustainable discharge $Q$; (b) area protected by a 1-year time-of-travel capture zone around the well, at that discharge.

Approach. Use the Dupuit–Thiem equation for steady radial flow to a well in an unconfined aquifer, $Q=\pi K(h_0^2-h_w^2)/\ln(R/r_w)$. The source doesn't give an observation-well distance, so (per Note 1 on the exam, "state your assumptions") the radius of influence $R$ is estimated with Sichardt's empirical formula, standard practice for a single-well test with no observation data. Part (b) then uses a simple cylindrical-flow mass balance: the water pumped in one year must be supplied from the pore volume of a circular capture zone of the undisturbed aquifer thickness.

  1. Part (a) — radius of influence (Sichardt's formula) and drawdown geometry. With $K=10\ \text{m/day}=1.157\times10^{-4}\ \text{m/s}$ and $s_w=7.5$ m, $$R=3000\,s_w\sqrt{K_{[\text{m/s}]}}=3000\times7.5\times\sqrt{1.157\times10^{-4}}=\boxed{242\ \text{m}}.$$ The saturated thickness at the well is $h_w=h_0-s_w=15-7.5=\boxed{7.5\ \text{m}}$.
  2. Apply the Dupuit–Thiem equation. $$Q=\frac{\pi K\left(h_0^2-h_w^2\right)}{\ln(R/r_w)}=\frac{\pi\times10\times(15^2-7.5^2)}{\ln(242/0.10)}=\frac{\pi\times10\times168.75}{7.79}=\boxed{680\ \text{m}^3/\text{day}}.$$
  3. Part (b) — 1-year capture-zone volume. The volume pumped in one year is $$V=Q\,t=680\times365=\boxed{248{,}400\ \text{m}^3}.$$ Idealizing the capture zone as a cylinder of the undisturbed aquifer thickness $h_0$ and porosity $n$ (radial flow, mass balance: pumped volume = pore volume drained from the zone), $$\text{Area}=\frac{V}{n\,h_0}=\frac{248{,}400}{0.25\times15}=\boxed{66{,}200\ \text{m}^2\ (\approx6.6\ \text{ha})},\qquad r=\sqrt{\frac{\text{Area}}{\pi}}=\boxed{145\ \text{m}}.$$ This radius (145 m) is comfortably inside the assumed 242 m radius of influence, as it must be — a useful check that the assumption in Step 1 is at least self-consistent.
Check: engineering assumption — the figure shown with this question is the generic Thiem/Dupuit well-hydraulics setup (observation wells, $r_1$/$r_2$/$h_1$/$h_2$ labels) with no numeric distances printed anywhere in the source text or figure, so a radius of influence must be assumed to close the problem; Sichardt's empirical formula ($R=3000\,s_w\sqrt{K}$, K in m/s) is used as a standard, citable estimate for exactly this "single well, no observation data" case. Because $Q$ depends on $R$ only through $\ln(R/r_w)$, a ±50% error in the assumed R changes Q by only about ±7%, so the answer is not highly sensitive to this choice. Part (b) similarly assumes the undisturbed thickness $h_0$ (rather than the locally-drawn-down thickness) represents the capture zone, standard practice since most of its area lies well outside the cone of depression.
QuantityValue
Assumed radius of influence, $R$ (Sichardt)242 m
$h_0$, $h_w$15 m, 7.5 m
(a) Max. discharge, $Q$680 m³/day
1-yr pumped volume248,400 m³
(b) 1-yr protection area≈66,200 m² (r ≈ 145 m)