{"id":69,"date":"2024-12-06T05:49:50","date_gmt":"2024-12-06T05:49:50","guid":{"rendered":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/1-7-the-cone-penetration-test-cpt\/"},"modified":"2026-03-16T13:52:40","modified_gmt":"2026-03-16T13:52:40","slug":"1-7-the-cone-penetration-test-cpt","status":"publish","type":"chapter","link":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/1-7-the-cone-penetration-test-cpt\/","title":{"raw":"1.7 The Cone Penetration Test (CPT)","rendered":"1.7 The Cone Penetration Test (CPT)"},"content":{"raw":"A very common method for <em>in situ<\/em> testing of soils is the Cone Penetration Test (CPT). A cone is hydraulically pushed into the soil at a constant rate, and the resistance to the penetration of the cone, as well as the frictional resistance of a surface sleeve, are continuously recorded. Today the piezocone test (CPTu) is more common, where pore pressure is also measured during penetration. Other variants allow for the measurement of S- and P- wave velocities (seismo-cone), moisture content, soil pH etc. A detailed description of the Cone Penetration Test procedure presented herein is included in AS1289.6.5.1.\n\n[caption id=\"attachment_66\" align=\"aligncenter\" width=\"800\"]<img class=\"wp-image-61 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2025\/03\/1.21-replace-e1747982424655.png\" alt=\"Photo of a white truck housing in situ testing equipment labelled with the University of Newcastle and TUNRA logos.\" width=\"800\" height=\"480\"> Figure 1.21. University of Newcastle CPT testing equipment fitted on a truck truck (\u00a9 TUNRA Geotechnic\/University of Newcastle).[\/caption]\n\nThe Cone Penetration Test provides a continuous profile of soil stratigraphy, and allows also for continuous evaluation of soil properties; contrary to the SPT test where information about the soil penetration resistance is obtained at specific intervals. However, soil samples for visual inspection and laboratory index testing are not retrieved, as with the SPT test. CPT tests can be performed in very soft clays to dense sands alike, onshore and offshore (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.21-replace-e1747982424655.png\">Figure 1.21<\/a>). In addition, Cone Penetration Testing is often used in other geotechnical engineering applications, such as estimating the liquefaction potential of loose coarse-grained deposits.\n<p style=\"text-align: left\">However, CPT is unsuitable for gravelly soils, cemented soils and soft rocks, as the cone cannot penetrate through such formations. Some of the advantages and disadvantages of the CPT test are summarised in Table 1.6.<\/p>\nDuring a CPT sounding, the following quantities are measured:\n<ul>\n \t<li>The <em>cone resistance q<sub>c<\/sub><\/em> (units: stress), which results from dividing the total force acting on the cone <em>F<sub>cone<\/sub><\/em> by the projected area of the cone, <em>A<sub>c <\/sub><\/em>(<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.22-replace-e1747982477702.png\">Figure 1.22<\/a>).<\/li>\n \t<li>The <em>sleeve friction resistance f<sub>s<\/sub><\/em> (units: stress) which results from dividing the total friction force acting on the sleeve <em>F<sub>sleeve<\/sub> <\/em>by the area of the sleeve, <em>\u0391<\/em><em><sub>s<\/sub> <\/em>(<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.22-replace-e1747982477702.png\">Figure 1.22<\/a>).<\/li>\n<\/ul>\nThe diameter of standardised cones is 35.7 mm, and their projected area is <em>A<sub>c <\/sub><\/em>= 1000 mm<sup>2<\/sup>.\n<table class=\"grid aligncenter\" style=\"border-collapse: collapse;width: 100%;height: 122px\" border=\"0\"><caption><strong>Table 1.6.<\/strong> Advantages and disadvantages of the CPT test (with information from FHWA, 2006).<\/caption>\n<tbody>\n<tr style=\"height: 15px\">\n<th style=\"width: 50%;text-align: center;height: 15px\">Advantages<\/th>\n<th style=\"width: 50%;text-align: center;height: 15px\">Disadvantages<\/th>\n<\/tr>\n<tr style=\"height: 15px\">\n<td style=\"width: 50%;text-align: center;height: 15px\">Continuous profiling<\/td>\n<td style=\"width: 50%;text-align: center;height: 15px\">No soil samples are retrieved, estimates of soil type are indirect<\/td>\n<\/tr>\n<tr style=\"height: 15px\">\n<td style=\"width: 50%;text-align: center;height: 15px\">Economical and productive. 100 m to 350 m\/day, depending on equipment and soil conditions<\/td>\n<td style=\"width: 50%;text-align: center;height: 15px\">High capital investment<\/td>\n<\/tr>\n<tr style=\"height: 15px\">\n<td style=\"width: 50%;text-align: center;height: 15px\">Results are not operator-dependent<\/td>\n<td style=\"width: 50%;text-align: center;height: 15px\">Requires skilled operator<\/td>\n<\/tr>\n<tr style=\"height: 31px\">\n<td style=\"width: 50%;text-align: center;height: 31px\">Many interpretation methods based on rigorous theoretical background, and not just empiricism<\/td>\n<td style=\"width: 50%;text-align: center;height: 31px\">Requires calibration, noise filtering as well as careful instrument preparation e.g., saturation of pore pressure sensor (tensiometer)<\/td>\n<\/tr>\n<tr style=\"height: 31px\">\n<td style=\"width: 50%;text-align: center;height: 31px\">Particularly suitable for soft soils as well as applications such as assessment of seismic liquefaction potential<\/td>\n<td style=\"width: 50%;text-align: center;height: 31px\">Unsuitable for fills, gravel\/boulder deposits and cemented soils<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n[caption id=\"attachment_66\" align=\"aligncenter\" width=\"1000\"]<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.22-replace-e1747982477702.png\"><img class=\"wp-image-62 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.22-replace-e1747982477702.png\" alt=\"Image on the right shows a sketch of a cone indicating where cone resistance, pore pressure and sleeve friction resistance. Image on the middle is a cross-section of a cone, indicating its various components (load cells, strain gauges, O-rings etc). Image on the right is a photo of a cone equipped with two transducers for pore pressure measurement.\" width=\"1000\" height=\"590\"><\/a> Figure 1.22. (a) Terminology for cone penetrometers, (b) Typical electrical friction-cone penetrometer, and (c) Typical cone featuring two transducers for pore pressure measurement.[\/caption]\n\nCPT testing (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.23-replace-e1747982526282.png\">Figure 1.23<\/a>) must follow some standarised procedures (AS1289.6.5.1):\n<ul>\n \t<li>To avoid damaging the cone when penetrating through artificial compacted fills or surficial hard soils, <em>pre-drilling<\/em> might be necessary.<\/li>\n \t<li>The cone thrust direction should be as near as possible to vertical. Its deviation, measured by means of an inclinometer installed on the rig, should not exceed 2 deg.<\/li>\n \t<li>Reference measurements must be obtained, and zero forces on the cone should be recorded at the start and at the end of each CPT sounding.<\/li>\n \t<li>The rate of penetration of the cone should range between 10 to 20 mm\/sec. This implies that a 20 m CPT sounding can be completed in about 30 min, and excess pore pressures will develop during CPT tests in low permeability soils (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.24-replace-e1747982583471.png\">Figure 1.24<\/a>).<\/li>\n \t<li>Measurements must be obtained at 25 mm to 35 mm intervals for soil under a pavement or for design of pavement depth, or every 150 mm to 200 mm for any other application. This is the minimum interval prescribed in the standard, more frequent measurements are obtained with modern equipment.<\/li>\n \t<li>During a pause in penetration, any excess pore pressure generated around the cone will start to dissipate. The rate of dissipation depends on the coefficient of consolidation, and thus the permeability of the soil. <em>Dissipation tests <\/em>can be performed in fine grained soils at any depth to get estimates of permeability, by measuring the decay of excess pore pressures with time.<\/li>\n \t<li>When CPTu tests are performed in saturated soft clays and silts, the cone resistance <em>q<sub>c<\/sub><\/em> must be corrected to account for the pore water pressure acting on the cone geometry as: <em>q<sub>t<\/sub> = q<sub>c<\/sub>+u<sub>2<\/sub>(1-a) <\/em>where <em>u<sub>2<\/sub><\/em> is the measured pore water pressure and <em>a<\/em> is determined from calibration tests (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.25-replace-e1747982627313.png\">Figure 1.25<\/a>). Generally, the tip area ratio <em>a<\/em> ranges between <em>a <\/em>= 0.70 to 0.85, and should not be less than <em>a <\/em>= 0.75.<\/li>\n<\/ul>\n[caption id=\"attachment_66\" align=\"aligncenter\" width=\"900\"]<img class=\"size-full wp-image-63\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.23-replace-e1747982526282.png\" alt=\"Graphic showing the basic principles of CPT testing according to ASTM D5770. A sketch of a cone is showing where sleeve friction, porewater pressure and tip stress (cone resistance are measured). The relevant symbols for each measured quantity are introduced). An inclinometer is also shown. The formula for correcting the cone resistance for pore pressure effects is also shown. A sketch showing a cone being hydraulically pushed into the ground from a truck indicates standard cone penetration rate, cone diameter, and frequency of reading. The standard dimensions of a cone and the procedure to saturate the cone instruments and obtaining baseline readings is also shown.\" width=\"900\" height=\"648\"> Figure 1.23. (Piezo)cone Penetration Test components and procedures (FHWA 2006, U.S. Govt copyright).[\/caption]\n\nInterpretation of CPT tests is based on theoretical considerations regarding the properties of the failure surface that continuously develops near the cone tip (and around the sleeve) as the cone is being advanced into soil. While interpreting CPT tests one must consider that i) the soil near the cone tip reaches its peak shear strength, while ii) the soil\u2019s residual strength associated with large shear strains is mobilised around the sleeve.\n\n[caption id=\"attachment_66\" align=\"aligncenter\" width=\"1000\"]<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.24-replace-e1747982583471.png\"><img class=\"wp-image-64 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.24-replace-e1747982583471.png\" alt=\"The figure on the left presents results of a numerical simulation of cone penetration in soil, in terms of soil shear strain contours in the vicinity of the cone. Large strains develop around the cone shaft, which demonstrate that the soil in that zone will be at its remolded state. The stress-strain curve of a soil that has reached its remolded state is provided. Near the cone tip a failure surface is formed, and the soil near the cone tip is at its peak strength. The stress-strain curve of a soil that is at its peak strength is provided. The figure on the right presents results of the same simulation, this time in terms of excess pore pressure contours. Large excess pore pressures develop around and below the cone tip.\" width=\"1000\" height=\"494\"><\/a> Figure 1.24. Cone Penetration Test mechanisms and background for interpretation.[\/caption]\n\n[caption id=\"attachment_66\" align=\"aligncenter\" width=\"450\"]<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.25-replace-e1747982627313.png\"><img class=\"wp-image-65 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.25-replace-e1747982627313.png\" alt=\"Cross-section of a piezocone demonstrating pore pressures acting on the cone during cone penetration, in support of the requirement to correct the cone tip resistance for pore pressure effects according to the formula qt=qc+u2(1-a), where a is the area ratio a=An\/Ac\" width=\"450\" height=\"291\"><\/a> Figure 1.25. Correction of cone resistance for unequal end area effects.[\/caption]\n\nConsidering the above, the variation with depth of the following quantities is calculated (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.26-replace-e1747982669134.png\">Figure 1.26<\/a>), according to AS1289.6.5.1:\n\n[caption id=\"attachment_66\" align=\"aligncenter\" width=\"1000\"]<img class=\"wp-image-66 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.26-replace-e1747982669134.png\" alt=\"Variation with depth of cone resistance, skin friction resistance, pore pressure and friction ratio. The interpreted groundwater table is also shown.\" width=\"1000\" height=\"681\"> Figure 1.26. Typical CPTu test measurements.[\/caption]\n\nThe <em>cone resistance q<sub>c<\/sub> <\/em>(kPa), determined as:\n\n<strong>(1.6)<\/strong><em>\u00a0[latex]{q_c} = 1000{F_{cone}} + 9.8{m_g}[\/latex]<\/em>\n\nwhere <em>F<sub>cone<\/sub><\/em> is the force acting on the cone tip (kN), measured by means of a load cell (cone strain gauge load cell, <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.22-replace-e1747982477702.png\">Figure 1.22b<\/a>), and <em>m<sub>g<\/sub><\/em> is mass of the inner rods at the test depth (kg).\n\nIf necessary (i.e., in CPTu tests), cone resistance is corrected for pore pressure development, according to the mentioned above:\n\n<strong>(1.7)<\/strong><em> [latex]{q_t} = {q_c} + {u_2}(1-a)[\/latex]<\/em>\n\nNote that we may use the symbols <em>q<sub>c<\/sub><\/em> and <em>q<sub>t<\/sub><\/em> interchangeably: <em>q<sub>c<\/sub><\/em> refers to cone resistance from CPT tests, and <em>q<sub>t<\/sub><\/em> refers to cone resistance from CPTu tests, which has been correct for pore pressure effects.\n\nThe <em>sleeve friction resistance f<sub>s<\/sub> <\/em>(kPa), determined as:\n\n<strong>(1.8) <\/strong>[latex]{f_s} = \\dfrac{{{F_{sleeve}}}}{{{A_s}}}{10^6}[\/latex]\n\nwhere <em>F<sub>sleeve<\/sub><\/em> is the force on the sleeve, equal to the total force on the cone and sleeve (measured by means of the friction strain gauge load cell,<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.22-replace-e1747982477702.png\"> Figure 1.22b<\/a>) minus the force on the cone alone (kN), and <em>A<sub>s<\/sub> <\/em>is the surface area of the friction sleeve (mm<sup>2<\/sup>).\n\nThe <em>friction ratio <\/em>(%), which is equal to:\n\n<strong>(1.9)<\/strong><em> [latex]{F_R} = \\dfrac{{{f_s}}}{{{q_t}}}100{\\rm{\\: or\\:}}\\dfrac{{{f_s}}}{{{q_c}}} 100[\/latex]<\/em>\n\nand the <em>pore water pressure<\/em> <em>u<sub>2<\/sub><\/em>, measured via a pore pressure transducer installed above the tip of the cone in CPTu rigs.\n\nOne of the main applications of the CPT test is the indirect determination of subsoil stratigraphy i.e., the thickness of soil layers and the soil type. As a rule-of-thumb, the cone resistance <em>q<sub>c<\/sub><\/em> is high in sands and low in clays, and the friction ratio <em>F<sub>R<\/sub><\/em> is high in clays (3% &lt; <em>F<sub>R<\/sub> <\/em>&lt; 10%) and low (0.5% &lt; <em>F<sub>R<\/sub>\u00a0 <\/em>&lt; 1.5%) in sands. It was mentioned before that we cannot obtain soil samples from the CPT test for laboratory characterisation tests. Thus, the CPT test cannot provide direct characterisation of the soil based e.g. on its grain size distribution, but rather of the <em>Soil Behavior Type <\/em>(SBT)<em>,<\/em> a quantity which can be correlated to its mechanical characteristics (Robertson and Kabal, 2022). The Soil Behavior Type is determined from the chart presented in <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/05\/1.27-non-normalised-soil-behaviour-type.png\">Figure 1.27<\/a>, based on the dimensionless cone resistance measured at a particular depth, divided against the atmospheric pressure <em>q<sub>c<\/sub>\/p<sub>a<\/sub> <\/em>(or <em>q<sub>t<\/sub>\/p<sub>a<\/sub><\/em>, if applicable), and the corresponding friction ratio <em>F<sub>R<\/sub> <\/em>at the same depth from Eq. 1.9.\n\n[caption id=\"attachment_66\" align=\"aligncenter\" width=\"1221\"]<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/05\/1.27-non-normalised-soil-behaviour-type.png\"><img class=\"wp-image-67 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.27-non-normalised-soil-behaviour-type.png\" alt=\"Soil behaviour type chart, showing 9 different zones of soil behaviour depending on the cone resistance-friction ratio combination. A table providing the description of each one of the soil behaviour types is provided on the left.\" width=\"1221\" height=\"655\"><\/a> Figure 1.27. Non-normalised Soil Behaviour Type SBT chart (after Robertson and Kabal 2022).[\/caption]\n\nA disadvantage of the soil stratigraphy interpretation method described above is that it does not account for the increase in cone resistance and sleeve friction resistance with overburden stress, as the cone is being pushed deeper into the soil. To alleviate this, interpretation methods based on normalised cone resistance and sleeve friction resistance have been proposed. Such a procedure is described in Robertson and Kabal (2022). First, the normalised cone resistance <em>Q<sub>tn<\/sub><\/em> is calculated as:\n\n<strong>(1.10) <\/strong><em>[latex]{Q_{tn}} = \\left( {\\dfrac{{{q_t} - {{\\sigma '}_{z0}}}}{{{p_a}}}} \\right) {C_c}[\/latex] <\/em><sub>\u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0<\/sub>\n\nwhere <em>\u03c3\u2032<sub>z<\/sub><sub>0<\/sub><\/em> is the effective vertical geostatic stress at the depth where each cone resistance measurement <em>q<sub>t<\/sub><\/em> is obtained, <em>p<sub>a<\/sub><\/em> is the atmospheric pressure and <em>C<sub>c<\/sub><\/em> is a correction factor similar to that of Eq. 1.2, calculated as:\n\n<strong>(1.11) <\/strong><em>[latex]{C_c} = {\\left( {\\dfrac{{{p_a}}}{{{{\\sigma '}_{z0}}}}} \\right)^n}{\\rm{ }}[\/latex]\u00a0 \u00a0 \u00a0 \u00a0 \u00a0<\/em>\n\nwhere <em>n <\/em>\u2264 1.0 is an exponent provided by the following expression:\n\n<strong>(1.12) <\/strong><em>[latex]n = 0.381{I_c} + 0.05\\left( {\\dfrac{{{{\\sigma '}_{z0}}}}{{{p_a}}}} \\right) - 0.15[\/latex]<\/em>\n\nThe factor <em>I<sub>c<\/sub><\/em> is the so-called Soil Behaviour Type index, and is calculated as:\n\n<strong>(1.13)<\/strong> [latex]{I_c} = \\sqrt {{{\\left( {3.47 - \\log {Q_{tn}}} \\right)}^2} + {{\\left( {1.22 + \\log {F_r}} \\right)}^2}} [\/latex]\n\nwhere <em>F<sub>r<\/sub><\/em> (%) is the normalised sleeve friction resistance:\n\n<strong>(1.14)<\/strong><em> [latex]{F_r} = \\left( { \\dfrac{{{f_s}}}{{{q_t} - {\\sigma _{z0}}}} } \\right) 100[\/latex]<\/em>\n\nwhere <em>\u03c3<\/em><em><sub>z<\/sub><\/em><sub>0<\/sub> is the total vertical geostatic stress at the depth where each cone resistance and sleeve friction measurement is obtained. As it is clear from the above expressions, <em>Q<sub>tn<\/sub><\/em> must be calculated iteratively, by assuming an initial value of the exponent <em>n<\/em> e.g., <em>n<\/em> = 1 and iterating until the change in <em>n<\/em> between successive iterations becomes less than \u0394<em>n<\/em> = 0.01.\n\nAccordingly, <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.28-replace-e1747982745895.png\">Figure 1.28<\/a> (Robertson and Kabal 2022) can be used to obtain the Soil Behaviour Type, as well as an estimate of the behaviour of non-cemented soils at large strains (dilative or contractive). CD in <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.28-replace-e1747982745895.png\">Figure 1.28<\/a> defines the boundary between contractive and dilative behaviour, while <em>I<sub>B<\/sub><\/em> is a modified Soil Behaviour Type index that defines the transition zone between sand-like and clay-like behaviour via an intermediate (transitional) soil zone.\n\n[caption id=\"attachment_66\" align=\"aligncenter\" width=\"1000\"]<img class=\"wp-image-4015 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.28-replace-e1747982745895.png\" alt=\"Chart providing the soil behaviour type as function of normalised cone resistance-normalised sleeve friction resistance measurements. Seven different soil behaviour types are identified, depending on the grain size distribution (clay-like, sand-like) and the shearing response (contractive, dilative).\" width=\"1000\" height=\"607\"> Figure 1.28. Normalised Soil Behaviour Type SBT chart (after Robertson and Kabal 2022).[\/caption]\n\nAn example soil behavior type profile determined with the method depicted in <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/05\/1.27-non-normalised-soil-behaviour-type.png\">Figure 1.27<\/a> is presented in <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/05\/1.29-example-soil-stratigraphy.png\">Figure 1.29<\/a>. Different dots in the soil behavior type chart correspond to different cone resistance\/friction ratio pairs, depicted from their distribution with depth on the left. Depending on the zone of the chart where each dot lies, a SBT is assigned to each pair, and a different color is used. Using the distribution of SBT with depth, different layers can be identified along the soil profile, as presented on the right.\u00a0 Although it is clear that CPT provides a more \u201cobjective\u201d evaluation of the soil profile, based on the SBT chart, engineering judgment is always necessary to interpret a rational soil stratigraphy.","rendered":"<p>A very common method for <em>in situ<\/em> testing of soils is the Cone Penetration Test (CPT). A cone is hydraulically pushed into the soil at a constant rate, and the resistance to the penetration of the cone, as well as the frictional resistance of a surface sleeve, are continuously recorded. Today the piezocone test (CPTu) is more common, where pore pressure is also measured during penetration. Other variants allow for the measurement of S- and P- wave velocities (seismo-cone), moisture content, soil pH etc. A detailed description of the Cone Penetration Test procedure presented herein is included in AS1289.6.5.1.<\/p>\n<figure id=\"attachment_66\" aria-describedby=\"caption-attachment-66\" style=\"width: 800px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" class=\"wp-image-61 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2025\/03\/1.21-replace-e1747982424655.png\" alt=\"Photo of a white truck housing in situ testing equipment labelled with the University of Newcastle and TUNRA logos.\" width=\"800\" height=\"480\" srcset=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/03\/1.21-replace-e1747982424655.png 800w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/03\/1.21-replace-e1747982424655-300x180.png 300w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/03\/1.21-replace-e1747982424655-768x461.png 768w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/03\/1.21-replace-e1747982424655-65x39.png 65w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/03\/1.21-replace-e1747982424655-225x135.png 225w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/03\/1.21-replace-e1747982424655-350x210.png 350w\" sizes=\"(max-width: 800px) 100vw, 800px\" \/><figcaption id=\"caption-attachment-66\" class=\"wp-caption-text\">Figure 1.21. University of Newcastle CPT testing equipment fitted on a truck truck (\u00a9 TUNRA Geotechnic\/University of Newcastle).<\/figcaption><\/figure>\n<p>The Cone Penetration Test provides a continuous profile of soil stratigraphy, and allows also for continuous evaluation of soil properties; contrary to the SPT test where information about the soil penetration resistance is obtained at specific intervals. However, soil samples for visual inspection and laboratory index testing are not retrieved, as with the SPT test. CPT tests can be performed in very soft clays to dense sands alike, onshore and offshore (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.21-replace-e1747982424655.png\">Figure 1.21<\/a>). In addition, Cone Penetration Testing is often used in other geotechnical engineering applications, such as estimating the liquefaction potential of loose coarse-grained deposits.<\/p>\n<p style=\"text-align: left\">However, CPT is unsuitable for gravelly soils, cemented soils and soft rocks, as the cone cannot penetrate through such formations. Some of the advantages and disadvantages of the CPT test are summarised in Table 1.6.<\/p>\n<p>During a CPT sounding, the following quantities are measured:<\/p>\n<ul>\n<li>The <em>cone resistance q<sub>c<\/sub><\/em> (units: stress), which results from dividing the total force acting on the cone <em>F<sub>cone<\/sub><\/em> by the projected area of the cone, <em>A<sub>c <\/sub><\/em>(<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.22-replace-e1747982477702.png\">Figure 1.22<\/a>).<\/li>\n<li>The <em>sleeve friction resistance f<sub>s<\/sub><\/em> (units: stress) which results from dividing the total friction force acting on the sleeve <em>F<sub>sleeve<\/sub> <\/em>by the area of the sleeve, <em>\u0391<\/em><em><sub>s<\/sub> <\/em>(<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.22-replace-e1747982477702.png\">Figure 1.22<\/a>).<\/li>\n<\/ul>\n<p>The diameter of standardised cones is 35.7 mm, and their projected area is <em>A<sub>c <\/sub><\/em>= 1000 mm<sup>2<\/sup>.<\/p>\n<table class=\"grid aligncenter\" style=\"border-collapse: collapse;width: 100%;height: 122px\">\n<caption><strong>Table 1.6.<\/strong> Advantages and disadvantages of the CPT test (with information from FHWA, 2006).<\/caption>\n<tbody>\n<tr style=\"height: 15px\">\n<th style=\"width: 50%;text-align: center;height: 15px\">Advantages<\/th>\n<th style=\"width: 50%;text-align: center;height: 15px\">Disadvantages<\/th>\n<\/tr>\n<tr style=\"height: 15px\">\n<td style=\"width: 50%;text-align: center;height: 15px\">Continuous profiling<\/td>\n<td style=\"width: 50%;text-align: center;height: 15px\">No soil samples are retrieved, estimates of soil type are indirect<\/td>\n<\/tr>\n<tr style=\"height: 15px\">\n<td style=\"width: 50%;text-align: center;height: 15px\">Economical and productive. 100 m to 350 m\/day, depending on equipment and soil conditions<\/td>\n<td style=\"width: 50%;text-align: center;height: 15px\">High capital investment<\/td>\n<\/tr>\n<tr style=\"height: 15px\">\n<td style=\"width: 50%;text-align: center;height: 15px\">Results are not operator-dependent<\/td>\n<td style=\"width: 50%;text-align: center;height: 15px\">Requires skilled operator<\/td>\n<\/tr>\n<tr style=\"height: 31px\">\n<td style=\"width: 50%;text-align: center;height: 31px\">Many interpretation methods based on rigorous theoretical background, and not just empiricism<\/td>\n<td style=\"width: 50%;text-align: center;height: 31px\">Requires calibration, noise filtering as well as careful instrument preparation e.g., saturation of pore pressure sensor (tensiometer)<\/td>\n<\/tr>\n<tr style=\"height: 31px\">\n<td style=\"width: 50%;text-align: center;height: 31px\">Particularly suitable for soft soils as well as applications such as assessment of seismic liquefaction potential<\/td>\n<td style=\"width: 50%;text-align: center;height: 31px\">Unsuitable for fills, gravel\/boulder deposits and cemented soils<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<figure id=\"attachment_66\" aria-describedby=\"caption-attachment-66\" style=\"width: 1000px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.22-replace-e1747982477702.png\"><img decoding=\"async\" class=\"wp-image-62 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.22-replace-e1747982477702.png\" alt=\"Image on the right shows a sketch of a cone indicating where cone resistance, pore pressure and sleeve friction resistance. Image on the middle is a cross-section of a cone, indicating its various components (load cells, strain gauges, O-rings etc). Image on the right is a photo of a cone equipped with two transducers for pore pressure measurement.\" width=\"1000\" height=\"590\" srcset=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.22-replace-e1747982477702.png 1000w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.22-replace-e1747982477702-300x177.png 300w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.22-replace-e1747982477702-768x453.png 768w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.22-replace-e1747982477702-65x38.png 65w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.22-replace-e1747982477702-225x133.png 225w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.22-replace-e1747982477702-350x207.png 350w\" sizes=\"(max-width: 1000px) 100vw, 1000px\" \/><\/a><figcaption id=\"caption-attachment-66\" class=\"wp-caption-text\">Figure 1.22. (a) Terminology for cone penetrometers, (b) Typical electrical friction-cone penetrometer, and (c) Typical cone featuring two transducers for pore pressure measurement.<\/figcaption><\/figure>\n<p>CPT testing (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.23-replace-e1747982526282.png\">Figure 1.23<\/a>) must follow some standarised procedures (AS1289.6.5.1):<\/p>\n<ul>\n<li>To avoid damaging the cone when penetrating through artificial compacted fills or surficial hard soils, <em>pre-drilling<\/em> might be necessary.<\/li>\n<li>The cone thrust direction should be as near as possible to vertical. Its deviation, measured by means of an inclinometer installed on the rig, should not exceed 2 deg.<\/li>\n<li>Reference measurements must be obtained, and zero forces on the cone should be recorded at the start and at the end of each CPT sounding.<\/li>\n<li>The rate of penetration of the cone should range between 10 to 20 mm\/sec. This implies that a 20 m CPT sounding can be completed in about 30 min, and excess pore pressures will develop during CPT tests in low permeability soils (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.24-replace-e1747982583471.png\">Figure 1.24<\/a>).<\/li>\n<li>Measurements must be obtained at 25 mm to 35 mm intervals for soil under a pavement or for design of pavement depth, or every 150 mm to 200 mm for any other application. This is the minimum interval prescribed in the standard, more frequent measurements are obtained with modern equipment.<\/li>\n<li>During a pause in penetration, any excess pore pressure generated around the cone will start to dissipate. The rate of dissipation depends on the coefficient of consolidation, and thus the permeability of the soil. <em>Dissipation tests <\/em>can be performed in fine grained soils at any depth to get estimates of permeability, by measuring the decay of excess pore pressures with time.<\/li>\n<li>When CPTu tests are performed in saturated soft clays and silts, the cone resistance <em>q<sub>c<\/sub><\/em> must be corrected to account for the pore water pressure acting on the cone geometry as: <em>q<sub>t<\/sub> = q<sub>c<\/sub>+u<sub>2<\/sub>(1-a) <\/em>where <em>u<sub>2<\/sub><\/em> is the measured pore water pressure and <em>a<\/em> is determined from calibration tests (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.25-replace-e1747982627313.png\">Figure 1.25<\/a>). Generally, the tip area ratio <em>a<\/em> ranges between <em>a <\/em>= 0.70 to 0.85, and should not be less than <em>a <\/em>= 0.75.<\/li>\n<\/ul>\n<figure id=\"attachment_66\" aria-describedby=\"caption-attachment-66\" style=\"width: 900px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" class=\"size-full wp-image-63\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.23-replace-e1747982526282.png\" alt=\"Graphic showing the basic principles of CPT testing according to ASTM D5770. A sketch of a cone is showing where sleeve friction, porewater pressure and tip stress (cone resistance are measured). The relevant symbols for each measured quantity are introduced). An inclinometer is also shown. The formula for correcting the cone resistance for pore pressure effects is also shown. A sketch showing a cone being hydraulically pushed into the ground from a truck indicates standard cone penetration rate, cone diameter, and frequency of reading. The standard dimensions of a cone and the procedure to saturate the cone instruments and obtaining baseline readings is also shown.\" width=\"900\" height=\"648\" srcset=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.23-replace-e1747982526282.png 900w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.23-replace-e1747982526282-300x216.png 300w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.23-replace-e1747982526282-768x553.png 768w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.23-replace-e1747982526282-65x47.png 65w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.23-replace-e1747982526282-225x162.png 225w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.23-replace-e1747982526282-350x252.png 350w\" sizes=\"(max-width: 900px) 100vw, 900px\" \/><figcaption id=\"caption-attachment-66\" class=\"wp-caption-text\">Figure 1.23. (Piezo)cone Penetration Test components and procedures (FHWA 2006, U.S. Govt copyright).<\/figcaption><\/figure>\n<p>Interpretation of CPT tests is based on theoretical considerations regarding the properties of the failure surface that continuously develops near the cone tip (and around the sleeve) as the cone is being advanced into soil. While interpreting CPT tests one must consider that i) the soil near the cone tip reaches its peak shear strength, while ii) the soil\u2019s residual strength associated with large shear strains is mobilised around the sleeve.<\/p>\n<figure id=\"attachment_66\" aria-describedby=\"caption-attachment-66\" style=\"width: 1000px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.24-replace-e1747982583471.png\"><img decoding=\"async\" class=\"wp-image-64 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.24-replace-e1747982583471.png\" alt=\"The figure on the left presents results of a numerical simulation of cone penetration in soil, in terms of soil shear strain contours in the vicinity of the cone. Large strains develop around the cone shaft, which demonstrate that the soil in that zone will be at its remolded state. The stress-strain curve of a soil that has reached its remolded state is provided. Near the cone tip a failure surface is formed, and the soil near the cone tip is at its peak strength. The stress-strain curve of a soil that is at its peak strength is provided. The figure on the right presents results of the same simulation, this time in terms of excess pore pressure contours. Large excess pore pressures develop around and below the cone tip.\" width=\"1000\" height=\"494\" srcset=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.24-replace-e1747982583471.png 1000w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.24-replace-e1747982583471-300x148.png 300w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.24-replace-e1747982583471-768x379.png 768w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.24-replace-e1747982583471-65x32.png 65w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.24-replace-e1747982583471-225x111.png 225w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.24-replace-e1747982583471-350x173.png 350w\" sizes=\"(max-width: 1000px) 100vw, 1000px\" \/><\/a><figcaption id=\"caption-attachment-66\" class=\"wp-caption-text\">Figure 1.24. Cone Penetration Test mechanisms and background for interpretation.<\/figcaption><\/figure>\n<figure id=\"attachment_66\" aria-describedby=\"caption-attachment-66\" style=\"width: 450px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.25-replace-e1747982627313.png\"><img decoding=\"async\" class=\"wp-image-65 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.25-replace-e1747982627313.png\" alt=\"Cross-section of a piezocone demonstrating pore pressures acting on the cone during cone penetration, in support of the requirement to correct the cone tip resistance for pore pressure effects according to the formula qt=qc+u2(1-a), where a is the area ratio a=An\/Ac\" width=\"450\" height=\"291\" srcset=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.25-replace-e1747982627313.png 450w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.25-replace-e1747982627313-300x194.png 300w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.25-replace-e1747982627313-65x42.png 65w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.25-replace-e1747982627313-225x146.png 225w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.25-replace-e1747982627313-350x226.png 350w\" sizes=\"(max-width: 450px) 100vw, 450px\" \/><\/a><figcaption id=\"caption-attachment-66\" class=\"wp-caption-text\">Figure 1.25. Correction of cone resistance for unequal end area effects.<\/figcaption><\/figure>\n<p>Considering the above, the variation with depth of the following quantities is calculated (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.26-replace-e1747982669134.png\">Figure 1.26<\/a>), according to AS1289.6.5.1:<\/p>\n<figure id=\"attachment_66\" aria-describedby=\"caption-attachment-66\" style=\"width: 1000px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" class=\"wp-image-66 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.26-replace-e1747982669134.png\" alt=\"Variation with depth of cone resistance, skin friction resistance, pore pressure and friction ratio. The interpreted groundwater table is also shown.\" width=\"1000\" height=\"681\" srcset=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.26-replace-e1747982669134.png 1000w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.26-replace-e1747982669134-300x204.png 300w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.26-replace-e1747982669134-768x523.png 768w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.26-replace-e1747982669134-65x44.png 65w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.26-replace-e1747982669134-225x153.png 225w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.26-replace-e1747982669134-350x238.png 350w\" sizes=\"(max-width: 1000px) 100vw, 1000px\" \/><figcaption id=\"caption-attachment-66\" class=\"wp-caption-text\">Figure 1.26. Typical CPTu test measurements.<\/figcaption><\/figure>\n<p>The <em>cone resistance q<sub>c<\/sub> <\/em>(kPa), determined as:<\/p>\n<p><strong>(1.6)<\/strong><em>\u00a0[latex]{q_c} = 1000{F_{cone}} + 9.8{m_g}[\/latex]<\/em><\/p>\n<p>where <em>F<sub>cone<\/sub><\/em> is the force acting on the cone tip (kN), measured by means of a load cell (cone strain gauge load cell, <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.22-replace-e1747982477702.png\">Figure 1.22b<\/a>), and <em>m<sub>g<\/sub><\/em> is mass of the inner rods at the test depth (kg).<\/p>\n<p>If necessary (i.e., in CPTu tests), cone resistance is corrected for pore pressure development, according to the mentioned above:<\/p>\n<p><strong>(1.7)<\/strong><em> [latex]{q_t} = {q_c} + {u_2}(1-a)[\/latex]<\/em><\/p>\n<p>Note that we may use the symbols <em>q<sub>c<\/sub><\/em> and <em>q<sub>t<\/sub><\/em> interchangeably: <em>q<sub>c<\/sub><\/em> refers to cone resistance from CPT tests, and <em>q<sub>t<\/sub><\/em> refers to cone resistance from CPTu tests, which has been correct for pore pressure effects.<\/p>\n<p>The <em>sleeve friction resistance f<sub>s<\/sub> <\/em>(kPa), determined as:<\/p>\n<p><strong>(1.8) <\/strong>[latex]{f_s} = \\dfrac{{{F_{sleeve}}}}{{{A_s}}}{10^6}[\/latex]<\/p>\n<p>where <em>F<sub>sleeve<\/sub><\/em> is the force on the sleeve, equal to the total force on the cone and sleeve (measured by means of the friction strain gauge load cell,<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.22-replace-e1747982477702.png\"> Figure 1.22b<\/a>) minus the force on the cone alone (kN), and <em>A<sub>s<\/sub> <\/em>is the surface area of the friction sleeve (mm<sup>2<\/sup>).<\/p>\n<p>The <em>friction ratio <\/em>(%), which is equal to:<\/p>\n<p><strong>(1.9)<\/strong><em> [latex]{F_R} = \\dfrac{{{f_s}}}{{{q_t}}}100{\\rm{\\: or\\:}}\\dfrac{{{f_s}}}{{{q_c}}} 100[\/latex]<\/em><\/p>\n<p>and the <em>pore water pressure<\/em> <em>u<sub>2<\/sub><\/em>, measured via a pore pressure transducer installed above the tip of the cone in CPTu rigs.<\/p>\n<p>One of the main applications of the CPT test is the indirect determination of subsoil stratigraphy i.e., the thickness of soil layers and the soil type. As a rule-of-thumb, the cone resistance <em>q<sub>c<\/sub><\/em> is high in sands and low in clays, and the friction ratio <em>F<sub>R<\/sub><\/em> is high in clays (3% &lt; <em>F<sub>R<\/sub> <\/em>&lt; 10%) and low (0.5% &lt; <em>F<sub>R<\/sub>\u00a0 <\/em>&lt; 1.5%) in sands. It was mentioned before that we cannot obtain soil samples from the CPT test for laboratory characterisation tests. Thus, the CPT test cannot provide direct characterisation of the soil based e.g. on its grain size distribution, but rather of the <em>Soil Behavior Type <\/em>(SBT)<em>,<\/em> a quantity which can be correlated to its mechanical characteristics (Robertson and Kabal, 2022). The Soil Behavior Type is determined from the chart presented in <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/05\/1.27-non-normalised-soil-behaviour-type.png\">Figure 1.27<\/a>, based on the dimensionless cone resistance measured at a particular depth, divided against the atmospheric pressure <em>q<sub>c<\/sub>\/p<sub>a<\/sub> <\/em>(or <em>q<sub>t<\/sub>\/p<sub>a<\/sub><\/em>, if applicable), and the corresponding friction ratio <em>F<sub>R<\/sub> <\/em>at the same depth from Eq. 1.9.<\/p>\n<figure id=\"attachment_66\" aria-describedby=\"caption-attachment-66\" style=\"width: 1221px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/05\/1.27-non-normalised-soil-behaviour-type.png\"><img decoding=\"async\" class=\"wp-image-67 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.27-non-normalised-soil-behaviour-type.png\" alt=\"Soil behaviour type chart, showing 9 different zones of soil behaviour depending on the cone resistance-friction ratio combination. A table providing the description of each one of the soil behaviour types is provided on the left.\" width=\"1221\" height=\"655\" srcset=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.27-non-normalised-soil-behaviour-type.png 1221w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.27-non-normalised-soil-behaviour-type-300x161.png 300w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.27-non-normalised-soil-behaviour-type-1024x549.png 1024w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.27-non-normalised-soil-behaviour-type-768x412.png 768w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.27-non-normalised-soil-behaviour-type-65x35.png 65w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.27-non-normalised-soil-behaviour-type-225x121.png 225w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2026\/03\/1.27-non-normalised-soil-behaviour-type-350x188.png 350w\" sizes=\"(max-width: 1221px) 100vw, 1221px\" \/><\/a><figcaption id=\"caption-attachment-66\" class=\"wp-caption-text\">Figure 1.27. Non-normalised Soil Behaviour Type SBT chart (after Robertson and Kabal 2022).<\/figcaption><\/figure>\n<p>A disadvantage of the soil stratigraphy interpretation method described above is that it does not account for the increase in cone resistance and sleeve friction resistance with overburden stress, as the cone is being pushed deeper into the soil. To alleviate this, interpretation methods based on normalised cone resistance and sleeve friction resistance have been proposed. Such a procedure is described in Robertson and Kabal (2022). First, the normalised cone resistance <em>Q<sub>tn<\/sub><\/em> is calculated as:<\/p>\n<p><strong>(1.10) <\/strong><em>[latex]{Q_{tn}} = \\left( {\\dfrac{{{q_t} - {{\\sigma '}_{z0}}}}{{{p_a}}}} \\right) {C_c}[\/latex] <\/em><sub>\u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0<\/sub><\/p>\n<p>where <em>\u03c3\u2032<sub>z<\/sub><sub>0<\/sub><\/em> is the effective vertical geostatic stress at the depth where each cone resistance measurement <em>q<sub>t<\/sub><\/em> is obtained, <em>p<sub>a<\/sub><\/em> is the atmospheric pressure and <em>C<sub>c<\/sub><\/em> is a correction factor similar to that of Eq. 1.2, calculated as:<\/p>\n<p><strong>(1.11) <\/strong><em>[latex]{C_c} = {\\left( {\\dfrac{{{p_a}}}{{{{\\sigma '}_{z0}}}}} \\right)^n}{\\rm{ }}[\/latex]\u00a0 \u00a0 \u00a0 \u00a0 \u00a0<\/em><\/p>\n<p>where <em>n <\/em>\u2264 1.0 is an exponent provided by the following expression:<\/p>\n<p><strong>(1.12) <\/strong><em>[latex]n = 0.381{I_c} + 0.05\\left( {\\dfrac{{{{\\sigma '}_{z0}}}}{{{p_a}}}} \\right) - 0.15[\/latex]<\/em><\/p>\n<p>The factor <em>I<sub>c<\/sub><\/em> is the so-called Soil Behaviour Type index, and is calculated as:<\/p>\n<p><strong>(1.13)<\/strong> [latex]{I_c} = \\sqrt {{{\\left( {3.47 - \\log {Q_{tn}}} \\right)}^2} + {{\\left( {1.22 + \\log {F_r}} \\right)}^2}}[\/latex]<\/p>\n<p>where <em>F<sub>r<\/sub><\/em> (%) is the normalised sleeve friction resistance:<\/p>\n<p><strong>(1.14)<\/strong><em> [latex]{F_r} = \\left( { \\dfrac{{{f_s}}}{{{q_t} - {\\sigma _{z0}}}} } \\right) 100[\/latex]<\/em><\/p>\n<p>where <em>\u03c3<\/em><em><sub>z<\/sub><\/em><sub>0<\/sub> is the total vertical geostatic stress at the depth where each cone resistance and sleeve friction measurement is obtained. As it is clear from the above expressions, <em>Q<sub>tn<\/sub><\/em> must be calculated iteratively, by assuming an initial value of the exponent <em>n<\/em> e.g., <em>n<\/em> = 1 and iterating until the change in <em>n<\/em> between successive iterations becomes less than \u0394<em>n<\/em> = 0.01.<\/p>\n<p>Accordingly, <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.28-replace-e1747982745895.png\">Figure 1.28<\/a> (Robertson and Kabal 2022) can be used to obtain the Soil Behaviour Type, as well as an estimate of the behaviour of non-cemented soils at large strains (dilative or contractive). CD in <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2024\/12\/1.28-replace-e1747982745895.png\">Figure 1.28<\/a> defines the boundary between contractive and dilative behaviour, while <em>I<sub>B<\/sub><\/em> is a modified Soil Behaviour Type index that defines the transition zone between sand-like and clay-like behaviour via an intermediate (transitional) soil zone.<\/p>\n<figure id=\"attachment_66\" aria-describedby=\"caption-attachment-66\" style=\"width: 1000px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" class=\"wp-image-4015 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2026\/03\/1.28-replace-e1747982745895.png\" alt=\"Chart providing the soil behaviour type as function of normalised cone resistance-normalised sleeve friction resistance measurements. Seven different soil behaviour types are identified, depending on the grain size distribution (clay-like, sand-like) and the shearing response (contractive, dilative).\" width=\"1000\" height=\"607\" \/><figcaption id=\"caption-attachment-66\" class=\"wp-caption-text\">Figure 1.28. Normalised Soil Behaviour Type SBT chart (after Robertson and Kabal 2022).<\/figcaption><\/figure>\n<p>An example soil behavior type profile determined with the method depicted in <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/05\/1.27-non-normalised-soil-behaviour-type.png\">Figure 1.27<\/a> is presented in <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/05\/1.29-example-soil-stratigraphy.png\">Figure 1.29<\/a>. Different dots in the soil behavior type chart correspond to different cone resistance\/friction ratio pairs, depicted from their distribution with depth on the left. Depending on the zone of the chart where each dot lies, a SBT is assigned to each pair, and a different color is used. Using the distribution of SBT with depth, different layers can be identified along the soil profile, as presented on the right.\u00a0 Although it is clear that CPT provides a more \u201cobjective\u201d evaluation of the soil profile, based on the SBT chart, engineering judgment is always necessary to interpret a rational soil stratigraphy.<\/p>\n","protected":false},"author":1,"menu_order":8,"template":"","meta":{"pb_show_title":"","pb_short_title":"1.7 The Cone Penetration Test (CPT)","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"class_list":["post-69","chapter","type-chapter","status-publish","hentry"],"part":24,"_links":{"self":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapters\/69","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\/69\/revisions"}],"predecessor-version":[{"id":70,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapters\/69\/revisions\/70"}],"part":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/parts\/24"}],"metadata":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapters\/69\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/wp\/v2\/media?parent=69"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapter-type?post=69"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/wp\/v2\/contributor?post=69"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/wp\/v2\/license?post=69"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}