{"id":173,"date":"2025-01-08T22:48:59","date_gmt":"2025-01-08T22:48:59","guid":{"rendered":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/3-2-stresses-in-the-soil-due-to-a-point-load\/"},"modified":"2026-03-16T13:56:55","modified_gmt":"2026-03-16T13:56:55","slug":"3-2-stresses-in-the-soil-due-to-a-point-load","status":"publish","type":"chapter","link":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/chapter\/3-2-stresses-in-the-soil-due-to-a-point-load\/","title":{"raw":"3.2 Stresses in the soil due to a point load","rendered":"3.2 Stresses in the soil due to a point load"},"content":{"raw":"Load transferred to the soil from e.g., the foundation of an electric power pole can be simulated as a point load <em>Q<sub>ext<\/sub><\/em> acting on the surface of a homogeneous elastic half-space (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/01\/3.5-replace-e1747991485946.png\">Figure 3.5<\/a>). As both load and geometry are axisymmetric, additional soil stresses due to the application of the load can be calculated as:\n\n[caption id=\"attachment_172\" align=\"aligncenter\" width=\"400\"]<img class=\"wp-image-172 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2025\/01\/3.5-replace-e1747991485946.png\" alt=\"Diagram depicting a point load acting on the surface of a half space, resulting in radial (\u0394\u03c3_r), axial (\u0394\u03c3_z), and tangential (\u0394\u03c3_\u03b8) stresses at depth z and radial distance r from the point load.\" width=\"400\" height=\"269\"> Figure 3.5. Stresses due to point load acting on the surface of a homogeneous elastic half-space.[\/caption]\n\n<strong>(3.1)<\/strong> [latex]\\Delta {\\sigma _z} = \\dfrac{{3{Q_{ext}}}}{{2\\pi {z^2}{{\\left[ {1 + {{\\left( {\\dfrac{r}{z}} \\right)}^2}} \\right]}^{\\tfrac{5}{2}}}}}[\/latex]\n\n<strong>(3.2) <\/strong>[latex]\\Delta {\\sigma _r} = \\dfrac{{{Q_{ext}}}}{{2\\pi }}\\left( {\\dfrac{{3{r^2}z}}{{{{\\left( {{r^2} + {z^2}} \\right)}^{\\tfrac{5}{2}}}}} - \\dfrac{{\\left( {1 - 2{\\nu _s}} \\right)}}{{{r^2} + {z^2} + z{{\\left( {{r^2} + {z^2}} \\right)}^{\\tfrac{1}{2}}}}}} \\right) [\/latex]\n\n<strong>(3.3)<\/strong> [latex]\\Delta {\\sigma _\\theta } = \\dfrac{{{Q_{ext}}}}{{2\\pi }}\\left( {1 - 2{\\nu _s}} \\right)\\left( {\\dfrac{z}{{{{\\left( {{r^2} + {z^2}} \\right)}^{\\tfrac{3}{2}}}}} - \\dfrac{1}{{{r^2} + {z^2} + z{{\\left( {{r^2} + {z^2}} \\right)}^{\\tfrac{1}{2}}}}}} \\right)[\/latex]\n\n<strong>(3.4)<\/strong> [latex]\\Delta {\\tau _{rz}} = \\dfrac{{3{Q_{ext}}}}{{2\\pi }}\\left( {\\dfrac{{r{z^2}}}{{{{\\left( {{r^2} + {z^2}} \\right)}^{\\tfrac{5}{2}}}}}} \\right)[\/latex]\n\nThe above expressions provide the <em>stress increments <\/em>\u0394<em>\u03c3<\/em> due to the application of the point load, which should be added to existing geostatic stresses to find the total stress in the soil. In Eqs. 3.1 to 3.4 <em>v<sub>s <\/sub><\/em>is the Poisson ratio of the soil, while the corresponding stress components \u0394<em>\u03c3<\/em><sub>z<\/sub>, \u0394<em>\u03c3<\/em><sub>r<\/sub><em>, <\/em>\u0394<em>\u03c3<sub>\u03b8<\/sub><\/em> and \u0394<em>\u03c4<\/em><sub>rz<\/sub> and the vertical <em>z<\/em> and radial <em>r<\/em> distance from the point load are defined in <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/01\/3.5-stresses-point-load.png\">Figure 3.5<\/a>.","rendered":"<p>Load transferred to the soil from e.g., the foundation of an electric power pole can be simulated as a point load <em>Q<sub>ext<\/sub><\/em> acting on the surface of a homogeneous elastic half-space (<a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/01\/3.5-replace-e1747991485946.png\">Figure 3.5<\/a>). As both load and geometry are axisymmetric, additional soil stresses due to the application of the load can be calculated as:<\/p>\n<figure id=\"attachment_172\" aria-describedby=\"caption-attachment-172\" style=\"width: 400px\" class=\"wp-caption aligncenter\"><img decoding=\"async\" class=\"wp-image-172 size-full\" src=\"https:\/\/libraryresources.nse.org.ng\/wp-content\/uploads\/sites\/9\/2025\/01\/3.5-replace-e1747991485946.png\" alt=\"Diagram depicting a point load acting on the surface of a half space, resulting in radial (\u0394\u03c3_r), axial (\u0394\u03c3_z), and tangential (\u0394\u03c3_\u03b8) stresses at depth z and radial distance r from the point load.\" width=\"400\" height=\"269\" srcset=\"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/01\/3.5-replace-e1747991485946.png 400w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/01\/3.5-replace-e1747991485946-300x202.png 300w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/01\/3.5-replace-e1747991485946-65x44.png 65w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/01\/3.5-replace-e1747991485946-225x151.png 225w, https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-content\/uploads\/sites\/9\/2025\/01\/3.5-replace-e1747991485946-350x235.png 350w\" sizes=\"(max-width: 400px) 100vw, 400px\" \/><figcaption id=\"caption-attachment-172\" class=\"wp-caption-text\">Figure 3.5. Stresses due to point load acting on the surface of a homogeneous elastic half-space.<\/figcaption><\/figure>\n<p><strong>(3.1)<\/strong> [latex]\\Delta {\\sigma _z} = \\dfrac{{3{Q_{ext}}}}{{2\\pi {z^2}{{\\left[ {1 + {{\\left( {\\dfrac{r}{z}} \\right)}^2}} \\right]}^{\\tfrac{5}{2}}}}}[\/latex]<\/p>\n<p><strong>(3.2) <\/strong>[latex]\\Delta {\\sigma _r} = \\dfrac{{{Q_{ext}}}}{{2\\pi }}\\left( {\\dfrac{{3{r^2}z}}{{{{\\left( {{r^2} + {z^2}} \\right)}^{\\tfrac{5}{2}}}}} - \\dfrac{{\\left( {1 - 2{\\nu _s}} \\right)}}{{{r^2} + {z^2} + z{{\\left( {{r^2} + {z^2}} \\right)}^{\\tfrac{1}{2}}}}}} \\right)[\/latex]<\/p>\n<p><strong>(3.3)<\/strong> [latex]\\Delta {\\sigma _\\theta } = \\dfrac{{{Q_{ext}}}}{{2\\pi }}\\left( {1 - 2{\\nu _s}} \\right)\\left( {\\dfrac{z}{{{{\\left( {{r^2} + {z^2}} \\right)}^{\\tfrac{3}{2}}}}} - \\dfrac{1}{{{r^2} + {z^2} + z{{\\left( {{r^2} + {z^2}} \\right)}^{\\tfrac{1}{2}}}}}} \\right)[\/latex]<\/p>\n<p><strong>(3.4)<\/strong> [latex]\\Delta {\\tau _{rz}} = \\dfrac{{3{Q_{ext}}}}{{2\\pi }}\\left( {\\dfrac{{r{z^2}}}{{{{\\left( {{r^2} + {z^2}} \\right)}^{\\tfrac{5}{2}}}}}} \\right)[\/latex]<\/p>\n<p>The above expressions provide the <em>stress increments <\/em>\u0394<em>\u03c3<\/em> due to the application of the point load, which should be added to existing geostatic stresses to find the total stress in the soil. In Eqs. 3.1 to 3.4 <em>v<sub>s <\/sub><\/em>is the Poisson ratio of the soil, while the corresponding stress components \u0394<em>\u03c3<\/em><sub>z<\/sub>, \u0394<em>\u03c3<\/em><sub>r<\/sub><em>, <\/em>\u0394<em>\u03c3<sub>\u03b8<\/sub><\/em> and \u0394<em>\u03c4<\/em><sub>rz<\/sub> and the vertical <em>z<\/em> and radial <em>r<\/em> distance from the point load are defined in <a href=\"https:\/\/oercollective.caul.edu.au\/app\/uploads\/sites\/143\/2025\/01\/3.5-stresses-point-load.png\">Figure 3.5<\/a>.<\/p>\n","protected":false},"author":1,"menu_order":2,"template":"","meta":{"pb_show_title":"","pb_short_title":"3.2 Stresses in the soil due to a point load","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"class_list":["post-173","chapter","type-chapter","status-publish","hentry"],"part":165,"_links":{"self":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapters\/173","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\/173\/revisions"}],"predecessor-version":[{"id":174,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapters\/173\/revisions\/174"}],"part":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/parts\/165"}],"metadata":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapters\/173\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/wp\/v2\/media?parent=173"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/pressbooks\/v2\/chapter-type?post=173"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/wp\/v2\/contributor?post=173"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/libraryresources.nse.org.ng\/fundamentalsoffoundationengineering\/wp-json\/wp\/v2\/license?post=173"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}