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Example 6.6

Estimation of the ultimate geotechnical strength of a pile subjected to axial compressive load based on CPT test results

Estimate the ultimate geotechnical strength Qf of the driven concrete pile shown below. The pile is subjected to axial compressive load and is embedded in a layered profile comprising both fine-grained and coarse-grained layers. Use CPT-based methods of Schmertmann (1978) and Bustamante and Gianeselli (1982) (Chapter 6.12) together with the CPT results provided below. Ignore the weight of the pile in the calculations.

The figure on the left shows the variation of dimensionless cone resistance qc/pa with depth, up to a depth 15m. The figure in the mid shows the variation of sleeve friction resistance with depth, up to a depth 15m. The figure on the right shows a concrete pile driven in layered soil, with the SBT of each soil layer determined from the CPT data. The length of the pile is 8 m and its diameter is 1 m. The pile is loaded with an axial compressive load Qf at its head.
Example 6.6. Problem description and input parameters.

Answer:

As discussed in Chapter 6.12, the correction factor α used in Schmertmann’s method in the determination of the skin friction resistance Qsf of the pile depends on the nature of the surrounding soil (coarse-grained or fine grained). Thus, before proceeding with the estimation of the skin friction resistance, the soil behavior types SBT encountered along the length of the pile must be determined, according to the mentioned in Chapter 1.7.

1. Calculation of skin friction resistance Qf using the method proposed by Schmertmann (1978):

1.1 Skin friction resistance along pile shaft embedded in sand (SBT 5/6):

For the part of the concrete pile that is embedded into sand, the variation of the correction factor α′ with depth z is determined with the aid of Eq. 6.24 (Figure 6.55):

\alpha ' = 1.85 - 0.1\left( {\dfrac{z}{D}} \right) + 0.0025{\left( {\dfrac{z}{D}} \right)^2} - 0.259 \times {10^{ - 4}}{\left( {\dfrac{z}{D}} \right)^3}

The sand layer is divided into sublayers, the thickness ΔL of which depends on the frequency of sleeve friction resistance fs measurements from the CPT test.

The unit friction resistance of each sublayer ΔQf is then estimated with Eq. 6.23 (Figure 6.55):

\Delta {Q_{sf}} = {f_{sf}}\left( {\pi D} \right)\Delta L = \left( {\alpha '{f_s}} \right)\left( {\pi D} \right)dL

and summed to find the skin friction resistance of the pile that develops along the part of the shaft embedded in the sand layer, Qsf,sand.

Alternatively, we can use the Bustamante and Gianeselli’s method to estimate Qsf,sand. In that case the skin friction resistance along each sublayer is calculated as fsf = qc/α where the coefficient α is provided by Table 6.6 for sand with qc > 12 MPa (generally qc/pa > 120 in the provided data indicating dense sand) and driven precast concrete piles (Category IIA) to be α = 150. The limiting value of fsf is from Table 6.6 fsf < 120 kPa. Using the provided qc values we calculate Qsf,sand = 823 kN. There is significant difference between the results of the two methods, and is attributed only partly to the Bustamante and Gianeselli’s method imposing a limiting value to fsf, as the fsf is exceeded in merely two sublayers.

1.2 Skin friction resistance along pile shaft embedded in clay (SBT3) and silt (SBT4):

A similar procedure is followed for the part of the pile embedded into the fine-grained clay/silt layers. In that case, the correction factor α′ depends on the sleeve friction resistance, and is provided from Eq. 6.26 for concrete piles (Figure 6.56):

\alpha ' = 1.28 - 1.473\left( {\dfrac{{{f_s}}}{{{p_a}}}} \right) + 0.839{\left( {\dfrac{{{f_s}}}{{{p_a}}}} \right)^2} - 0.1634{\left( {\dfrac{{{f_s}}}{{{p_a}}}} \right)^3}

The figure on the left shows the variation with depth of sleeve friction resistance along the part of the pile embedded in sand-type layers. The figure in the mid shows the variation with depth of the parameter α' corresponding to the sleeve friction resistance. The figure on the right presents the variation of the skin friction force ΔQsf developing along pile segments of 0.5 m. The sum of the skin friction force along all segments is Qsf,sand = 1988 kN.
Figure 6.55. Calculation of pile’s skin friction resistance along the sand layer (SBT5/6).
The figure on the left shows the variation with depth of sleeve friction resistance along the part of the pile embedded in clay-type layers. The figure in the mid shows the variation with depth of the parameter α' corresponding to the sleeve friction resistance. The figure on the right presents the variation of the skin friction force ΔQsf developing along pile segments of length ranging from 0.75 to 0.25m. The sum of the skin friction force along all segments is Qsf,clay = 699 kN.
Figure 6.56. Calculation of the pile’s skin friction resistance along the clay (SBT3) and silt (SBT4) layers.

Dividing again into sublayers we can estimate the unit skin friction resistance with Eq. 6.23, and the total friction resistance developing along the part of the pile embedded in fine-grained soil, Qsf,clay (Figure 6.56).

Again we will use the Bustamante and Gianeselli’s method to estimate Qsf,clay, for comparison purposes. Skin friction resistance along each sublayer is again calculated as fsf = qc/α where the coefficient α for clay with qc = 1 to 5 MPa (firm to stiff clay) and driven precast concrete piles (Category IIA) to be α = 40. The limiting value of fsf is from Table 6.6 fsf < 35 kPa. Using the provided qc values we calculate Qsf,clay = 499 kN. Again, there is a significant difference between the results of the two methods.

While this comparison is based on fictitious CPT data, therefore one may argue that the differences between the two methods may have been exaggerated (the total skin friction resistance estimated with Schmertmann’s method is Qsf = 2700 kN, and the total skin friction resistance estimated with Bustamante and Gianeselli’s method is Qsf = 1322 kN i.e., less than half) its purpose in not to endorse one method over the other. Instead, its purpose is to inform the reader about the uncertainties associated with estimating the ultimate geotechnical strength with empirical methods. This is the reason why careful selection of risk ratings AS2159 is required, particularly when using legacy methods to estimate the design bearing capacity of piles.

2. End-bearing resistance, Qb:

In order to apply the LCPC method and use Eq. 6.29 to estimation the end bearing resistance of the pile, we must first estimate the equivalent average cone resistance qc(eq), following the procedure described in Chapter 6.12:

  • Consider the cone tip resistance qc within a range of 1.5D = 1.5 m below the pile toe to 1.5D = 1.5 m above the pile toe (Figure 6.57b) and calculate the average value of qc(av) = 1648 kPa within this zone.
  • Eliminate qc values that are higher than 0.7qc(av) and lower than 1.3qc(av) (Figure 6.57c) and calculate qc(eq) = 1482 kPa by averaging the remaining qc values.
Figure (a) on the left presents the pile toe embedded in SBT 3 (clay soil). The diameter of the pile is 1m. Figure (b) in the mid presents the variation of cone resistance with depth along a length 1.5D above and 1.5D below the pile's toe. From these values it is calculated that qc(av)=1648 kPa. Figure (c) on the right presents the range of values 0.7qc(av) and 1.3qc(av). qc values that fall within that range are used to calculate qc(eq) = 1482 kPa.
Figure 6.57. (a) Detail of the pile toe area, (b) Calculation of qc(av), and (c) Calculation of qc(eq).

Furthermore, as the pile toe is embedded in clay, the empirical bearing capacity factor to be introduced in Eq. 6.29 is kb = 0.6 according to Briaud and Miran (1991). Substituting in Eq. 6.29 yields:

{Q_b} = {q_{c\left( {eq} \right)}}{k_c}{A_b} = 1482 \times 0.6 \times \pi \times \dfrac{{{D^2}}}{4} = 698{\rm{ \:kN}}

We can perform a sanity check here, if we consider that the undrained strength of clays is correlated to the cone resistance with Eq. 1.16 as:

{S_u} = \dfrac{{{q_t} - {\sigma _z}}}{{{N_{kt}}}} = \dfrac{{1482 - {\sigma _z}}}{{{N_{kt}}}}

If we take an average Nkt value Nkt = 15 and an estimate of the total vertical stress at -8 m i.e. σz = 16 x 8 = 128 kPa we calculate at the base of the pile Su,b = 90 kPa, which is reasonable for a stiff clay. Using Eq. 6.9 to calculate the end bearing resistance with the α-method we obtain:

{Q_b} = {N_{cp}}{S_{u,b}}{A_b} = 9 \times 90 \times \pi \times \dfrac{{{D^2}}}{4} = 636{\rm{ \:kN}}

Such “sanity checks” are particularly important, when empirical methods are employed for the design of piles.

3. Ultimate geotechnical strength, Qf:

The collapse load of the pile is the sum of its skin friction resistance along the clay/silt and the sand layers, and end-bearing resistance:

{Q_f} = {Q_b} + {Q_{sf,sand}} + {Q_{sf,clay}} = 698 + 1988 + 699 = 3385{\rm{ \:kN}} (using Schmertmann’s method to calculate Qsf)

{Q_f} = {Q_b} + {Q_{sf,sand}} + {Q_{sf,clay}} = 698 + 823 + 499 = 2020{\rm{ \:kN}} (using Bustamante and Gianeselli’s method to calculate Qsf)

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