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16-Civ-B3 Geotechnical Design · December 2016

Question 9 of 9: Overturning and sliding stability of a cantilever retaining wall

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 2016 — 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 four design questions of 24 marks each (answer any three); the examinable total is 4 × 7 + 3 × 24 = 100 marks. All nine questions are worked below, because the set is a study resource rather than a timed attempt.

Reference texts (98-Civ-B3 / 16-Civ-B3 Geotechnical Design).

Sources of design charts and assumed values (page-1 Note 6). Note 6 requires the candidate to identify the source of every design chart and of every value assumed where the paper supplies none. They are named at the point of use and collected here:

  • Adhesion factor α = 0.55 for a drilled shaft in clay (Q6) — O'Neill and Reese (1999), reproduced in Das, Principles of Foundation Engineering, 9th ed., Section 12.9; the exclusion of the top 1.5 m and of one shaft diameter above the bell comes from the same source.
  • Bearing-capacity factor Nc* = 9 (Q6) — Skempton (1951), as tabulated in Das, Section 11.11.
  • Overburden correction CN = √(pa/σ'o) (Q7) — Liao and Whitman (1986), Das Principles of Geotechnical Engineering, Section 17.6.
  • SPT-to-friction-angle correlation (Q7) — Peck, Hanson and Thornburn (1974) as fitted by Wolff (1989); cross-checked against Kulhawy and Mayne (1990). Both are tabulated in Das, Principles of Foundation Engineering, 9th ed., Section 2.9.
  • Bearing-capacity factors and shape/depth factors (Q7) — Vesic (1973) and De Beer (1970), Das Sections 3.6 and 3.7.
  • Strain-influence diagram and the C1, C2 factors (Q7) — Schmertmann, Hartman and Brown (1978), Das Section 5.6; the modulus correlation Es = 500(N60 + 15) kPa is Bowles (1996), reproduced in the same section.
  • Rankine active coefficient for an inclined backfill (Q9) — Das, Principles of Geotechnical Engineering, 9th ed., Eq. (13.35); the base friction and adhesion reductions k1 = k2 = 2/3 are Das Section 8.4.
  • Unit weight of the submerged backfill (Q9) — assumed equal to the printed moist unit weight, 18 kN/m3, in the absence of a saturated value; the consequence of that assumption is bounded in the Q9 callout.

Section A

Question 9: Overturning and sliding stability of a cantilever retaining wall (24 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.

QuantitySymbolValue
Base width / thicknessB / t4.8 m / 0.9 m
Toe / stem at base / heel—0.76 m / 1.04 m / 3.0 m
Stem height / top thickness—6.1 m / 0.4 m
Overall height, base underside to top of stemH7.0 m
Backfill slope / surchargeα / q8° / 20 kPa
Backfill sandγ, φ', c'18 kN/m3, 30°, 0
Water table above top of base—2.2 m (3.1 m above base underside)
Concreteγc23.5 kN/m3
Founding soilγ2, φ'2, c'2 19 kN/m3, 15°, 15 kPa
Depth of ground in front of the toeD1.0 m

Find. The factor of safety against overturning about the toe and the factor of safety against sliding along the base.

[Figure not reproduced: Figure 9.1 — The wall of Figure 3, redrawn to scale. The red dashed line at the back of the heel is the Rankine virtual back plane on which the active thrust is computed; the free body taken for stability is everything to the left of it, including the wedge of backfill standing on the heel. See the official exam paper.]

Approach. Use the Rankine method on a virtual vertical plane rising from the back of the heel. The free body is the concrete plus all the soil and surcharge standing on the heel; the earth thrust acts on that vertical plane, parallel to the sloping ground surface. Water enters three times — through the submerged unit weight below the water table, through a hydrostatic thrust on the plane, and through uplift on the base — and all three must be carried consistently. Moments are taken about the front bottom edge of the base (the toe).

  1. Establish the height of the virtual back plane. The ground surface starts at the top of the stem, 7.0 m above the base underside, and rises at 8° across the 3.0 m heel, so at the back of the heel $$H' = 7.0 + 3.0\tan 8^\circ = 7.0 + 0.4216 = 7.4216\ \text{m}$$
  2. Compute the Rankine active coefficient for the sloping backfill. With α = 8° and φ' = 30°, $$K_a = \cos\alpha\, \frac{\cos\alpha - \sqrt{\cos^2\alpha - \cos^2\phi'}} {\cos\alpha + \sqrt{\cos^2\alpha - \cos^2\phi'}} = 0.99027\,\frac{0.99027 - 0.48024}{0.99027 + 0.48024} = 0.3435$$ The resultant thrust on the vertical plane acts parallel to the ground surface, that is inclined at 8° to the horizontal.
  3. Build the effective lateral pressure diagram. The water table lies 3.1 m above the base underside, so it is 7.4216 − 3.1 = 4.3216 m below the surface. Above it the sand has γ = 18 kN/m3; below it the submerged value γ' = 18 − 9.81 = 8.19 kN/m3 applies. Effective vertical stresses on the plane are therefore $$\sigma'_v(0) = q = 20\ \text{kPa},\quad \sigma'_v(\text{WT}) = 20 + 18(4.3216) = 97.79\ \text{kPa},$$ $$\sigma'_v(\text{base}) = 97.79 + 8.19(3.1) = 123.18\ \text{kPa}$$ and multiplying by Ka gives lateral pressures of 6.87, 33.59 and 42.31 kPa at those three levels.
  4. Integrate the earth thrust and locate it. Splitting the diagram into the rectangle and triangle above the water table and the rectangle and triangle below it, $$P_1 = 6.87(4.3216) = 29.69,\quad P_2 = \tfrac12(33.59-6.87)(4.3216) = 57.73,$$ $$P_3 = 33.59(3.1) = 104.12,\quad P_4 = \tfrac12(42.31-33.59)(3.1) = 13.52\ \text{kN/m}$$ $$P_a = 205.05\ \text{kN/m}\quad\text{acting at}\quad \bar{y} = 2.895\ \text{m above the base underside}$$ Resolving at 8° to the horizontal, $$P_{ah} = 205.05\cos 8^\circ = 203.06\ \text{kN/m},\qquad P_{av} = 205.05\sin 8^\circ = 28.54\ \text{kN/m}$$ The vertical component acts downwards on the virtual plane at the back of the heel, so it is a stabilising force with the largest lever arm of all.
  5. Add the water thrust. The pore pressure on the virtual plane is hydrostatic below the water table, reaching u = 9.81(3.1) = 30.41 kPa at the base underside, so $$P_w = \tfrac12 \gamma_w h_w^2 = \tfrac12 (9.81)(3.1)^2 = 47.14\ \text{kN/m} \quad\text{at } 1.033\ \text{m above the base}$$ This acts horizontally and is purely destabilising. Its presence is the single most important feature of this wall.
    virtual back planeu = 30.41 kPawater tableKa q = 6.87 kPa33.59 kPa42.31 kPaKa = 0.3435H' = 7.422 m
    Figure 9.2 — Lateral pressure on the virtual back plane. Blue to the right of the plane: effective active earth pressure, kinked where the submerged unit weight takes over. Shaded to the left: the hydrostatic water pressure, which adds 47.1 kN/m of horizontal thrust that the drained wall would not carry.
  6. Assemble the vertical forces and their moments about the toe. Total (saturated) unit weights are used for the soil, so uplift must be added explicitly later. This step and the next two constitute the overturning check.
    ComponentForce (kN/m)Arm from toe (m)Moment (kN·m/m)
    Base slab, 4.8 × 0.9 × 23.5101.522.400243.65
    Stem (trapezoid 0.4/1.04 × 6.1) × 23.5103.211.416146.18
    Backfill on heel, below the water table118.803.300392.04
    Backfill on heel, above the water table210.603.300694.98
    Sloping wedge above the level of the stem top11.383.80043.26
    Surcharge over the heel, 20 × 3.060.003.300198.00
    Vertical component of the active thrust28.544.800136.99
    Totals634.05— 1855.1
    The soil standing on the toe (about 1.4 kN/m) is neglected, which is conservative for overturning.
  7. Compute the overturning moment and the uplift. The two horizontal thrusts give $$M_O = P_{ah}\bar{y} + P_w(1.033) = 203.06(2.895) + 47.14(1.033) = 587.9 + 48.7 = 636.6\ \text{kN}\cdot\text{m/m}$$ Because the backfill is ponded to 3.1 m and the ground in front is only 1.0 m deep and dry, water seeps beneath the base. Taking the standard linear approximation — full pressure 30.41 kPa at the heel falling to zero at the toe — $$U = \tfrac12 (30.41)(4.8) = 72.99\ \text{kN/m}\ \text{acting at }\tfrac23(4.8) = 3.20\ \text{m from the toe}$$ $$M_U = 72.99 \times 3.20 = 233.6\ \text{kN}\cdot\text{m/m}$$ which is a destabilising moment because it lifts the heel end of the base.
  8. Factor of safety against overturning. $$FS_{OT} = \frac{M_R}{M_O + M_U} = \frac{1855.1}{636.6 + 233.6} = \frac{1855.1}{870.2}$$ $$\boxed{FS_{OT} = 2.13}$$ If the base is assumed to be pressure-relieved so that no uplift acts, the same numbers give FSOT = 1855.1 / 636.6 = 2.91. Either way the wall is adequate against overturning, comfortably above the usual requirement of 1.5 to 2.0.
  9. Assemble the sliding resistance. The sliding check starts here. The net vertical force on the base is reduced by the uplift: $$\sum V_{\text{net}} = 634.05 - 72.99 = 561.07\ \text{kN/m}$$ Following Das Section 8.4, the base friction and adhesion are taken as fractions of the founding soil's strength, $k_1 = k_2 = \tfrac23$, giving $\delta' = \tfrac23(15^\circ) = 10^\circ$ and $c_a = \tfrac23(15) = 10$ kPa: $$F_R = \sum V_{\text{net}}\tan\delta' + B c_a = 561.07(0.17633) + 4.8(10) = 98.9 + 48.0 = 146.9\ \text{kN/m}$$
  10. Evaluate the passive resistance in front of the toe. Over the 1.0 m of founding soil standing in front of the wall, with $K_p = \tan^2(45^\circ + 15^\circ/2) = 1.698$, $$P_p = \tfrac12 K_p \gamma_2 D^2 + 2c'_2\sqrt{K_p}\,D = \tfrac12(1.698)(19)(1.0)^2 + 2(15)(1.303)(1.0) = 16.1 + 39.1 = 55.2\ \text{kN/m}$$ It is standard practice to neglect this term, because the 1.0 m of soil in front of a wall is the material most likely to be removed by a service trench, by scour or by future regrading, and because mobilising it needs far more movement than the active side does (Question 3).
  11. Factor of safety against sliding. The driving force is the sum of the two horizontal thrusts, $P_{ah} + P_w = 203.06 + 47.14 = 250.20$ kN/m, so $$FS_{SL} = \frac{F_R}{P_{ah}+P_w} = \frac{146.9}{250.2}$$ $$\boxed{FS_{SL} = 0.59\quad(\text{0.81 if the passive wedge is counted})}$$ Even with no uplift and the undiscounted base strength (k = 1), with the passive wedge still neglected, the ratio only reaches 0.97; adding the full passive wedge as well takes it to 1.19, still well short of 1.5. The wall as drawn does not satisfy sliding; it is at or beyond the point of failure.
  12. Check the base pressure, and state the remedy. The line of action of the net vertical force is at $\bar{x} = (1855.1 - 636.6 - 233.6)/561.07 = 1.755$ m from the toe, so the eccentricity is $e = 4.8/2 - 1.755 = 0.645$ m, less than B/6 = 0.8 m; the base stays in compression, with $q_{\max} = 211$ kPa and $q_{\min} = 22.7$ kPa. Bearing is therefore not the problem — sliding is, and the diagnosis is unambiguous. Draining the backfill removes both the water thrust and the uplift and lifts the sliding ratio only to 0.73, so drainage alone is not enough; the founding soil, at φ' = 15°, is simply too weak in friction. The effective remedy is a shear key beneath the base, which forces the failure surface into undisturbed soil so that the full φ'2 and c'2 may be used, and mobilises passive resistance over the full key depth. Reaching FSSL = 1.5 requires 375 kN/m of resistance against the 222 kN/m available on the full-strength base, so the key must generate a further 153 kN/m, which corresponds to a key extending to about 2.1 m below the front ground surface, that is roughly 1.1 m below the underside of the base. A weep-holed granular drainage blanket behind the stem should be provided in any case.
QuantityValue
Height of the virtual back plane, H'7.4216 m
Rankine active coefficient (α = 8°, φ' = 30°)Ka = 0.3435
Active thrust Pa (at 2.895 m, inclined 8°)205.05 kN/m
Horizontal / vertical components203.06 / 28.54 kN/m
Hydrostatic thrust Pw47.14 kN/m at 1.033 m
Total vertical force before uplift, ΣV634.05 kN/m
Resisting moment about the toe, MR1855.1 kN·m/m
Overturning moment (thrusts / uplift)636.6 / 233.6 kN·m/m
Factor of safety, overturning (with uplift)2.13
Factor of safety, overturning (no uplift)2.91
Base sliding resistance FR146.9 kN/m
Passive resistance available at the toe, Pp55.2 kN/m (neglected)
Factor of safety, sliding (uplift, Pp neglected) 0.59 — UNSAFE
Factor of safety, sliding (Pp included)0.81
Eccentricity / maximum base pressure0.645 m (< B/6) / 211 kPa
Shear key required for FSSL = 1.5about 1.1 m below the base

Check: the three modelling choices that move these numbers, and by how much.

  • Uplift beneath the base. Figure 3 shows ponded water 3.1 m up the back of the wall and dry ground 1.0 m deep in front, so seepage beneath the base is real and a linear uplift from 30.41 kPa at the heel to zero at the toe is the standard simple treatment. Omitting it entirely gives FSOT = 2.91 and FSSL = 0.64. The conclusion is unchanged either way: safe in overturning, unsafe in sliding. Both are reported so the reader can see the span.
  • Unit weight of the submerged backfill. The figure prints one value, γ = 18 kN/m3, and it has been used both above and below the water table. If instead the sand were taken as dry at 18 and saturated at about 21.0 kN/m3 (the value implied by Gs = 2.65 with that dry weight), γ' would rise from 8.19 to 11.2 kN/m3: the thrust would grow by about 5 kN/m and the resisting weight of the heel backfill by about 20 kN/m, moving FSSL from 0.587 to 0.591. The assumption is immaterial.
  • Reading of the toe dimension. Figure 3 is not drawn to scale. Its drawn proportions give a toe of about 0.76 m and a stem 1.04 m thick at its base (the reading used above, with toe + stem = 1.8 m), but the arrowed dimension carrying the “1.04 m” label spans the toe projection, which read literally gives a 1.04 m toe and a 0.76 m stem. On that reading the stem weighs 83.1 kN/m instead of 103.2, and FSOT = 2.11 (2.88 without uplift) and FSSL = 0.57 (0.79 with the passive wedge). The conclusion is unchanged: adequate in overturning, failing in sliding.
  • Rankine on the virtual plane versus Coulomb on the stem face. The virtual vertical plane through the heel is the correct free body for a cantilever wall with a projecting heel, and it is the treatment used here. A Coulomb analysis applied to the battered back face of the stem would not be self-consistent with counting the whole soil column over the heel as resisting weight, because that soil lies on the far side of the pressure plane.
  • Full-strength base for the shear-key sizing. Sizing the key uses φ'2 = 15° and c'2 = 15 kPa undiscounted, which is the point of a key: the failure surface no longer lies at a concrete-to-soil interface. If the two-thirds reduction were retained the required key would be substantially deeper.
  • What was not checked. The question asks only for overturning and sliding. Bearing capacity of the founding soil, overall (deep-seated) slope stability through the weak φ' = 15° stratum, and structural design of the stem and base are all outside the scope but would all be required before construction. Given the sliding result, a deep-seated stability check would be the next thing this designer would run.
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