{"id":525,"date":"2025-03-31T04:10:00","date_gmt":"2025-03-31T04:10:00","guid":{"rendered":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/example-6-6-estimation-of-the-ultimate-geotechnical-strength-of-a-pile-subjected-to-axial-compressive-load-based-on-cpt-test-results\/"},"modified":"2026-03-16T14:11:15","modified_gmt":"2026-03-16T14:11:15","slug":"example-6-6-estimation-of-the-ultimate-geotechnical-strength-of-a-pile-subjected-to-axial-compressive-load-based-on-cpt-test-results","status":"publish","type":"chapter","link":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/example-6-6-estimation-of-the-ultimate-geotechnical-strength-of-a-pile-subjected-to-axial-compressive-load-based-on-cpt-test-results\/","title":{"raw":"Example 6.6","rendered":"Example 6.6"},"content":{"raw":"Estimate the ultimate geotechnical strength <em>Q<sub>f<\/sub><\/em> 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) (<a href=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/6-12-ultimate-geotechnical-strength-of-piles-subjected-to-axial-compressive-load-from-cpt-test-results\/\">Chapter 6.12<\/a>) together with the CPT results provided below. Ignore the weight of the pile in the calculations.\n\n[caption id=\"attachment_524\" align=\"aligncenter\" width=\"900\"]<img class=\"wp-image-521 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2025\/03\/example-6.6brief-hr-e1743553620893.png\" alt=\"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. \" width=\"900\" height=\"659\"> Example 6.6. Problem description and input parameters.[\/caption]\n<h2>Answer:<\/h2>\nAs discussed in <a href=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/6-12-ultimate-geotechnical-strength-of-piles-subjected-to-axial-compressive-load-from-cpt-test-results\/\">Chapter 6.12<\/a>, the correction factor <em>\u03b1<\/em><em>\u2032<\/em> used in Schmertmann\u2019s method in the determination of the skin friction resistance <em>Q<sub>sf<\/sub><\/em> 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 <a href=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/1-7-the-cone-penetration-test-cpt\/\">Chapter 1.7<\/a>.\n\n1. Calculation of skin friction resistance <em>Q<sub>f<\/sub><\/em> using the method proposed by Schmertmann (1978):\n<p style=\"padding-left: 40px\">1.1\u00a0Skin friction resistance along pile shaft embedded in sand (SBT 5\/6):<\/p>\nFor the part of the concrete pile that is embedded into sand, the variation of the correction factor <em>\u03b1\u2032<\/em><em>\u00a0<\/em>with depth <em>z<\/em> is determined with the aid of Eq. 6.24 (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/03\/6.55-hr.png\">Figure 6.55<\/a>):\n\n[latex]\\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}[\/latex]\n\nThe sand layer is divided into sublayers, the thickness \u0394<em>L<\/em> of which depends on the frequency of sleeve friction resistance <em>f<sub>s<\/sub><\/em> measurements from the CPT test.\n\nThe unit friction resistance of each sublayer \u0394<em>Q<sub>f <\/sub><\/em>is then estimated with Eq. 6.23 (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/03\/6.55-hr.png\">Figure 6.55<\/a>):\n\n[latex]\\Delta {Q_{sf}} = {f_{sf}}\\left( {\\pi D} \\right)\\Delta L = \\left( {\\alpha '{f_s}} \\right)\\left( {\\pi D} \\right)dL[\/latex]\n\nand summed to find the skin friction resistance of the pile that develops along the part of the shaft embedded in the sand layer, <em>Q<sub>sf,sand<\/sub><\/em>.\n\nAlternatively, we can use the Bustamante and Gianeselli\u2019s method to estimate <em>Q<sub>sf,sand<\/sub><\/em>. In that case the skin friction resistance along each sublayer is calculated as <em>f<sub>sf<\/sub><\/em> = <em>q<sub>c<\/sub><\/em>\/<em>\u03b1<\/em> where the coefficient <em>\u03b1<\/em> is provided by Table 6.6 for sand with <em>q<sub>c<\/sub><\/em> &gt; 12 MPa (generally <em>q<sub>c<\/sub><\/em>\/<em>p<sub>a<\/sub><\/em> &gt; 120 in the provided data indicating dense sand) and driven precast concrete piles (Category IIA) to be <em>\u03b1<\/em> = 150. The limiting value of <em>f<sub>sf<\/sub><\/em> is from Table 6.6 <em>f<sub>sf<\/sub><\/em> &lt; 120 kPa. Using the provided <em>q<sub>c<\/sub><\/em> values we calculate <em>Q<sub>sf,sand<\/sub><\/em> = 823 kN. There is significant difference between the results of the two methods, and is attributed only partly to the Bustamante and Gianeselli\u2019s method imposing a limiting value to <em>f<sub>sf<\/sub><\/em>, as the <em>f<sub>sf<\/sub><\/em> is exceeded in merely two sublayers.\n<p style=\"padding-left: 40px\">1.2 Skin friction resistance along pile shaft embedded in clay (SBT3) and silt (SBT4):<\/p>\nA similar procedure is followed for the part of the pile embedded into the fine-grained clay\/silt layers. In that case, the correction factor <em>\u03b1\u2032<\/em><em>\u00a0<\/em>depends on the sleeve friction resistance, and is provided from Eq. 6.26 for concrete piles (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/03\/6.56-hr.png\">Figure 6.56<\/a>):\n\n[latex]\\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}[\/latex]\n\n[caption id=\"attachment_524\" align=\"aligncenter\" width=\"900\"]<img class=\"wp-image-522 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/6.55-hr-e1743553637824.png\" alt=\"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 \u03b1' corresponding to the sleeve friction resistance. The figure on the right presents the variation of the skin friction force \u0394Qsf developing along pile segments of 0.5 m. The sum of the skin friction force along all segments is Qsf,sand = 1988 kN.\" width=\"900\" height=\"732\"> Figure 6.55. Calculation of pile\u2019s skin friction resistance along the sand layer (SBT5\/6).[\/caption]\n\n[caption id=\"attachment_524\" align=\"aligncenter\" width=\"900\"]<img class=\"wp-image-523 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/6.56-hr-e1743553657602.png\" alt=\"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 \u03b1' corresponding to the sleeve friction resistance. The figure on the right presents the variation of the skin friction force \u0394Qsf 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.\" width=\"900\" height=\"750\"> Figure 6.56. Calculation of the pile\u2019s skin friction resistance along the clay (SBT3) and silt (SBT4) layers.[\/caption]\n\nDividing 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, <em>Q<sub>sf,clay<\/sub><\/em> (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/03\/6.56-hr.png\">Figure 6.56<\/a>).\n\nAgain we will use the Bustamante and Gianeselli\u2019s method to estimate <em>Q<sub>sf,clay<\/sub><\/em>, for comparison purposes. Skin friction resistance along each sublayer is again calculated as <em>f<sub>sf<\/sub><\/em> = <em>q<sub>c<\/sub><\/em>\/<em>\u03b1<\/em> where the coefficient <em>\u03b1<\/em> for clay with <em>q<sub>c<\/sub><\/em> = 1 to 5 MPa (firm to stiff clay) and driven precast concrete piles (Category IIA) to be <em>\u03b1<\/em> = 40. The limiting value of <em>f<sub>sf<\/sub><\/em> is from Table 6.6 <em>f<sub>sf<\/sub><\/em> &lt; 35 kPa. Using the provided <em>q<sub>c<\/sub><\/em> values we calculate <em>Q<sub>sf,clay<\/sub><\/em> = 499 kN. Again, there is a significant difference between the results of the two methods.\n\nWhile 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\u2019s method is <em>Q<sub>sf<\/sub><\/em> = 2700 kN, and the total skin friction resistance estimated with Bustamante and Gianeselli\u2019s method is <em>Q<sub>sf<\/sub><\/em> = 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.\n\n2. End-bearing resistance, <em>Q<sub>b<\/sub><\/em>:\n\nIn 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 <em>q<sub>c(eq)<\/sub><\/em>, following the procedure described in <a href=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/6-12-ultimate-geotechnical-strength-of-piles-subjected-to-axial-compressive-load-from-cpt-test-results\/\">Chapter 6.12<\/a>:\n<ul>\n \t<li>Consider the cone tip resistance <em>q<sub>c<\/sub><\/em> within a range of 1.5<em>D <\/em>= 1.5 m below the pile toe to 1.5<em>D <\/em>= 1.5 m above the pile toe (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/03\/6.57-detail-and-calculations.png\">Figure 6.57b<\/a>) and calculate the average value of <em>q<sub>c(av) <\/sub><\/em>= 1648 kPa within this zone.<\/li>\n \t<li>Eliminate <em>q<sub>c <\/sub><\/em>values that are higher than 0.7<em>q<sub>c(av) <\/sub><\/em>and lower than 1.3<em>q<sub>c(av)<\/sub><\/em> (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/03\/6.57-detail-and-calculations.png\">Figure 6.57c<\/a>) and calculate <em>q<sub>c(eq) <\/sub><\/em>= 1482 kPa by averaging the remaining <em>q<sub>c<\/sub><\/em> values.<\/li>\n<\/ul>\n[caption id=\"attachment_524\" align=\"aligncenter\" width=\"913\"]<img class=\"wp-image-524 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/6.57-detail-and-calculations.png\" alt=\"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. \" width=\"913\" height=\"271\"> Figure 6.57. (a) Detail of the pile toe area, (b) Calculation of <em>q<\/em><sub>c(av)<\/sub>, and (c) Calculation of <em>q<\/em><sub>c(eq)<\/sub>.[\/caption]\n\nFurthermore, as the pile toe is embedded in clay, the empirical bearing capacity factor to be introduced in Eq. 6.29 is <em>k<sub>b <\/sub><\/em>= 0.6 according to Briaud and Miran (1991). Substituting in Eq. 6.29 yields:\n\n[latex]{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}}[\/latex]\n\nWe 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:\n\n[latex]{S_u} = \\dfrac{{{q_t} - {\\sigma _z}}}{{{N_{kt}}}} = \\dfrac{{1482 - {\\sigma _z}}}{{{N_{kt}}}}[\/latex]\n\nIf we take an average <em>N<sub>kt<\/sub><\/em> value <em>N<sub>kt<\/sub><\/em> = 15 and an estimate of the total vertical stress at -8 m i.e. <em>\u03c3<\/em><sub>z<\/sub> = 16 x 8 = 128 kPa we calculate at the base of the pile <em>S<sub>u,b<\/sub><\/em> = 90 kPa, which is reasonable for a stiff clay. Using Eq. 6.9 to calculate the end bearing resistance with the <em>\u03b1<\/em>-method we obtain:\n\n[latex]{Q_b} = {N_{cp}}{S_{u,b}}{A_b} = 9 \\times 90 \\times \\pi \\times \\dfrac{{{D^2}}}{4} = 636{\\rm{ \\:kN}}[\/latex]\n\nSuch \u201csanity checks\u201d are particularly important, when empirical methods are employed for the design of piles.\n\n3. Ultimate geotechnical strength, <em>Q<sub>f<\/sub><\/em>:\n\nThe 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:\n\n[latex]{Q_f} = {Q_b} + {Q_{sf,sand}} + {Q_{sf,clay}} = 698 + 1988 + 699 = 3385{\\rm{ \\:kN}}[\/latex]\u00a0(using Schmertmann\u2019s method to calculate <em>Q<sub>sf<\/sub><\/em>)\n\n[latex]{Q_f} = {Q_b} + {Q_{sf,sand}} + {Q_{sf,clay}} = 698 + 823 + 499 = 2020{\\rm{ \\:kN}}[\/latex]\u00a0(using Bustamante and Gianeselli\u2019s method to calculate <em>Q<sub>sf<\/sub><\/em>)","rendered":"<p>Estimate the ultimate geotechnical strength <em>Q<sub>f<\/sub><\/em> 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) (<a href=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/6-12-ultimate-geotechnical-strength-of-piles-subjected-to-axial-compressive-load-from-cpt-test-results\/\">Chapter 6.12<\/a>) together with the CPT results provided below. Ignore the weight of the pile in the calculations.<\/p>\n<figure id=\"attachment_524\" aria-describedby=\"caption-attachment-524\" style=\"width: 900px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" class=\"wp-image-521 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2025\/03\/example-6.6brief-hr-e1743553620893.png\" alt=\"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.\" width=\"900\" height=\"659\" srcset=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/03\/example-6.6brief-hr-e1743553620893.png 900w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/03\/example-6.6brief-hr-e1743553620893-300x220.png 300w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/03\/example-6.6brief-hr-e1743553620893-768x562.png 768w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/03\/example-6.6brief-hr-e1743553620893-65x48.png 65w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/03\/example-6.6brief-hr-e1743553620893-225x165.png 225w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/03\/example-6.6brief-hr-e1743553620893-350x256.png 350w\" sizes=\"(max-width: 900px) 100vw, 900px\" \/><figcaption id=\"caption-attachment-524\" class=\"wp-caption-text\">Example 6.6. Problem description and input parameters.<\/figcaption><\/figure>\n<h2>Answer:<\/h2>\n<p>As discussed in <a href=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/6-12-ultimate-geotechnical-strength-of-piles-subjected-to-axial-compressive-load-from-cpt-test-results\/\">Chapter 6.12<\/a>, the correction factor <em>\u03b1<\/em><em>\u2032<\/em> used in Schmertmann\u2019s method in the determination of the skin friction resistance <em>Q<sub>sf<\/sub><\/em> 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 <a href=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/1-7-the-cone-penetration-test-cpt\/\">Chapter 1.7<\/a>.<\/p>\n<p>1. Calculation of skin friction resistance <em>Q<sub>f<\/sub><\/em> using the method proposed by Schmertmann (1978):<\/p>\n<p style=\"padding-left: 40px\">1.1\u00a0Skin friction resistance along pile shaft embedded in sand (SBT 5\/6):<\/p>\n<p>For the part of the concrete pile that is embedded into sand, the variation of the correction factor <em>\u03b1\u2032<\/em><em>\u00a0<\/em>with depth <em>z<\/em> is determined with the aid of Eq. 6.24 (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/03\/6.55-hr.png\">Figure 6.55<\/a>):<\/p>\n<p>[latex]\\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}[\/latex]<\/p>\n<p>The sand layer is divided into sublayers, the thickness \u0394<em>L<\/em> of which depends on the frequency of sleeve friction resistance <em>f<sub>s<\/sub><\/em> measurements from the CPT test.<\/p>\n<p>The unit friction resistance of each sublayer \u0394<em>Q<sub>f <\/sub><\/em>is then estimated with Eq. 6.23 (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/03\/6.55-hr.png\">Figure 6.55<\/a>):<\/p>\n<p>[latex]\\Delta {Q_{sf}} = {f_{sf}}\\left( {\\pi D} \\right)\\Delta L = \\left( {\\alpha '{f_s}} \\right)\\left( {\\pi D} \\right)dL[\/latex]<\/p>\n<p>and summed to find the skin friction resistance of the pile that develops along the part of the shaft embedded in the sand layer, <em>Q<sub>sf,sand<\/sub><\/em>.<\/p>\n<p>Alternatively, we can use the Bustamante and Gianeselli\u2019s method to estimate <em>Q<sub>sf,sand<\/sub><\/em>. In that case the skin friction resistance along each sublayer is calculated as <em>f<sub>sf<\/sub><\/em> = <em>q<sub>c<\/sub><\/em>\/<em>\u03b1<\/em> where the coefficient <em>\u03b1<\/em> is provided by Table 6.6 for sand with <em>q<sub>c<\/sub><\/em> &gt; 12 MPa (generally <em>q<sub>c<\/sub><\/em>\/<em>p<sub>a<\/sub><\/em> &gt; 120 in the provided data indicating dense sand) and driven precast concrete piles (Category IIA) to be <em>\u03b1<\/em> = 150. The limiting value of <em>f<sub>sf<\/sub><\/em> is from Table 6.6 <em>f<sub>sf<\/sub><\/em> &lt; 120 kPa. Using the provided <em>q<sub>c<\/sub><\/em> values we calculate <em>Q<sub>sf,sand<\/sub><\/em> = 823 kN. There is significant difference between the results of the two methods, and is attributed only partly to the Bustamante and Gianeselli\u2019s method imposing a limiting value to <em>f<sub>sf<\/sub><\/em>, as the <em>f<sub>sf<\/sub><\/em> is exceeded in merely two sublayers.<\/p>\n<p style=\"padding-left: 40px\">1.2 Skin friction resistance along pile shaft embedded in clay (SBT3) and silt (SBT4):<\/p>\n<p>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 <em>\u03b1\u2032<\/em><em>\u00a0<\/em>depends on the sleeve friction resistance, and is provided from Eq. 6.26 for concrete piles (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/03\/6.56-hr.png\">Figure 6.56<\/a>):<\/p>\n<p>[latex]\\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}[\/latex]<\/p>\n<figure id=\"attachment_524\" aria-describedby=\"caption-attachment-524\" style=\"width: 900px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" class=\"wp-image-522 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/6.55-hr-e1743553637824.png\" alt=\"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 \u03b1' corresponding to the sleeve friction resistance. The figure on the right presents the variation of the skin friction force \u0394Qsf developing along pile segments of 0.5 m. The sum of the skin friction force along all segments is Qsf,sand = 1988 kN.\" width=\"900\" height=\"732\" srcset=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.55-hr-e1743553637824.png 900w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.55-hr-e1743553637824-300x244.png 300w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.55-hr-e1743553637824-768x625.png 768w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.55-hr-e1743553637824-65x53.png 65w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.55-hr-e1743553637824-225x183.png 225w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.55-hr-e1743553637824-350x285.png 350w\" sizes=\"(max-width: 900px) 100vw, 900px\" \/><figcaption id=\"caption-attachment-524\" class=\"wp-caption-text\">Figure 6.55. Calculation of pile\u2019s skin friction resistance along the sand layer (SBT5\/6).<\/figcaption><\/figure>\n<figure id=\"attachment_524\" aria-describedby=\"caption-attachment-524\" style=\"width: 900px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" class=\"wp-image-523 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/6.56-hr-e1743553657602.png\" alt=\"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 \u03b1' corresponding to the sleeve friction resistance. The figure on the right presents the variation of the skin friction force \u0394Qsf 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.\" width=\"900\" height=\"750\" srcset=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.56-hr-e1743553657602.png 900w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.56-hr-e1743553657602-300x250.png 300w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.56-hr-e1743553657602-768x640.png 768w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.56-hr-e1743553657602-65x54.png 65w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.56-hr-e1743553657602-225x188.png 225w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.56-hr-e1743553657602-350x292.png 350w\" sizes=\"(max-width: 900px) 100vw, 900px\" \/><figcaption id=\"caption-attachment-524\" class=\"wp-caption-text\">Figure 6.56. Calculation of the pile\u2019s skin friction resistance along the clay (SBT3) and silt (SBT4) layers.<\/figcaption><\/figure>\n<p>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, <em>Q<sub>sf,clay<\/sub><\/em> (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/03\/6.56-hr.png\">Figure 6.56<\/a>).<\/p>\n<p>Again we will use the Bustamante and Gianeselli\u2019s method to estimate <em>Q<sub>sf,clay<\/sub><\/em>, for comparison purposes. Skin friction resistance along each sublayer is again calculated as <em>f<sub>sf<\/sub><\/em> = <em>q<sub>c<\/sub><\/em>\/<em>\u03b1<\/em> where the coefficient <em>\u03b1<\/em> for clay with <em>q<sub>c<\/sub><\/em> = 1 to 5 MPa (firm to stiff clay) and driven precast concrete piles (Category IIA) to be <em>\u03b1<\/em> = 40. The limiting value of <em>f<sub>sf<\/sub><\/em> is from Table 6.6 <em>f<sub>sf<\/sub><\/em> &lt; 35 kPa. Using the provided <em>q<sub>c<\/sub><\/em> values we calculate <em>Q<sub>sf,clay<\/sub><\/em> = 499 kN. Again, there is a significant difference between the results of the two methods.<\/p>\n<p>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\u2019s method is <em>Q<sub>sf<\/sub><\/em> = 2700 kN, and the total skin friction resistance estimated with Bustamante and Gianeselli\u2019s method is <em>Q<sub>sf<\/sub><\/em> = 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.<\/p>\n<p>2. End-bearing resistance, <em>Q<sub>b<\/sub><\/em>:<\/p>\n<p>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 <em>q<sub>c(eq)<\/sub><\/em>, following the procedure described in <a href=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/6-12-ultimate-geotechnical-strength-of-piles-subjected-to-axial-compressive-load-from-cpt-test-results\/\">Chapter 6.12<\/a>:<\/p>\n<ul>\n<li>Consider the cone tip resistance <em>q<sub>c<\/sub><\/em> within a range of 1.5<em>D <\/em>= 1.5 m below the pile toe to 1.5<em>D <\/em>= 1.5 m above the pile toe (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/03\/6.57-detail-and-calculations.png\">Figure 6.57b<\/a>) and calculate the average value of <em>q<sub>c(av) <\/sub><\/em>= 1648 kPa within this zone.<\/li>\n<li>Eliminate <em>q<sub>c <\/sub><\/em>values that are higher than 0.7<em>q<sub>c(av) <\/sub><\/em>and lower than 1.3<em>q<sub>c(av)<\/sub><\/em> (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/03\/6.57-detail-and-calculations.png\">Figure 6.57c<\/a>) and calculate <em>q<sub>c(eq) <\/sub><\/em>= 1482 kPa by averaging the remaining <em>q<sub>c<\/sub><\/em> values.<\/li>\n<\/ul>\n<figure id=\"attachment_524\" aria-describedby=\"caption-attachment-524\" style=\"width: 913px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" class=\"wp-image-524 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/6.57-detail-and-calculations.png\" alt=\"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.\" width=\"913\" height=\"271\" srcset=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.57-detail-and-calculations.png 913w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.57-detail-and-calculations-300x89.png 300w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.57-detail-and-calculations-768x228.png 768w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.57-detail-and-calculations-65x19.png 65w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.57-detail-and-calculations-225x67.png 225w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/6.57-detail-and-calculations-350x104.png 350w\" sizes=\"(max-width: 913px) 100vw, 913px\" \/><figcaption id=\"caption-attachment-524\" class=\"wp-caption-text\">Figure 6.57. (a) Detail of the pile toe area, (b) Calculation of <em>q<\/em><sub>c(av)<\/sub>, and (c) Calculation of <em>q<\/em><sub>c(eq)<\/sub>.<\/figcaption><\/figure>\n<p>Furthermore, as the pile toe is embedded in clay, the empirical bearing capacity factor to be introduced in Eq. 6.29 is <em>k<sub>b <\/sub><\/em>= 0.6 according to Briaud and Miran (1991). Substituting in Eq. 6.29 yields:<\/p>\n<p>[latex]{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}}[\/latex]<\/p>\n<p>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:<\/p>\n<p>[latex]{S_u} = \\dfrac{{{q_t} - {\\sigma _z}}}{{{N_{kt}}}} = \\dfrac{{1482 - {\\sigma _z}}}{{{N_{kt}}}}[\/latex]<\/p>\n<p>If we take an average <em>N<sub>kt<\/sub><\/em> value <em>N<sub>kt<\/sub><\/em> = 15 and an estimate of the total vertical stress at -8 m i.e. <em>\u03c3<\/em><sub>z<\/sub> = 16 x 8 = 128 kPa we calculate at the base of the pile <em>S<sub>u,b<\/sub><\/em> = 90 kPa, which is reasonable for a stiff clay. Using Eq. 6.9 to calculate the end bearing resistance with the <em>\u03b1<\/em>-method we obtain:<\/p>\n<p>[latex]{Q_b} = {N_{cp}}{S_{u,b}}{A_b} = 9 \\times 90 \\times \\pi \\times \\dfrac{{{D^2}}}{4} = 636{\\rm{ \\:kN}}[\/latex]<\/p>\n<p>Such \u201csanity checks\u201d are particularly important, when empirical methods are employed for the design of piles.<\/p>\n<p>3. Ultimate geotechnical strength, <em>Q<sub>f<\/sub><\/em>:<\/p>\n<p>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:<\/p>\n<p>[latex]{Q_f} = {Q_b} + {Q_{sf,sand}} + {Q_{sf,clay}} = 698 + 1988 + 699 = 3385{\\rm{ \\:kN}}[\/latex]\u00a0(using Schmertmann\u2019s method to calculate <em>Q<sub>sf<\/sub><\/em>)<\/p>\n<p>[latex]{Q_f} = {Q_b} + {Q_{sf,sand}} + {Q_{sf,clay}} = 698 + 823 + 499 = 2020{\\rm{ \\:kN}}[\/latex]\u00a0(using Bustamante and Gianeselli\u2019s method to calculate <em>Q<sub>sf<\/sub><\/em>)<\/p>\n","protected":false},"author":1,"menu_order":21,"template":"","meta":{"pb_show_title":"","pb_short_title":"Example 6.6","pb_subtitle":"Estimation of the ultimate geotechnical strength of a pile subjected to axial compressive load based on CPT test results","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"class_list":["post-525","chapter","type-chapter","status-publish","hentry"],"part":421,"_links":{"self":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapters\/525","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/wp\/v2\/users\/1"}],"version-history":[{"count":1,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapters\/525\/revisions"}],"predecessor-version":[{"id":526,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapters\/525\/revisions\/526"}],"part":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/parts\/421"}],"metadata":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapters\/525\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/wp\/v2\/media?parent=525"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapter-type?post=525"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/wp\/v2\/contributor?post=525"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/wp\/v2\/license?post=525"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}