Question 2 of 10: Shear-strength parameters for long-term slope stability in expansive soil
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. Professional Engineers Ontario /
Engineers Canada National Examinations, December 2014 — 98-Civ-B3 Geotechnical
Design. Three hours, OPEN BOOK, any non-communicating calculator. Section A carries five
discussion questions of 7 marks each (answer any four); Section B carries five design
questions of 24 marks each (answer any three); the examinable total is
4 × 7 + 3 × 24 = 100 marks. All ten questions are worked below, because the
set is a study resource rather than a timed attempt.
B. M. Das, Principles of Foundation Engineering, 9th ed. — bearing
capacity (Ch. 3), stress increase in a soil mass (Ch. 6), retaining walls (Ch. 8), pile
foundations (Ch. 11).
B. M. Das, Principles of Geotechnical Engineering, 9th ed. — lateral
earth pressure (Ch. 13), shear strength (Ch. 12), slope stability (Ch. 15), subsurface
exploration (Ch. 17).
Canadian Geotechnical Society, Canadian Foundation Engineering Manual
(CFEM), 4th ed. — the governing Canadian practice document for site investigation,
bearing resistance, deep foundations and earth-retaining structures.
R. F. Craig, Craig's Soil Mechanics, 8th ed. — earth pressure theory
and slope stability.
D. P. Coduto, Foundation Design: Principles and Practices, 2nd ed. —
in-situ testing and SPT correlations.
J. E. Bowles, Foundation Analysis and Design, 5th ed. — bearing
capacity factors and retaining-wall stability tables.
Sources of charts and assumed values (page-1 Note 6). Note 6 of this
paper requires the candidate to identify the source of every design chart and every
assumed value. Each chart reading and each assumption below is therefore named where it is
used, and the values assumed in the absence of data are collected here:
Q6 — adhesion factor α from Das,
Principles of Foundation Engineering, Table 11.6 (Terzaghi, Peck & Mesri
form, α against $c_u/p_a$); $\lambda$ from Vijayvergiya & Focht
(1972) as tabulated by Das, Table 11.7.
Q7 — overburden correction $C_N$ from Liao & Whitman
(1986); $\phi'$ from Wolff (1989) and from Hatanaka & Uchida (1996), both reproduced
in Das, Ch. 2; settlement-controlled bearing pressure from Meyerhof (1965) as given by
Das, Ch. 5, used only as a serviceability check because the question forbids direct
correlations of bearing capacity to penetration index. Table I prints the blow counts as
field values $N_f$; with no hammer data they are converted as $N_{60} = N_f$, i.e. a
safety hammer at the reference 60 per cent energy ratio with borehole, sampler and
rod-length factors of 1 (Das, Ch. 2, hammer-efficiency and correction-factor tables).
Q8 — embankment influence factor from Osterberg (1957),
reproduced as Das Fig. 6.24; the closed form of that chart is used so the reading carries
no chart-scaling error.
Q9 — Meyerhof general bearing-capacity equation with the shape
factors of De Beer (1970) and the depth factors of Hansen (1970), as set out in Das,
Ch. 3.
Q10 — Coulomb active earth-pressure coefficient, Das
Eq. 13.31; unit weight of the mass-concrete wall assumed
$\gamma_c = 24\ \text{kN/m}^3$ (CFEM 4th ed., normal-density concrete), the only value
the figure does not supply.
Question 2: Shear-strength parameters for long-term slope stability in expansive soil
(7 marks)
Long-term stability is by definition a drained condition, so the analysis must be
carried out in effective stresses using the drained parameters
$c'$ and $\phi'$, with the pore pressures taken from the steady-state seepage
condition rather than from the end of construction. That much is common to every clay
slope. What is specific to an expansive clay is which drained
parameters, because the peak drained envelope measured on an intact specimen is not the
strength that will be available on a slip surface decades later.
The parameters recommended are therefore:
Where no pre-existing shear surface exists: the
fully softened strength, that is $c' = 0$ with the fully softened
friction angle $\phi'_{fs}$, measured on a normally consolidated, remoulded specimen
in a drained direct shear or consolidated-undrained triaxial test with pore-pressure
measurement.
Where a pre-existing slip surface, bedding-plane shear or old landslide is
present: the residual strength, $c'_r = 0$ and
$\phi'_r$, measured in a ring-shear apparatus (Bromhead) or by reversal direct
shear.
Three mechanisms make the peak parameters unsafe in this soil. First, an expansive
clay is a high-plasticity clay whose volume changes with water content. Seasonal wetting
and drying opens a network of fissures to depths of several metres; each fissure is a
plane of near-zero cohesion, and the mass strength collapses towards the strength of the
fissure walls. Any $c'$ intercept measured on an intact 38 mm triaxial specimen simply
does not exist at the scale of a slope.
Second, swelling on wetting destroys the suction and the diagenetic bonding that
produced the cohesion intercept in the first place. Skempton's classic observation on
Brown London Clay is that a cut slope in a stiff fissured clay stands for years and then
fails at a mobilised strength corresponding to $c' = 0$ — the fully softened
condition — because water has slowly entered the fissures and swelled the clay to a
normally consolidated state. The delay between excavation and failure is exactly the delay
required for negative excess pore pressures to dissipate and for softening to progress.
Third, stiff clays are strain-softening: peak strength occurs at a small strain and
falls away as displacement continues. Along a curved slip surface the local displacement
is not uniform, so the peak cannot be mobilised everywhere at once. Progressive failure
propagates from the toe, and the average strength available at collapse lies between peak
and residual. Where movement has already occurred — a reactivated slide, a
bedding-plane shear, a slope showing tension cracks — the clay platelets on the shear
plane are fully aligned and the residual value, which for a high-plasticity clay can be as
low as 8° to 12°, is the only defensible choice.
Two practical points complete the answer. The pore pressures must correspond to the
long-term steady seepage regime, taken from piezometers and a flow net, and should include
the worst credible condition (a wet-season perched water table, a blocked drain). And in
an expansive clay the seasonal swelling pressure itself imposes a horizontal stress that
can approach the passive value in the active zone; where a structure is founded within
that zone this must be carried as a load, not ignored.