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18-Geol-A2 Hydrogeology · May 2018

Question 4 of 5: Step-Rate Pump Test Superposition, Two-Well Unconfined Flow, and Areal Recharge

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

Notes on this paper

National Exams — May 2018 — 04-Geol-A2 Hydrogeology. Three-hour, open-book exam; any non-communicating calculator permitted. Five questions constitute a complete paper and all five are of equal value; most call for an essay-format answer with clarity and organization counted. Unless stated otherwise, water density is taken as 1000 kg/m³, water viscosity as 0.001 kg/m-sec, and g as 9.81 m/s².

Reference texts: Freeze & Cherry, Groundwater (Prentice-Hall, 1979) — Darcy's law and anisotropic conductivity tensors, soil phase relations, permeameter testing, layered-medium effective conductivity, the Theis and Thiem well equations, image-well boundary methods, leaky-aquifer (Hantush-Jacob) theory, the Dupuit-Forchheimer approximation with areal recharge, and slug-test analysis (Hvorslev, Bouwer-Rice, Cooper-Bredehoeft-Papadopulos); Todd & Mays, Groundwater Hydrology — supplementary well-test and unconfined-flow methods; EGBC Geoscience Professional Practice Guidelines for assumption-disclosure conventions on open-book calculations.

Question 4: Step-Rate Pump Test Superposition, Two-Well Unconfined Flow, and Areal Recharge (equal value)

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. (a) Confined aquifer $b=40$ m, $K=1.3\times10^{-3}$ cm/sec, $S_s=1.2\times10^{-5}\ \text{m}^{-1}$; pump rate 8 L/s for the first 12 h, then 5 L/s for the next 12 h, then shut off; drawdown wanted at $r=100$ m, $t=36$ h. (b) Unconfined aquifer $K=3\times10^{-3}$ cm/sec, width 2400 m, porosity $n_e=0.33$, base 30 m below ground; two wells 150 m apart, water levels 8 m and 11 m below ground; no recharge. (c) vertical recharge 0.25 m/yr added, otherwise unchanged.

Find. (a) drawdown at $r=100$ m, 36 h after the start of the multi-rate test. (b) (i) total flow through the aquifer, (ii) head halfway between the wells, (iii) pore (linear) velocity halfway between the wells. (c) head halfway between the wells once areal recharge is included.

Approach. Part (a) superposes three Theis solutions — the initial rate starting at $t=0$, plus a rate CHANGE of $-3$ L/s starting at $t=12$ h, plus a further change of $-5$ L/s (shut-off) starting at $t=24$ h — each evaluated at its own elapsed time since it began. Part (b) applies the Dupuit-Forchheimer approximation for steady unconfined flow between two fixed heads with no recharge. Part (c) reuses part (b)'s two-well geometry with an added areal-recharge term in the Dupuit head-squared profile.

Check: part (c) as printed says "the aquifer in Question 4(a)," but asks for the head "halfway between the wells" — that phrase only has meaning for the two-well system of part (b) (part (a) has a single pumping well and one observation point, not two wells). This is treated as a reference slip for "Question 4(b)," and part (c) is solved as part (b)'s system with recharge added, consistent with the "answer what the data actually supports" convention for internally inconsistent exam wording.
  1. Part (a) — aquifer properties. $T=Kb=(1.3\times10^{-3}/100)(40)=\boxed{5.20\times10^{-4}\ \text{m}^2\text{/s}}$, $S=S_sb=(1.2\times10^{-5})(40)=\boxed{4.80\times10^{-4}}$.
  2. Step-rate + shutoff superposition. At $t=36\ \text{h}=129{,}600$ s and $r=100$ m, three Theis terms apply: $Q_1=8$ L/s since $t=0$ (elapsed 36 h), $\Delta Q_2=5-8=-3$ L/s since $t=12$ h (elapsed 24 h), $\Delta Q_3=0-5=-5$ L/s since $t=24$ h (elapsed 12 h): $$s=\frac{Q_1}{4\pi T}W(u_{36})+\frac{\Delta Q_2}{4\pi T}W(u_{24})+\frac{\Delta Q_3}{4\pi T}W(u_{12})=\boxed{0.996\ \text{m}}.$$
  3. Part (b)(i) — heads above the aquifer base. With the base as datum, $h_1=30-8=22$ m, $h_2=30-11=19$ m over $L=150$ m. Dupuit-Forchheimer unit-width flow: $$q=\frac{K(h_1^2-h_2^2)}{2L}=\frac{(3\times10^{-5})(22^2-19^2)}{2(150)}=1.23\times10^{-5}\ \text{m}^2\text{/s},$$ $$Q_{\text{tot}}=q\times(\text{width})=(1.23\times10^{-5})(2400)=\boxed{0.0295\ \text{m}^3\text{/s}\ (29.5\ \text{L/s})}.$$
  4. Part (b)(ii) — head at the midpoint. $$h^2(x)=h_1^2-\frac{h_1^2-h_2^2}{L}x\ \Rightarrow\ h(75)=\sqrt{22^2-\frac{22^2-19^2}{150}(75)}=\boxed{20.55\ \text{m above the base}}$$ (depth below ground $\approx30-20.55=9.45$ m).
  5. Part (b)(iii) — pore (linear) velocity at the midpoint. With no recharge, unit-width discharge $q$ is constant along $x$, so the local Darcy flux is $q/h(x)$: $$v_{\text{Darcy}}=\frac{q}{h(75)}=\frac{1.23\times10^{-5}}{20.55}=5.98\times10^{-7}\ \text{m/s},\qquad v_{\text{linear}}=\frac{v_{\text{Darcy}}}{n_e}=\frac{5.98\times10^{-7}}{0.33}=\boxed{1.81\times10^{-6}\ \text{m/s}}.$$
  6. Part (c) — head at the midpoint with areal recharge. Recharge $W=0.25\ \text{m/yr}=7.92\times10^{-9}\ \text{m/s}$; the Dupuit head-squared profile gains a mounding term: $$h^2(x)=h_1^2-\frac{h_1^2-h_2^2}{L}x+\frac{W}{K}x(L-x)\ \Rightarrow\ h(75)=\sqrt{422.5+\left(\frac{7.92\times10^{-9}}{3\times10^{-5}}\right)(75)(75)}=\boxed{20.59\ \text{m above the base}}$$ (depth below ground $\approx30-20.59=9.41$ m) — slightly higher than the no-recharge case, as the added infiltration mounds the water table.
QuantityResult
(a) $T$, $S$5.20×10⁻⁴ m²/s, 4.80×10⁻⁴
(a) Drawdown at $r$=100 m, $t$=36 h0.996 m
(b)(i) Total flow $Q_{\text{tot}}$0.0295 m³/s (29.5 L/s)
(b)(ii) Head at midpoint (no recharge)20.55 m above base (≈9.45 m depth)
(b)(iii) Pore (linear) velocity at midpoint1.81×10⁻⁶ m/s
(c) Head at midpoint (with recharge)20.59 m above base (≈9.41 m depth)