18-Env-A3 Geotechnical and Hydrogeological Engineering · December 2017
Question 6 of 6: Falling-Head Permeability Test
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Exams — December 2017 — 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, compaction, seepage/flow nets, and consolidation chapters; Craig & Knappett, Craig's Soil Mechanics (8th ed.) — cross-reference for flow-net theory and finite-difference seepage; Freeze & Cherry, Groundwater (1979) — Darcy's law, the Thiem confined-flow equation, and radial travel time.
Question 6: Falling-Head Permeability Test (20 marks)
500 mm above counter ($\Delta h_0=400\ \text{mm}$)
Standpipe elevation at $t=24\ \text{h}$
—
250 mm above counter ($\Delta h_1=150\ \text{mm}$)
Find. (a) hydraulic conductivity, with a comment on reasonableness; (b) standpipe elevation at $t=4$ h and $t=12$ h.
Approach. Apply the falling-head formula to the head loss measured ABOVE the constant bath level, then use the same exponential head-decay relation to evaluate the head (and hence elevation) at the two intermediate times.
Fig. Q6 — falling-head apparatus; heads $\Delta h_0$, $\Delta h(t)$, $\Delta h_1$ are measured above the constant bath level.
Areas and head loss. $a=\dfrac{\pi}{4}(0.5\ \text{cm})^2=0.1963\ \text{cm}^2$ (standpipe); $A=\dfrac{\pi}{4}(10\ \text{cm})^2=78.54\ \text{cm}^2$ (specimen); heads measured ABOVE the bath: $h_1=50-10=40\ \text{cm}$ at $t=0$, $h_2=25-10=15\ \text{cm}$ at $t=24\ \text{h}=86{,}400\ \text{s}$.
Part (a) — hydraulic conductivity.
$$k=\frac{aL}{At}\ln\Big(\frac{h_1}{h_2}\Big)=\frac{0.1963\times2.0}{78.54\times86{,}400}\ln\Big(\frac{40}{15}\Big)=\boxed{5.68\times10^{-8}\ \text{cm/s}}.$$
This falls squarely in the typical clay range ($10^{-6}$ to $10^{-9}$ cm/s), so the value IS reasonable for a clay specimen.
Part (b) — head at intermediate times. The falling-head solution is an exponential decay of the head above the bath, $h(t)=h_1\exp\!\big[-\tfrac{kA}{aL}t\big]$; evaluating at $t=4$ and $12$ h (and confirming it reproduces $h_2=15\ \text{cm}$ at 24 h):
$$\begin{aligned} h(4\ \text{h})&=34.0\ \text{cm}\ \Rightarrow\ \boxed{439.7\ \text{mm above the counter}} \\ h(12\ \text{h})&=24.5\ \text{cm}\ \Rightarrow\ \boxed{344.9\ \text{mm above the counter}} \end{aligned}$$
Check: elevations are the head above the bath PLUS the constant 100 mm bath level (e.g. $340\ \text{mm}+100\ \text{mm}=439.7$ mm reported to one decimal); the $t=24$ h check reproduces the given 250 mm exactly, confirming the fitted $k$.