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	<front>
		<journal-meta>
			<journal-id journal-id-type="publisher-id">dyna</journal-id>
			<journal-title-group>
				<journal-title>DYNA</journal-title>
				<abbrev-journal-title abbrev-type="publisher">Dyna rev.fac.nac.minas</abbrev-journal-title>
			</journal-title-group>
			<issn pub-type="epub">2346-2183</issn>
			<issn pub-type="ppub">0012-7353</issn>
			<publisher>
				<publisher-name>Universidad Nacional de Colombia</publisher-name>
			</publisher>
		</journal-meta>
		<article-meta>
			<article-id pub-id-type="doi">10.15446/dyna.v89n223.100030</article-id>
			<article-id pub-id-type="publisher-id">00001</article-id>
			<article-categories>
				<subj-group subj-group-type="heading">
					<subject>Articles</subject>
				</subj-group>
			</article-categories>
			<title-group>
				<article-title>A general model for rectangular footings part II: modeling for design</article-title>
				<trans-title-group xml:lang="es">
					<trans-title>Un modelo general para zapatas rectangulares parte II: modelado para diseño</trans-title>
				</trans-title-group>
			</title-group>
			<contrib-group>
				<contrib contrib-type="author">
					<contrib-id contrib-id-type="orcid">0000-0002-0514-0796</contrib-id>
					<name>
						<surname>Rivera-Mendoza</surname>
						<given-names>José Benito</given-names>
					</name>
					<xref ref-type="aff" rid="aff1"><sup>a</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<contrib-id contrib-id-type="orcid">0000-0002-0198-3614</contrib-id>
					<name>
						<surname>Luévanos-Rojas</surname>
						<given-names>Arnulfo</given-names>
					</name>
					<xref ref-type="aff" rid="aff1b"><sup>a</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<contrib-id contrib-id-type="orcid">0000-0001-8909-1794</contrib-id>
					<name>
						<surname>López-Chavarría</surname>
						<given-names>Sandra</given-names>
					</name>
					<xref ref-type="aff" rid="aff1c"><sup>a</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<contrib-id contrib-id-type="orcid">0000-0002-6113-4964</contrib-id>
					<name>
						<surname>Medina-Elizondo</surname>
						<given-names>Manuel</given-names>
					</name>
					<xref ref-type="aff" rid="aff1d"><sup>a</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<contrib-id contrib-id-type="orcid">0000-0001-8854-0930</contrib-id>
					<name>
						<surname>García-Galván</surname>
						<given-names>Marylú</given-names>
					</name>
					<xref ref-type="aff" rid="aff1e"><sup>a</sup></xref>
				</contrib>
				</contrib-group>
				<aff id="aff1">
					<label>a</label>
					<institution content-type="original"> Instituto de Investigaciones Multidisciplinarias, Universidad Autónoma de Coahuila, Torreón, Coahuila, México. benitoriveramendoza@hotmail.com, arnulfol_2007@hotmail.com, sandylopez5@hotmail.com, drmanuelmedina@yahoo.com.mx, marylugarciagalvan@live.com.mx</institution>
				  <institution content-type="normalized">Universidad Autónoma de Coahuila</institution>
					<institution content-type="orgname">Universidad Autónoma de Coahuila</institution>
					<addr-line>
						<named-content content-type="city">Torreón</named-content>
            <named-content content-type="state">Coahuila</named-content>
					</addr-line>
					<country country="MX">México</country>
					<email>benitoriveramendoza@hotmail.com</email>
				</aff>
				<aff id="aff1b">
					<label>a</label>
					<institution content-type="original"> Instituto de Investigaciones Multidisciplinarias, Universidad Autónoma de Coahuila, Torreón, Coahuila, México. benitoriveramendoza@hotmail.com, arnulfol_2007@hotmail.com, sandylopez5@hotmail.com, drmanuelmedina@yahoo.com.mx, marylugarciagalvan@live.com.mx</institution>
				  <institution content-type="normalized">Universidad Autónoma de Coahuila</institution>
					<institution content-type="orgname">Universidad Autónoma de Coahuila</institution>
					<addr-line>
						<named-content content-type="city">Torreón</named-content>
            <named-content content-type="state">Coahuila</named-content>
					</addr-line>
					<country country="MX">México</country>
					<email>arnulfol_2007@hotmail.com</email>
				</aff>
				<aff id="aff1c">
					<label>a</label>
					<institution content-type="original"> Instituto de Investigaciones Multidisciplinarias, Universidad Autónoma de Coahuila, Torreón, Coahuila, México. benitoriveramendoza@hotmail.com, arnulfol_2007@hotmail.com, sandylopez5@hotmail.com, drmanuelmedina@yahoo.com.mx, marylugarciagalvan@live.com.mx</institution>
				  <institution content-type="normalized">Universidad Autónoma de Coahuila</institution>
					<institution content-type="orgname">Universidad Autónoma de Coahuila</institution>
					<addr-line>
						<named-content content-type="city">Torreón</named-content>
            <named-content content-type="state">Coahuila</named-content>
					</addr-line>
					<country country="MX">México</country>
					<email>sandylopez5@hotmail.com</email>
				</aff>
				<aff id="aff1d">
					<label>a</label>
					<institution content-type="original"> Instituto de Investigaciones Multidisciplinarias, Universidad Autónoma de Coahuila, Torreón, Coahuila, México. benitoriveramendoza@hotmail.com, arnulfol_2007@hotmail.com, sandylopez5@hotmail.com, drmanuelmedina@yahoo.com.mx, marylugarciagalvan@live.com.mx</institution>
				  <institution content-type="normalized">Universidad Autónoma de Coahuila</institution>
					<institution content-type="orgname">Universidad Autónoma de Coahuila</institution>
					<addr-line>
						<named-content content-type="city">Torreón</named-content>
            <named-content content-type="state">Coahuila</named-content>
					</addr-line>
					<country country="MX">México</country>
					<email>drmanuelmedina@yahoo.com.mx</email>
				</aff>
				<aff id="aff1e">
					<label>a</label>
					<institution content-type="original"> Instituto de Investigaciones Multidisciplinarias, Universidad Autónoma de Coahuila, Torreón, Coahuila, México. benitoriveramendoza@hotmail.com, arnulfol_2007@hotmail.com, sandylopez5@hotmail.com, drmanuelmedina@yahoo.com.mx, marylugarciagalvan@live.com.mx</institution>
				  <institution content-type="normalized">Universidad Autónoma de Coahuila</institution>
					<institution content-type="orgname">Universidad Autónoma de Coahuila</institution>
					<addr-line>
						<named-content content-type="city">Torreón</named-content>
            <named-content content-type="state">Coahuila</named-content>
					</addr-line>
					<country country="MX">México</country>
					<email>marylugarciagalvan@live.com.mx</email>
				</aff>
			<!--<pub-date date-type="pub" publication-format="electronic">
				<day>27</day>
				<month>10</month>
				<year>2022</year>
			</pub-date>
			<pub-date date-type="collection" publication-format="electronic">-->
			<pub-date pub-type="epub-ppub">
				<season>Jul-Sep</season>
				<year>2022</year>
			</pub-date>
			<volume>89</volume>
			<issue>223</issue>
			<fpage>9</fpage>
			<lpage>18</lpage>
			<history>
				<date date-type="received">
					<day>10</day>
					<month>12</month>
					<year>2021</year>
				</date>
				<date date-type="rev-recd">
					<day>25</day>
					<month>04</month>
					<year>2022</year>
				</date>
				<date date-type="accepted">
					<day>04</day>
					<month>05</month>
					<year>2022</year>
				</date>
			</history>
			<permissions>
				<license license-type="open-access" xlink:href="https://creativecommons.org/licenses/by-nc-nd/4.0/" xml:lang="en">
					<license-p>This is an open-access article distributed under the terms of the Creative Commons Attribution License</license-p>
				</license>
			</permissions>
			<abstract>
				<title>Abstract</title>
				<p>This paper presents a general model for the design to obtain the thickness and reinforcing steel areas of rectangular footings that support from 1 to “<italic>n</italic>” columns aligned on a longitudinal axis. The pressure diagram is considered linear. Some recently published papers are restricted to certain types of footings as the rectangular isolated footings, and rectangular combined footings that support two columns. The first part of this paper shows the minimum soil area that supports 1 to “<italic>n</italic>” columns aligned on a longitudinal axis. Three numerical examples are presented for design of rectangular footings subjected to an axial load and two orthogonal moments in each column that supports one, two and three columns. The main advantage of this document over other documents is: this model can be applied for one or more columns supported on a rectangular footing (unrestricted on its sides, one side restricted and two opposite sides restricted).</p>
			</abstract>
			<trans-abstract xml:lang="es">
				<title>Resumen</title>
				<p>Este artículo presenta un modelo general de diseño para obtener el espesor y áreas de acero de refuerzo de zapatas rectangulares que soportan de 1 a “<italic>n</italic>” columnas alineadas sobre un eje longitudinal. El diagrama de presión se considera lineal. Algunos documentos publicados recientemente están restringidos a ciertos tipos de zapatas como zapatas rectangulares aisladas, y zapatas rectangulares combinadas que sostienen dos columnas. La primera parte de este artículo muestra el área mínima del suelo que soporta de 1 a “<italic>n</italic>” columnas alineadas en un eje longitudinal. Tres ejemplos numéricos se presentan para el diseño de zapatas rectangulares sometidas a una carga axial y dos momentos ortogonales en cada columna que soporta una, dos y tres columnas. La principal ventaja de este documento sobre otros documentos es: este modelo se puede aplicar para una o más columnas apoyadas en una zapata rectangular (sin restricciones en sus lados, un lado restringido y dos lados opuestos restringidos).</p>
			</trans-abstract>
			<kwd-group xml:lang="en">
				<title>Keywords:</title>
				<kwd>General model for rectangular footings</kwd>
				<kwd>modeling for design</kwd>
				<kwd>rectangular isolated footings</kwd>
				<kwd>rectangular combined footings</kwd>
			</kwd-group>
			<kwd-group xml:lang="es">
				<title>Palabras clave:</title>
				<kwd>Modelo general para zapatas rectangulares</kwd>
				<kwd>modelado para diseño</kwd>
				<kwd>zapatas aisladas rectangulares</kwd>
				<kwd>zapatas combinadas rectangulares</kwd>
			</kwd-group>
			<counts>
				<fig-count count="4"/>
				<table-count count="6"/>
				<equation-count count="20"/>
				<ref-count count="26"/>
				<page-count count="10"/>
			</counts>
		</article-meta>
	</front>
	<body>
		<sec sec-type="intro">
			<title>1. Introduction</title>
			<p>
				<xref ref-type="fig" rid="f1">Fig. 1</xref> shows the distribution of the soil pressure below of the footing, and the distribution of the soil pressure is defined by the type and relative rigidity of the soil, the rigidity of the footing, and the depth of foundation at level of contact between the footing and the soil. <xref ref-type="fig" rid="f1">Fig. 1</xref>(a) presents a concrete rigid footing resting in granular soil (sand or gravel). <xref ref-type="fig" rid="f1">Fig. 1</xref>(b) shows a concrete rigid footing resting on a clay cohesive soil [<xref ref-type="bibr" rid="B1">1</xref>]. Now, to simplify the calculation, the hypothesis has been assumed that the soil is constituted by a bed of independent linear springs in such a way that the stresses that occur in the soil will be proportional to the displacements suffered by the foundation (the area of the real distribution is equal to the area of the uniform distribution).</p>
			<p>
				<fig id="f1">
					<label>Figure 1</label>
					<caption>
						<title>Distribution of the soil pressure below of the footing: (a) Rigid footing in non-cohesive soil (sand or gravel); (b) Rigid footing in clay cohesive soil.</title>
					</caption>
					<graphic xlink:href="2346-2183-dyna-89-223-9-gf1.png"/>
					<attrib>Source: Prepared by the author.</attrib>
				</fig>
			</p>
			<p>The traditional design of footings generally involves a method of successive approximations. This process assumes a uniform distribution of stresses under the foundation, which represents an inadequate approach.</p>
			<p>This work proposes direct equations to determine the effective depth and reinforcing steel areas of rectangular footings with different edge conditions for the calculation of bending moments, bending shear and punching shear for a linear distribution of stresses.</p>
			<p>The works on mathematical models for foundation structures have been investigated successfully in several structural and geotechnical engineering problems. The main scientific contributions of several researchers in recent years are: Guler and Celep [<xref ref-type="bibr" rid="B2">2</xref>] presented the rectangular-shaped plate-column system by means of the Winkler foundation without tension under static and dynamic loads. Chen et al. [<xref ref-type="bibr" rid="B3">3</xref>] studied the hybrid composite plates on elastic foundations under nonlinear vibration. Smith-Pardo [<xref ref-type="bibr" rid="B4">4</xref>] presented a framework that considers the soil-structure interaction through simplified rocking foundation models. Shahin and Cheung [<xref ref-type="bibr" rid="B5">5</xref>] investigated the stochastic design charts for bearing capacity of strip footings. Zhang et al. [<xref ref-type="bibr" rid="B6">6</xref>] developed a nonlinear analysis of a finite beam resting on a Winkler foundation that takes into account the effect of the resistance of the beam on the soil. Agrawal and Hora [<xref ref-type="bibr" rid="B7">7</xref>] proposed the nonlinear interaction of a frame-footings-soil system under seismic loading. Rad [<xref ref-type="bibr" rid="B8">8</xref>] studied the static behavior of 2-D functionally graded circular plate with gradient thickness and elastic foundations for compound loads. Orbanich et al. [<xref ref-type="bibr" rid="B9">9</xref>] estimated the reinforcement and the repair with fiber composite materials for concrete foundation beams. Mohamed et al. [<xref ref-type="bibr" rid="B10">10</xref>] presented the Schmertmann general equation for settlement of shallow footings resting on saturated and unsaturated sands. Orbanich and Ortega [<xref ref-type="bibr" rid="B11">11</xref>] used the finite differences method for elastic foundation plates using internal and perimetric reinforcement beams rested on elastic foundations. Luévanos-Rojas et al. [<xref ref-type="bibr" rid="B12">12</xref>] developed a novel model for the design of rectangular isolated footings. Aristizabal-Ochoa [<xref ref-type="bibr" rid="B13">13</xref>] presented the general conditions for the stability of thin cross section columns rested on an elastic foundation. Barreto-Maya et al. [<xref ref-type="bibr" rid="B14">14</xref>] compared the load capacity between the experiment load tests and the mathematical formulations for deep foundations. Luévanos-Rojas [<xref ref-type="bibr" rid="B15">15</xref>] developed a mathematical model for the design of circular isolated footings. Uncuoğlu [<xref ref-type="bibr" rid="B16">16</xref>] investigated the load capacity for square footings on sand layer overlying clay. Luévanos-Rojas [<xref ref-type="bibr" rid="B17">17</xref>] developed a novel model for the design of boundary trapezoidal combined footings. Camero [<xref ref-type="bibr" rid="B18">18</xref>] presented a novel finite element method for the design of grade industrial floor slabs and pavements applying edge loads. Luévanos-Rojas [<xref ref-type="bibr" rid="B19">19</xref>] developed a mathematical model for the design of boundary rectangular combined footings limited to two opposite sides. Mohebkhah [<xref ref-type="bibr" rid="B20">20</xref>] estimated the load capacity of stone masonry strip footings over a clay trench. López-Chavarría et al. [<xref ref-type="bibr" rid="B21">21</xref>] proposed a novel mathematical model for the design of square isolated footings that takes into account the eccentric load on the footing (general case). Anil et al. [<xref ref-type="bibr" rid="B22">22</xref>] presented an analysis for footings of different shapes supported on sandy soil by the finite element method and experimental tests. Luévanos-Rojas et al. [<xref ref-type="bibr" rid="B23">23</xref>] presented a comparative study for design of trapezoidal and rectangular boundary combined footings using new models. Luévanos-Rojas et al. [<xref ref-type="bibr" rid="B24">24</xref>] proposed a novel mathematical model of design for the T-shaped combined footings. Yáñez-Palafox et al. [<xref ref-type="bibr" rid="B25">25</xref>] developed a modeling for the design of the strap combined footings. </p>
			<p>The paper related to this work is: the design of rectangular combined footings of boundary with two opposite sides restricted that support two columns [<xref ref-type="bibr" rid="B19">19</xref>]. Thus, the review of the literature clearly shows that there is no close relationship with the topic of mathematical model for the design of rectangular footings that support one or more columns aligned on a longitudinal axis that is presented in this paper.</p>
			<p>The first part of this document shows the most economical contact area on the soil (optimal surface) for the rectangular footings that support one or more columns aligned on a longitudinal axis. This paper presents a general model for the design of rectangular footings that support one or more columns aligned on a longitudinal axis. The pressure diagram considered in this document is linear. The recently published papers are restricted for same types of rectangular footings such as the rectangular isolated footings and rectangular combined footings (one paper for a restricted side and it considers that the resultant force is located on the longitudinal axis, and another paper for the two opposite sides restricted). Also, three numerical examples are shown to obtain the design of rectangular footings subject to an axial load and two moments in orthogonal directions in each column. First example is for a rectangular footing that supports a column (rectangular isolated footing). Second example is for a rectangular footing that supports two columns (rectangular combined footing). Third example is for a rectangular footing that supports three columns (rectangular combined footing). </p>
		</sec>
		<sec>
			<title>2. Formulation of the general model</title>
			<p>
				<xref ref-type="fig" rid="f1">Fig. 1</xref> of the part I shows a rectangular footing that supports “<italic>n</italic>” columns aligned on a longitudinal axis (X axis), and each column provides an axial load and two orthogonal bending moments.</p>
			<p>
				<xref ref-type="fig" rid="f2">Fig. 2</xref> of the part I presents the pressure diagram below the rectangular footing, and also the soil pressure in each corner on the footing.</p>
			<p>
				<fig id="f2">
					<label>Figure 2</label>
					<caption>
						<title>Critical sections of the bending moments.</title>
					</caption>
					<graphic xlink:href="2346-2183-dyna-89-223-9-gf2.png"/>
					<attrib>Source: Prepared by the author.</attrib>
				</fig>
			</p>
			<p>Stress anywhere on the footing contact surface due to soil pressure is presented below.</p>
			<p>The stress in the main direction (longitudinal axis) of the X axis is (part I):</p>
			<p>
				<disp-formula id="e1">
					<alternatives>
					<graphic xlink:href="2346-2183-dyna-89-223-9-e1.jpg"/>
				</alternatives>
				</disp-formula>
			</p>
			<p>where: <italic>R</italic> is the sum of all the axial forces, <italic>M</italic>
 <sub>
 <italic>xT</italic>
</sub> is the sum of all the bending moments around the X axis and <italic>M</italic>
 <sub>
 <italic>yT</italic>
</sub> is the sum of all the bending moments around the Y axis, <italic>x</italic> is the distance parallel to the X axis measured from the center of gravity to the point in study, <italic>y</italic> is the distance parallel to the Y axis measured from the center of gravity to the point in study, <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> is the distance in X direction of the footing, <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> is the distance in Y direction of the footing. <italic>R</italic>, <italic>M</italic>
 <sub>
 <italic>xT</italic>
</sub> , <italic>M</italic>
 <sub>
 <italic>yT</italic>
</sub> , are presented in <xref ref-type="disp-formula" rid="e9">eq. (9)</xref>-(<xref ref-type="disp-formula" rid="e11">11</xref>) of the part I. </p>
			<p>The stress in the transverse direction (Y axis) to the main direction (X axis) for any column by the following equation is obtained:</p>
			<p>
				<disp-formula id="e2">
					<alternatives>
					<graphic xlink:href="2346-2183-dyna-89-223-9-e2.jpg"/>
				</alternatives>
				</disp-formula>
			</p>
			<p>where: <italic>x</italic>
 <sub>
 <italic>n</italic>
</sub> and <italic>y</italic>
 <sub>
 <italic>n</italic>
</sub> are the stress coordinates of the column <italic>n</italic>, <italic>P</italic>
 <sub>
 <italic>n</italic>
</sub> is the axial load in the column <italic>n</italic>, <italic>M</italic>
 <sub>
 <italic>xn</italic>
</sub> is the bending moment around the X axis in the column <italic>n</italic>, <italic>M</italic>
 <sub>
 <italic>yn</italic>
</sub> is the bending moment around the Y axis in the column <italic>n</italic>, <italic>w</italic>
 <sub>
 <italic>n</italic>
</sub> is the width of the analysis surface for the column <italic>n</italic> in the main direction (X axis). The width of the analysis surface for the column located closest to the property line is <italic>w</italic>
 <sub>
 <italic>n</italic>
</sub> 
 <italic>= s + c</italic>
 <sub>
 <italic>2n -1</italic>
</sub> 
 <italic>+ d/</italic>2 (If S≥d/2 →<italic>s =d/2, and if s &lt; d/2 → s = s</italic>), and for the columns located in the central part of the footing the width of the analysis surface is <italic>w</italic>
 <sub>
 <italic>n</italic>
</sub> 
 <italic>= c</italic>
 <sub>
 <italic>2n -1</italic> 
</sub> 
 <italic>+ d</italic> (<italic>d</italic> is the effective deep, <italic>s</italic> is the distance from the face of the column to the free end of the footing). The eccentricity <italic>e</italic>
 <sub>
 <italic>xn</italic>
</sub> for the column located in the property line is <italic>e</italic>
 <sub>
 <italic>xn</italic>
</sub> = <italic>w</italic>
 <sub>
 <italic>n</italic>
</sub> 
 <italic>/2 - s - C</italic>
 <sub>
 <italic>2n-1</italic> 
</sub> 
 <italic>/2</italic>, and for the columns located in the central part of the footing the eccentricity is <italic>e</italic>
 <sub>
 <italic>xn</italic>
</sub> = 0.</p>
			<sec>
				<title>2.1. Moments</title>
				<p>
					<xref ref-type="fig" rid="f2">Fig. 2</xref> shows the critical sections for the bending moments according to the code are [<xref ref-type="bibr" rid="B26">26</xref>]: For the axes parallel to the X axis are: <italic>a</italic>
 <sub>1</sub>, <italic>a</italic>
 <sub>2</sub>, <italic>a</italic>
 <sub>3</sub> … <italic>a</italic>
 <sub>n−1</sub>, <italic>a</italic>
 <sub>n</sub>. For the axes parallel to the Y axis are: <italic>b</italic>
 <sub>1</sub>, <italic>b</italic>
 <sub>2</sub>, <italic>b</italic>
 <sub>3</sub> … <italic>b</italic>
 <sub>n−1</sub>, <italic>b</italic>
 <sub>n</sub>, and <italic>d</italic>
 <sub>1</sub>, <italic>d</italic>
 <sub>2</sub>, <italic>d</italic>
 <sub>3</sub> … <italic>d</italic>
 <sub>n−1</sub>, <italic>d</italic>
 <sub>n</sub>.</p>
				<sec>
					<title>2.1.1. Moment around the xn’ - xn’ axis of 0 ≤ yn ≤ Ly/2 </title>
					<p>The shear force <italic>V</italic>
 <sub>
 <italic>yn</italic>
</sub> is obtained by the pressure volume of the surface formed by the <italic>x</italic>
 <sub>
 <italic>n</italic>
</sub> 
 <italic>´ - x</italic>
 <sub>
 <italic>n</italic>
</sub> 
 <italic>´</italic> axis with a width <italic>w</italic>
 <sub>
 <italic>n</italic>
</sub> and the free end (top side of the <xref ref-type="fig" rid="f2">Fig. 2</xref>) of the footing:</p>
					<p>
						<disp-formula id="e3">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e3.JPG"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>Now, the integration of the shear force is the bending moment at any point, the basic equation is presented as follows:</p>
					<p>
						<disp-formula id="e4">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e4.JPG"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>where: <italic>M</italic>
 <sub>
 <italic>xn´</italic>
</sub> is the moment around the <italic>x</italic>
 <sub>
 <italic>n’</italic>
</sub> axis and <italic>V</italic>
 <sub>
 <italic>yn</italic>
</sub> is the shear force at a distance <italic>y</italic>
 <sub>
 <italic>n</italic>
</sub> .</p>
					<p>Integrating <xref ref-type="disp-formula" rid="e4">eq. (4)</xref> the bending moment at any point is obtained:</p>
					<p>
						<disp-formula id="e5">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e5.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>Substituting <italic>y</italic>
 <sub>
 <italic>n</italic>
</sub> 
 <italic>= L</italic>
 <sub>
 <italic>y</italic>
</sub> 
 <italic>/2</italic> and <italic>M</italic>
 <sub>
 <italic>xn´</italic>
</sub> 
 <italic>=</italic> 0 into <xref ref-type="disp-formula" rid="e6">eq. (6)</xref>, the constant <italic>C</italic>
 <sub>
 <italic>1</italic>
</sub> is found:</p>
					<p>
						<disp-formula id="e6">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e6.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>Now, substituting <xref ref-type="disp-formula" rid="e7">eq. (7)</xref> into <xref ref-type="disp-formula" rid="e6">eq. (6)</xref>, the general equation for bending moments is shown as follows:</p>
					<p>
						<disp-formula id="e7">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e7.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>Substituting <italic>y</italic>
 <sub>
 <italic>n</italic>
</sub> 
 <italic>= c</italic>
 <sub>
 <italic>2n</italic>
</sub> 
 <italic>/</italic>2 into <xref ref-type="disp-formula" rid="e7">eq. (8)</xref>, the moment <italic>M</italic>
 <sub>
 <italic>an</italic>
</sub> on the <italic>a</italic>
 <sub>
 <italic>n</italic>
</sub> axis is obtained:</p>
					<p>
						<disp-formula id="e8">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e8.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
				</sec>
				<sec>
					<title>2.1.2. Moment around the y-y axis considered the left part of the footing</title>
					<p>The shear force <italic>V</italic>
 <sub>
 <italic>xk</italic>
</sub> is found by the pressure volume of the surface formed by the <italic>y - y</italic> axis with a width <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> and the free end (left side of the <xref ref-type="fig" rid="f2">Fig. 2</xref>) of the footing:</p>
					<p>
						<disp-formula id="e9">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e9.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>where: the first part of <xref ref-type="disp-formula" rid="e9">eq. (10)</xref> and (11) represents the loads due to the columns and the second part represents the soil pressure.</p>
					<p>Note: The shear forces due to column loads are not considered, when analyzed from the free end of the footing to the first column. </p>
					<p>Now, the integration of the shear force is the bending moment at any point, the basic equation is presented as follows:</p>
					<p>
						<disp-formula id="e10">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e10.JPG"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>where: <italic>M</italic>
 <sub>
 <italic>y</italic>
</sub> is the moment around the <italic>y</italic> axis and <italic>V</italic>
 <sub>
 <italic>xk</italic>
</sub> is the shear force at a distance <italic>x</italic>
 <sub>
 <italic>k</italic>
</sub> .</p>
					<p>Integrating the <xref ref-type="disp-formula" rid="e9">eq. (11)</xref> of the soil pressure and the bending moment at any point from the free end of the footing to the first column is obtained:</p>
					<p>
						<disp-formula id="e11">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e11.JPG"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>Substituting <italic>x</italic>
 <sub>
 <italic>k</italic>
</sub> 
 <italic>= L</italic>
 <sub>
 <italic>x</italic>
</sub> 
 <italic>/2</italic> and <italic>M</italic>
 <sub>
 <italic>y</italic>
</sub> 
 <italic>=</italic> 0 into <xref ref-type="disp-formula" rid="e11">eq. (13)</xref> and the constant <italic>C</italic>
 <sub>
 <italic>2</italic>
</sub> is obtained:</p>
					<p>
						<disp-formula id="e12">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e12.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>Now, substituting <xref ref-type="disp-formula" rid="e12">eq. (14)</xref> into <xref ref-type="disp-formula" rid="e11">eq. (13)</xref>, the general equation for bending moments at any point from the free end of the footing to the first column is shown as follows:</p>
					<p>
						<disp-formula id="e13">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e13.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>Now, the <xref ref-type="disp-formula" rid="e9">eq. (11)</xref> of part I due to the columns loads are considered for the analysis from the column 1 until the last column. The bending moment at a distance “<italic>x</italic>
 <sub>
 <italic>k</italic>
</sub> ” between the columns is:</p>
					<p>
						<disp-formula id="e14">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e14.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>where: M<sub>y1</sub> is bending moment due to the soil pressure, and M<sub>y2</sub> is bending moment due to column loads.</p>
					<p>The <xref ref-type="disp-formula" rid="e13">eq. (15)</xref> and (<xref ref-type="disp-formula" rid="e14">16</xref>) are added to obtain the general equation of the bending moments at any point from the first column until the last column, and equation is represented as follow:</p>
					<p>
						<disp-formula id="e15">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e15.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>Substituting <italic>x</italic>
 <sub>
 <italic>k</italic>
</sub> 
 <italic>= L</italic>
 <sub>
 <italic>x</italic>
</sub> /2 <italic>- L</italic>
 <sub>
 <italic>a</italic>
</sub> 
 <italic>+ c</italic>
 <sub>
 <italic>1</italic>
</sub> /2 into <xref ref-type="disp-formula" rid="e13">eq. (15)</xref>, the bending moment <italic>M</italic>
 <sub>
 <italic>b1</italic>
</sub> on the <italic>b</italic>
 <sub>
 <italic>1</italic>
</sub> axis is obtained:</p>
					<p>
						<disp-formula id="e16">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e16.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>Now, substituting the coordinates in X direction at the junction of the column face with the footing to obtain the bending moments around of the axes <italic>b</italic>
 <sub>2</sub>, <italic>b</italic>
 <sub>3</sub>, … <italic>b</italic>
 <sub>
 <italic>n-1</italic>
</sub> , <italic>b</italic>
 <sub>n</sub>, and <italic>d</italic>
 <sub>1</sub>, <italic>d</italic>
 <sub>2</sub>, <italic>d</italic>
 <sub>3</sub>, … <italic>d</italic>
 <sub>
 <italic>n-1</italic>
</sub> , <italic>d</italic>
 <sub>n</sub>.</p>
				</sec>
			</sec>
			<sec>
				<title><italic>2.2. Bending shear</italic></title>
				<p>Critical sections of the bending shear are presented at a distance d from the junction of the column with the footing, and these sections appear on en, fn and gn axes (see <xref ref-type="fig" rid="f3">Fig. 3</xref>).</p>
				<p>
					<fig id="f3">
						<label>Figure 3</label>
						<caption>
							<title>Critical sections of the bending shear.</title>
						</caption>
						<graphic xlink:href="2346-2183-dyna-89-223-9-gf3.png"/>
						<attrib>Source: Prepared by the author.</attrib>
					</fig>
				</p>
				<sec>
					<title><italic>2.2.1. Bending shear on the x</italic>
 <sub>
 <italic>n</italic>
</sub> 
 <italic>´ - x</italic>
 <sub>
 <italic>n</italic>
</sub> 
 <italic>´ axis</italic></title>
					<p>Substituting <italic>y</italic>
 <sub>
 <italic>n</italic>
</sub> 
 <italic>= c</italic>
 <sub>
 <italic>2n</italic>
</sub> 
 <italic>/2</italic> + <italic>d</italic> into eq. (4), the bending shear <italic>V</italic>
 <sub>
 <italic>en</italic>
</sub> on the <italic>e</italic>
 <sub>
 <italic>n</italic>
</sub> axis of the footing is obtained:</p>
					<p>
						<disp-formula id="e17">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e17.JPG"/>
						</alternatives>
						</disp-formula>
					</p>
				</sec>
				<sec>
					<title><italic>2.2.2. Bending shear on the y - y axis</italic></title>
					<p>Substituting <italic>x</italic>
 <sub>
 <italic>k</italic>
</sub> 
 <italic>= L</italic>
 <sub>
 <italic>x</italic>
</sub> 
 <italic>/2 - L</italic>
 <sub>
 <italic>a</italic>
</sub> 
 <italic>+ c</italic>
 <sub>
 <italic>1</italic>
</sub> 
 <italic>/2</italic> + <italic>d</italic> into the second part of the <xref ref-type="disp-formula" rid="e9">eq. (11)</xref>, the bending shear <italic>V</italic>
 <sub>
 <italic>f1</italic>
</sub> on the <italic>f</italic>
 <sub>
 <italic>1</italic>
</sub> axis of the footing is obtained:</p>
					<p>
						<disp-formula id="e18">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e18.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
					<p>where: the values of <italic>s</italic> are, if S ≥ d → s <italic>= d, and if s &lt; d → s = s.</italic></p>
					<p>Now, substituting the coordinates in X direction at a distance <italic>d</italic> from the junction of the column with the footing into eq. (11) to obtain the bending shear in the axes <italic>f</italic>
 <sub>2</sub>, <italic>f</italic>
 <sub>3</sub>, … <italic>f</italic>
 <sub>
 <italic>n-1</italic>
</sub> , <italic>f</italic>
 <sub>n</sub>, and <italic>g</italic>
 <sub>1</sub>, <italic>g</italic>
 <sub>2</sub>, <italic>g</italic>
 <sub>3</sub>, … <italic>g</italic>
 <sub>
 <italic>n-1</italic>
</sub> , <italic>g</italic>
 <sub>n</sub>.</p>
				</sec>
			</sec>
			<sec>
				<title><italic>2.3. Punching shear</italic></title>
				<p>Critical section for the punching shear appears at a distance <italic>d/2</italic> from the junction of the column with the footing in the two directions (see <xref ref-type="fig" rid="f4">Fig. 4</xref>).</p>
				<p>
					<fig id="f4">
						<label>Figure 4</label>
						<caption>
							<title>Critical sections of the punching shear.</title>
						</caption>
						<graphic xlink:href="2346-2183-dyna-89-223-9-gf4.png"/>
						<attrib>Source: Prepared by the author.</attrib>
					</fig>
				</p>
				<sec>
					<title><italic>2.3.1. Punching shear for theFGT boundary column</italic></title>
					<p>Critical section for the punching shear is presented in the rectangular section formed by the dotted surface of the boundary column. Punching shear acting on the footing <italic>V</italic>
 <sub>
 <italic>p1</italic>
</sub> is the force <italic>P</italic>
 <sub>
 <italic>1</italic>
</sub> acting on column 1 subtracting the pressure volume of the surface formed by the dotted surface of the boundary column:</p>
					<p>
						<disp-formula id="e19">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e19.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
				</sec>
				<sec>
					<title><italic>2.3.2. Punching shear for the inner column</italic></title>
					<p>Critical section for the punching shear is presented in the rectangular section formed by the dotted surface of the inner column. Punching shear acting on the footing <italic>V</italic>
 <sub>
 <italic>pn</italic>
</sub> is the force <italic>P</italic>
 <sub>
 <italic>n</italic>
</sub> acting on column <italic>n</italic> subtracting the pressure volume of the surface formed by the dotted surface of the inner column:</p>
					<p>
						<disp-formula id="e20">
							<alternatives>
							<graphic xlink:href="2346-2183-dyna-89-223-9-e20.jpg"/>
						</alternatives>
						</disp-formula>
					</p>
				</sec>
			</sec>
		</sec>
		<sec>
			<title>3. Numerical problems</title>
			<p>Three numerical examples are presented below: Example 1 is for a rectangular footing that supports a column. Example 2 is for a rectangular footing that supports two columns. Example 3 is for a rectangular footing that supports three columns.</p>
			<p>The thickness for the three examples is determined as follows: First, a minimum thickness is proposed according to the code of 25 cm [<xref ref-type="bibr" rid="B26">26</xref>], and then the thickness is revised to meet with the following conditions: bending moments, bending shear, and punching shear.</p>
			<sec>
				<title>3.1. Example 1</title>
				<p>The design of a rectangular footing (rectangular isolated footing) that supports a square column with the following information are presented: the column is of 40x40 <italic>cm</italic>; <italic>H =</italic> 2.0 <italic>m</italic>; <italic>P</italic>
 <sub>
 <italic>D1</italic>
</sub> 
 <italic>=</italic> 600 <italic>kN</italic>; <italic>P</italic>
 <sub>
 <italic>L1</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>Dx1</italic>
</sub> 
 <italic>=</italic> 200 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Lx1</italic>
</sub> 
 <italic>=</italic> 100 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Dy1</italic>
</sub> 
 <italic>=</italic> 100 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Ly1</italic>
</sub> 
 <italic>=</italic> 50 <italic>kN-m</italic>; <italic>f’</italic>
 <sub>
 <italic>c</italic>
</sub> 
 <italic>=</italic> 35 <italic>MPa</italic>; <italic>f</italic>
 <sub>
 <italic>y</italic>
</sub> 
 <italic>=</italic> 420 <italic>MPa</italic>; <italic>q</italic>
 <sub>
 <italic>a</italic>
</sub> 
 <italic>=</italic> 250 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> ; <italic>γ</italic>
 <sub>
 <italic>ppz</italic>
</sub> 
 <italic>=</italic> 24 <italic>kN/m</italic>
 <sup>
 <italic>3</italic>
</sup> ; <italic>γ</italic>
 <sub>
 <italic>pps</italic>
</sub> 
 <italic>=</italic> 15 <italic>kN/m</italic>
 <sup>
 <italic>3</italic>
</sup> . Where: <italic>H</italic> is the depth of the footing, <italic>P</italic>
 <sub>
 <italic>D1</italic>
</sub> is the dead load, <italic>P</italic>
 <sub>
 <italic>L1</italic>
</sub> is the live load, <italic>M</italic>
 <sub>
 <italic>Dx1</italic>
</sub> is the moment around the X axis of the dead load, <italic>M</italic>
 <sub>
 <italic>Lx1</italic>
</sub> is the moment around the X axis of the live load, <italic>M</italic>
 <sub>
 <italic>Dy1</italic>
</sub> is the moment around the Y axis of the dead load, <italic>M</italic>
 <sub>
 <italic>Ly1</italic>
</sub> is the moment around the Y axis of the live load.</p>
				<p>The load and moments that act on soil are: <italic>P</italic>
 <sub>
 <italic>1</italic>
</sub> 
 <italic>=</italic> 900 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>x1</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>y1</italic>
</sub> 
 <italic>=</italic> 150 <italic>kN-m</italic>.</p>
				<p>The thickness that meets the bending moments, bending shear, and punching shear is of 45 <italic>cm</italic>.</p>
				<p>Substituting the values of <italic>σ</italic>
 <sub>
 <italic>p</italic>
</sub> = 215.95 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>P</italic>
 <sub>
 <italic>1</italic>
</sub> 
 <italic>=</italic> 900 <italic>kN</italic>, <italic>M</italic>
 <sub>
 <italic>x1</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN-m</italic>, <italic>M</italic>
 <sub>
 <italic>y1</italic>
</sub> 
 <italic>=</italic> 150 <italic>kN-m</italic>, <italic>L</italic>
 <sub>
 <italic>a</italic>
</sub> = <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> /2 into eq. (15)-(23) of part I and using the MAPLE-15 software are obtained: <italic>S</italic>
 <sub>
 <italic>tmin</italic>
</sub> = 8.27 <italic>m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> = 2.03 <italic>m</italic>, <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> = 4.07 <italic>m</italic>, <italic>σ</italic>
 <sub>
 <italic>1</italic>
</sub> = 215.95 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>2</italic>
</sub> = 108.86 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>3</italic>
</sub> = 108.86 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>4</italic>
</sub> = 1.77 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> 
 <italic>.</italic></p>
				<p>Now the practical dimensions of the rectangular footing that supports a square column are: <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> 
 <italic>=</italic> 2.05 <italic>m, L</italic>
 <sub>
 <italic>y</italic>
</sub> 
 <italic>=</italic> 4.10 <italic>m</italic>. </p>
				<p>Substituting the values of <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> 
 <italic>=</italic> 2.05 <italic>m, L</italic>
 <sub>
 <italic>y</italic>
</sub> 
 <italic>=</italic> 4.10 <italic>m</italic> in the same MAPLE-15 software are obtained: <italic>S</italic>
 <sub>
 <italic>tmin</italic>
</sub> = 8.40 <italic>m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> = 2.05 <italic>m</italic>, <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> = 4.10 <italic>m</italic>, <italic>σ</italic>
 <sub>
 <italic>1</italic>
</sub> = 211.55 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>2</italic>
</sub> = 107.08 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>3</italic>
</sub> = 107.08 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>4</italic>
</sub> = 2.61 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> 
 <italic>.</italic></p>
				<p>The load and the bending moments around of the X and Y axes (factored mechanical elements) are [<xref ref-type="bibr" rid="B26">26</xref>]: <italic>P</italic>
 <sub>
 <italic>u1</italic>
</sub> 
 <italic>=</italic> 1200 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>ux1</italic>
</sub> 
 <italic>=</italic> 400 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>uy1</italic>
</sub> 
 <italic>=</italic> 200 <italic>kN-m</italic>.</p>
			</sec>
			<sec>
				<title>3.2. Example 2</title>
				<p>The design of a rectangular footing (rectangular combined footing) that supports two square columns with the following information are presented: the columns are of 40x40 <italic>cm</italic>; <italic>H =</italic> 2.0 <italic>m</italic>; <italic>L</italic>
 <sub>1</sub>
 <italic>=</italic> 6.00 <italic>m</italic>; <italic>P</italic>
 <sub>
 <italic>D1</italic>
</sub> 
 <italic>=</italic> 600 <italic>kN</italic>; <italic>P</italic>
 <sub>
 <italic>L1</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>Dx1</italic>
</sub> 
 <italic>=</italic> 200 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Lx1</italic>
</sub> 
 <italic>=</italic> 100 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Dy1</italic>
</sub> 
 <italic>=</italic> 100 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Ly1</italic>
</sub> 
 <italic>=</italic> 50 <italic>kN-m</italic>; <italic>P</italic>
 <sub>
 <italic>D2</italic>
</sub> 
 <italic>=</italic> 1200 <italic>kN</italic>; <italic>P</italic>
 <sub>
 <italic>L2</italic>
</sub> 
 <italic>=</italic> 600 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>Dx2</italic>
</sub> 
 <italic>=</italic> 400 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Lx2</italic>
</sub> 
 <italic>=</italic> 200 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Dy2</italic>
</sub> 
 <italic>=</italic> 200 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Ly2</italic>
</sub> 
 <italic>=</italic> 100 <italic>kN-m</italic>; <italic>f’</italic>
 <sub>
 <italic>c</italic>
</sub> 
 <italic>=</italic> 35 <italic>MPa</italic>; <italic>f</italic>
 <sub>
 <italic>y</italic>
</sub> 
 <italic>=</italic> 420 <italic>MPa</italic>; <italic>q</italic>
 <sub>
 <italic>a</italic>
</sub> 
 <italic>=</italic> 250 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> ; <italic>γ</italic>
 <sub>
 <italic>ppz</italic>
</sub> 
 <italic>=</italic> 24 <italic>kN/m</italic>
 <sup>
 <italic>3</italic>
</sup> ; <italic>γ</italic>
 <sub>
 <italic>pps</italic>
</sub> 
 <italic>=</italic> 15 <italic>kN/m</italic>
 <sup>
 <italic>3</italic>
</sup> .</p>
				<p>The loads and moments that act on soil are: <italic>P</italic>
 <sub>
 <italic>1</italic>
</sub> 
 <italic>=</italic> 900 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>x1</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>y1</italic>
</sub> 
 <italic>=</italic> 150 <italic>kN-m</italic>; <italic>P</italic>
 <sub>
 <italic>2</italic>
</sub> 
 <italic>=</italic> 1800 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>x2</italic>
</sub> 
 <italic>=</italic> 600 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>y2</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN-m</italic>.</p>
				<p>The thickness that meets the bending moments, bending shear, and punching shear is of 80 cm.</p>
				<p>Substituting the values of <italic>σ</italic>
 <sub>
 <italic>p</italic>
</sub> = 212.80 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>P</italic>
 <sub>
 <italic>1</italic>
</sub> 
 <italic>=</italic> 900 <italic>kN</italic>, <italic>M</italic>
 <sub>
 <italic>x1</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN-m</italic>, <italic>M</italic>
 <sub>
 <italic>y1</italic>
</sub> 
 <italic>=</italic> 150 <italic>kN-m</italic>, <italic>P</italic>
 <sub>
 <italic>2</italic>
</sub> 
 <italic>=</italic> 1800 <italic>kN</italic>, <italic>M</italic>
 <sub>
 <italic>x2</italic>
</sub> 
 <italic>=</italic> 600 <italic>kN-m</italic>, <italic>M</italic>
 <sub>
 <italic>y2</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN-m</italic> into eq. (15)-(23) of part I and using the MAPLE-15 software are obtained: <italic>S</italic>
 <sub>
 <italic>tmin</italic>
</sub> = 21.99 <italic>m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>L</italic>
 <sub>
 <italic>a</italic>
</sub> 
 <italic>=</italic> 0.20 <italic>m, L</italic>
 <sub>
 <italic>x</italic>
</sub> = 8.07 <italic>m</italic>, <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> = 2.73 <italic>m</italic>, <italic>M</italic>
 <sub>
 <italic>xT</italic>
</sub> = 900.00 <italic>kN-m</italic>, <italic>M</italic>
 <sub>
 <italic>yT</italic>
</sub> = 0.00 <italic>kN-m</italic>, <italic>R</italic> = 2700 <italic>kN</italic>, <italic>σ</italic>
 <sub>
 <italic>1</italic>
</sub> = 212.80 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>2</italic>
</sub> = 212.80 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>3</italic>
</sub> = 32.71 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>4</italic>
</sub> = 32.71 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> 
 <italic>.</italic></p>
				<p>Now the practical dimensions of the rectangular footing that supports two square columns are: <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> 
 <italic>=</italic> 8.10 <italic>m, L</italic>
 <sub>
 <italic>y</italic>
</sub> 
 <italic>=</italic> 2.75 <italic>m</italic>. </p>
				<p>Substituting the values of <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> 
 <italic>=</italic> 8.10 <italic>m, L</italic>
 <sub>
 <italic>y</italic>
</sub> 
 <italic>=</italic> 2.75 <italic>m</italic> in the same MAPLE-15 software are obtained: <italic>S</italic>
 <sub>
 <italic>tmin</italic>
</sub> = 22.27 <italic>m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>L</italic>
 <sub>
 <italic>a</italic>
</sub> 
 <italic>=</italic> 0.22 <italic>m, L</italic>
 <sub>
 <italic>x</italic>
</sub> = 8.10 <italic>m</italic>, <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> = 2.75 <italic>m</italic>, <italic>M</italic>
 <sub>
 <italic>xT</italic>
</sub> = 900.00 <italic>kN-m</italic>, <italic>M</italic>
 <sub>
 <italic>yT</italic>
</sub> = 1.00 <italic>kN-m</italic>, <italic>R</italic> = 2700 <italic>kN</italic>, <italic>σ</italic>
 <sub>
 <italic>1</italic>
</sub> = 209.40 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>2</italic>
</sub> = 209.33 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>3</italic>
</sub> = 33.09 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>4</italic>
</sub> = 33.02 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> 
 <italic>.</italic></p>
				<p>The loads and the bending moments around of the X and Y axes (factored mechanical elements) are [26]: <italic>P</italic>
 <sub>
 <italic>u1</italic>
</sub> 
 <italic>=</italic> 1200 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>ux1</italic>
</sub> 
 <italic>=</italic> 400 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>uy1</italic>
</sub> 
 <italic>=</italic> 200 <italic>kN-m</italic>, <italic>P</italic>
 <sub>
 <italic>u2</italic>
</sub> 
 <italic>=</italic> 2400 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>ux2</italic>
</sub> 
 <italic>=</italic> 800 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>uy2</italic>
</sub> 
 <italic>=</italic> 400 <italic>kN-m</italic>.</p>
				<p>The factored resultant loads and the factored resultant bending moments by Eqs. (16) to (18) of part I are obtained: <italic>R</italic>
 <sub>
 <italic>u</italic>
</sub> 
 <italic>=</italic> 3600 <italic>kN</italic>, <italic>M</italic>
 <sub>
 <italic>uxT</italic>
</sub> 
 <italic>=</italic> 1200 <italic>kN-m</italic>, <italic>M</italic>
 <sub>
 <italic>uyT</italic>
</sub> 
 <italic>=</italic> 60 <italic>kN-m</italic>.</p>
			</sec>
			<sec>
				<title>3.3. Example 3</title>
				<p>The design of a rectangular footing (rectangular combined footing) that supports three square columns with the following information are presented: the columns are of 40x40 <italic>cm</italic>; <italic>H =</italic> 2.0 <italic>m</italic>; <italic>L</italic>
 <sub>1</sub>
 <italic>=</italic> 6.00 <italic>m</italic>; <italic>P</italic>
 <sub>
 <italic>D1</italic>
</sub> 
 <italic>=</italic> 600 <italic>kN</italic>; <italic>P</italic>
 <sub>
 <italic>L1</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>Dx1</italic>
</sub> 
 <italic>=</italic> 200 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Lx1</italic>
</sub> 
 <italic>=</italic> 100 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Dy1</italic>
</sub> 
 <italic>=</italic> 100 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Ly1</italic>
</sub> 
 <italic>=</italic> 50 <italic>kN-m</italic>; <italic>P</italic>
 <sub>
 <italic>D2</italic>
</sub> 
 <italic>=</italic> 1200 <italic>kN</italic>; <italic>P</italic>
 <sub>
 <italic>L2</italic>
</sub> 
 <italic>=</italic> 600 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>Dx2</italic>
</sub> 
 <italic>=</italic> 400 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Lx2</italic>
</sub> 
 <italic>=</italic> 200 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Dy2</italic>
</sub> 
 <italic>=</italic> 200 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Ly2</italic>
</sub> 
 <italic>=</italic> 100 <italic>kN-m</italic>; <italic>P</italic>
 <sub>
 <italic>D3</italic>
</sub> 
 <italic>=</italic> 1200 <italic>kN</italic>; <italic>P</italic>
 <sub>
 <italic>L3</italic>
</sub> 
 <italic>=</italic> 600 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>Dx3</italic>
</sub> 
 <italic>=</italic> 400 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Lx3</italic>
</sub> 
 <italic>=</italic> 200 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Dy3</italic>
</sub> 
 <italic>=</italic> 200 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>Ly3</italic>
</sub> 
 <italic>=</italic> 100 <italic>kN-m</italic>; <italic>f’</italic>
 <sub>
 <italic>c</italic>
</sub> 
 <italic>=</italic> 35 <italic>MPa</italic>; <italic>f</italic>
 <sub>
 <italic>y</italic>
</sub> 
 <italic>=</italic> 420 <italic>MPa</italic>; <italic>q</italic>
 <sub>
 <italic>a</italic>
</sub> 
 <italic>=</italic> 250 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> ; <italic>γ</italic>
 <sub>
 <italic>ppz</italic>
</sub> 
 <italic>=</italic> 24 <italic>kN/m</italic>
 <sup>
 <italic>3</italic>
</sup> ; <italic>γ</italic>
 <sub>
 <italic>pps</italic>
</sub> 
 <italic>=</italic> 15 <italic>kN/m</italic>
 <sup>
 <italic>3</italic>
</sup> .</p>
				<p>The loads and moments that act on soil are: <italic>P</italic>
 <sub>
 <italic>1</italic>
</sub> 
 <italic>=</italic> 900 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>x1</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>y1</italic>
</sub> 
 <italic>=</italic> 150 <italic>kN-m</italic>; <italic>P</italic>
 <sub>
 <italic>2</italic>
</sub> 
 <italic>=</italic> 1800 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>x2</italic>
</sub> 
 <italic>=</italic> 600 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>y2</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN-m</italic>; <italic>P</italic>
 <sub>
 <italic>3</italic>
</sub> 
 <italic>=</italic> 1800 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>x3</italic>
</sub> 
 <italic>=</italic> 600 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>y3</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN-m</italic>.</p>
				<p>The thickness that meets the bending moments, bending shear, and punching shear is of 80 cm.</p>
				<p>Substituting the values of <italic>σ</italic>
 <sub>
 <italic>p</italic>
</sub> = 212.80 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>P</italic>
 <sub>
 <italic>1</italic>
</sub> 
 <italic>=</italic> 900 <italic>kN</italic>, <italic>M</italic>
 <sub>
 <italic>x1</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN-m</italic>, <italic>M</italic>
 <sub>
 <italic>y1</italic>
</sub> 
 <italic>=</italic> 150 <italic>kN-m</italic>, <italic>P</italic>
 <sub>
 <italic>2</italic>
</sub> 
 <italic>=</italic> 1800 <italic>kN</italic>, <italic>M</italic>
 <sub>
 <italic>x2</italic>
</sub> 
 <italic>=</italic> 600 <italic>kN-m</italic>, <italic>M</italic>
 <sub>
 <italic>y2</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN-m</italic>, <italic>P</italic>
 <sub>
 <italic>3</italic>
</sub> 
 <italic>=</italic> 1800 <italic>kN</italic>, <italic>M</italic>
 <sub>
 <italic>x3</italic>
</sub> 
 <italic>=</italic> 600 <italic>kN-m</italic>, <italic>M</italic>
 <sub>
 <italic>y3</italic>
</sub> 
 <italic>=</italic> 300 <italic>kN-m</italic> into eq. (15)-(23) of part I and using the MAPLE-15 software are obtained: <italic>S</italic>
 <sub>
 <italic>tmin</italic>
</sub> = 37.47 <italic>m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>L</italic>
 <sub>
 <italic>a</italic>
</sub> 
 <italic>=</italic> 0.20 <italic>m, L</italic>
 <sub>
 <italic>x</italic>
</sub> = 14.47 <italic>m</italic>, <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> = 2.59 <italic>m</italic>, <italic>M</italic>
 <sub>
 <italic>xT</italic>
</sub> = 1500.00 <italic>kN-m</italic>, <italic>M</italic>
 <sub>
 <italic>yT</italic>
</sub> = 0.00 <italic>kN-m</italic>, <italic>R</italic> = 4500 <italic>kN</italic>, <italic>σ</italic>
 <sub>
 <italic>1</italic>
</sub> = 212.80 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>2</italic>
</sub> = 212.80 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>3</italic>
</sub> = 27.37 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>4</italic>
</sub> = 27.37 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> 
 <italic>.</italic></p>
				<p>Now the practical dimensions of the rectangular footing that supports two square columns are: <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> 
 <italic>=</italic> 14.50 <italic>m, L</italic>
 <sub>
 <italic>y</italic>
</sub> 
 <italic>=</italic> 2.60 <italic>m</italic>. </p>
				<p>Substituting the values of <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> 
 <italic>=</italic> 14.50 <italic>m, L</italic>
 <sub>
 <italic>y</italic>
</sub> 
 <italic>=</italic> 2.60 <italic>m</italic> in the same MAPLE-15 software are obtained: <italic>S</italic>
 <sub>
 <italic>tmin</italic>
</sub> = 37.70 <italic>m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>L</italic>
 <sub>
 <italic>a</italic>
</sub> 
 <italic>=</italic> 0.22 <italic>m, L</italic>
 <sub>
 <italic>x</italic>
</sub> = 14.50 <italic>m</italic>, <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> = 2.60 <italic>m</italic>, <italic>M</italic>
 <sub>
 <italic>xT</italic>
</sub> = 1500.00 <italic>kN-m</italic>, <italic>M</italic>
 <sub>
 <italic>yT</italic>
</sub> = 1.00 <italic>kN-m</italic>, <italic>R</italic> = 4500 <italic>kN</italic>, <italic>σ</italic>
 <sub>
 <italic>1</italic>
</sub> = 211.19 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>2</italic>
</sub> = 211.17 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>3</italic>
</sub> = 27.56 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> , <italic>σ</italic>
 <sub>
 <italic>4</italic>
</sub> = 27.53 <italic>kN/m</italic>
 <sup>
 <italic>2</italic>
</sup> 
 <italic>.</italic></p>
				<p>The loads and the bending moments around of the X and Y axes (factored mechanical elements) are [<xref ref-type="bibr" rid="B26">26</xref>]: <italic>P</italic>
 <sub>
 <italic>u1</italic>
</sub> 
 <italic>=</italic> 1200 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>ux1</italic>
</sub> 
 <italic>=</italic> 400 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>uy1</italic>
</sub> 
 <italic>=</italic> 200 <italic>kN-m</italic>, <italic>P</italic>
 <sub>
 <italic>u2</italic>
</sub> 
 <italic>=</italic> 2400 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>ux2</italic>
</sub> 
 <italic>=</italic> 800 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>uy2</italic>
</sub> 
 <italic>=</italic> 400 <italic>kN-m</italic>, <italic>P</italic>
 <sub>
 <italic>u3</italic>
</sub> 
 <italic>=</italic> 2400 <italic>kN</italic>; <italic>M</italic>
 <sub>
 <italic>ux3</italic>
</sub> 
 <italic>=</italic> 800 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>uy3</italic>
</sub> 
 <italic>=</italic> 400 <italic>kN-m</italic>.</p>
				<p>The factored resultant loads and the factored resultant bending moments by <xref ref-type="disp-formula" rid="e16">Eqs. (16)</xref> to (<xref ref-type="disp-formula" rid="e16">18</xref>) of part I are obtained: <italic>R</italic>
 <sub>
 <italic>u</italic>
</sub> 
 <italic>=</italic> 6000 <italic>kN</italic>, <italic>M</italic>
 <sub>
 <italic>uxT</italic>
</sub> 
 <italic>=</italic> 2000 <italic>kN-m</italic>, <italic>M</italic>
 <sub>
 <italic>uyT = -</italic> 
</sub> 100 <italic>kN-m</italic>.</p>
			</sec>
		</sec>
		<sec sec-type="results">
			<title>4. Results</title>
			<p>One way to verify the model proposed in this document is: </p>
			<p>Substituting <italic>y</italic>
 <sub>
 <italic>n</italic>
</sub> = <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> /2 into <xref ref-type="disp-formula" rid="e8">eq. (8)</xref>, and the moment around the x<sub>n</sub>´-x<sub>n</sub>´ axis is <italic>M</italic>
 <sub>
 <italic>xn´</italic>
</sub> = 0. </p>
			<p>Now, substituting <italic>x</italic>
 <sub>
 <italic>k</italic>
</sub> = <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> /2 into <xref ref-type="disp-formula" rid="e12">eq. (15)</xref>, and the moment around the y<sub>1</sub>-y<sub>1</sub> axis is <italic>M</italic>
 <sub>
 <italic>y1</italic>
</sub> = 0. </p>
			<p>Substituting <italic>x</italic>
 <sub>
 <italic>k</italic>
</sub> = <italic>- L</italic>
 <sub>
 <italic>x</italic>
</sub> /2 into <xref ref-type="disp-formula" rid="e17">eq. (17)</xref> and the moment around the y-y axis is <italic>M</italic>
 <sub>
 <italic>y</italic>
</sub> = 0. </p>
			<p>Now, substituting <italic>y</italic>
 <sub>
 <italic>n</italic>
</sub> = <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> /2 into <xref ref-type="disp-formula" rid="e4">eq. (4)</xref> and the shear force on the x<sub>n</sub>´-x<sub>n</sub>´ axis is <italic>V</italic>
 <sub>
 <italic>yn</italic>
</sub> = 0.</p>
			<p>Substituting <italic>x</italic>
 <sub>
 <italic>k</italic>
</sub> = <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> /2 into <xref ref-type="disp-formula" rid="e9">eq. (11)</xref> considering only the second part that represents the soil pressure, and the shear force on the y<sub>1</sub>-y<sub>1</sub> axis is <italic>V</italic>
 <sub>
 <italic>xk</italic>
</sub> = 0.</p>
			<p>Now, substituting <italic>x</italic>
 <sub>
 <italic>k</italic>
</sub> = <italic>- L</italic>
 <sub>
 <italic>x</italic>
</sub> /2 into <xref ref-type="disp-formula" rid="e9">eq. (11)</xref>, and the shear force on the y-y axis is <italic>V</italic>
 <sub>
 <italic>xk</italic>
</sub> = 0.</p>
			<p>Therefore the equations for the bending moments and the shear forces are verified by equilibrium.</p>
			<sec>
				<title>4.1. Example 1</title>
				<p>Substituting the corresponding values into <xref ref-type="disp-formula" rid="e9">eq. (9)</xref>-(<xref ref-type="disp-formula" rid="e9">15</xref>) to obtain the bending moments that act on the critical sections of the rectangular isolated footing are shown below: <italic>M</italic>
 <sub>
 <italic>a1</italic>
</sub> = 671.68 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>b1</italic>
</sub> = 270.31 <italic>kN-m</italic>. </p>
				<p>After making different proposals, the effective depth is <italic>d</italic> = 37.00 <italic>cm</italic>, <italic>r</italic> = 8.00 <italic>cm</italic>, <italic>t</italic> = 45.00 <italic>cm</italic>.</p>
				<p>Substituting the corresponding values into <xref ref-type="disp-formula" rid="e9">eq. (19)</xref>-(<xref ref-type="disp-formula" rid="e18">20</xref>) to obtain the bending shear forces that act on the critical sections of the rectangular isolated footing are shown below: <italic>V</italic>
 <sub>
 <italic>e1 = -</italic> 
</sub> 568.20 <italic>kN</italic>; <italic>V</italic>
 <sub>
 <italic>f1 = - 367.43</italic>
</sub> 
 <italic>kN</italic>. Now, the allowable bending shear forces by the concrete are: <italic>∅</italic>
 <sub>
 <italic>v</italic>
</sub> 
 <italic>V</italic>
 <sub>
 <italic>ce1</italic>
</sub> = 648.42 <italic>kN</italic>; <italic>∅</italic>
 <sub>
 <italic>v</italic>
</sub> 
 <italic>V</italic>
 <sub>
 <italic>cf1</italic>
</sub> = 1296.84 <italic>kN</italic>. Then, the two bending shear forces satisfy with the code [<xref ref-type="bibr" rid="B26">26</xref>].</p>
				<p>Now, substituting the corresponding values into <xref ref-type="disp-formula" rid="e19">eq. (22)</xref> to obtain the punching shear force that acts on the critical section of the rectangular isolated footing is shown below: <italic>V</italic>
 <sub>
 <italic>p1</italic>
</sub> = 1115.35 <italic>kN</italic>. Now, the allowable punching shear forces by the concrete are: <italic>∅</italic>
 <sub>
 <italic>v</italic>
</sub> 
 <italic>V</italic>
 <sub>
 <italic>cp1</italic>
</sub> = 2922.64 <italic>kN</italic>, <italic>∅</italic>
 <sub>
 <italic>v</italic>
</sub> 
 <italic>V</italic>
 <sub>
 <italic>cp1</italic>
</sub> = 3236.86 <italic>kN</italic>, <italic>∅</italic>
 <sub>
 <italic>v</italic>
</sub> 
 <italic>V</italic>
 <sub>
 <italic>cp1</italic>
</sub> = 1891.12 <italic>kN</italic>. Then, the punching shear force satisfies with the code [<xref ref-type="bibr" rid="B26">26</xref>]. </p>
				<p>The reinforcement steel areas for the rectangular isolated footing that result of the bending moments are shown below: <italic>A</italic>
 <sub>
 <italic>sy</italic>
</sub> = 50.39 <italic>cm</italic>
 <sup>2</sup>; <italic>A</italic>
 <sub>
 <italic>sx</italic>
</sub> = 19.50 <italic>cm</italic>
 <sup>2</sup>, and the minimum steel areas according to the code are [<xref ref-type="bibr" rid="B26">26</xref>]: <italic>A</italic>
 <sub>
 <italic>symin</italic>
</sub> = 25.28 <italic>cm</italic>
 <sup>2</sup>; <italic>A</italic>
 <sub>
 <italic>sxmin</italic>
</sub> = 50.57 <italic>cm</italic>
 <sup>2</sup>. Hence, the reinforcement steel areas for the design of the rectangular isolated footing are: <italic>A</italic>
 <sub>
 <italic>sy</italic>
</sub> = 50.39 <italic>cm</italic>
 <sup>2</sup>; <italic>A</italic>
 <sub>
 <italic>sx</italic>
</sub> = 50.57 <italic>cm</italic>
 <sup>2</sup>. The proposed steel areas are: <italic>A</italic>
 <sub>
 <italic>sy</italic>
</sub> = 50.70 <italic>cm</italic>
 <sup>2</sup> (10Ø1”) spaced at 20.56 <italic>cm</italic>; <italic>A</italic>
 <sub>
 <italic>sx</italic>
</sub> = 50.70 <italic>cm</italic>
 <sup>2</sup> (10Ø1”) spaced at 43.33 <italic>cm</italic>.</p>
			</sec>
			<sec>
				<title>4.2. Example 2</title>
				<p>Substituting the corresponding values into <xref ref-type="disp-formula" rid="e8">eq. (9)</xref>, (<xref ref-type="disp-formula" rid="e13">15</xref>) and (<xref ref-type="disp-formula" rid="e15">17</xref>) to obtain the bending moments that act on the critical sections of the rectangular combined footing are shown below: <italic>M</italic>
 <sub>
 <italic>a1</italic>
</sub> = 457.908 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>a2</italic>
</sub> = 915.80 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>b1</italic>
</sub> = 0.09 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>d1=</italic> 
</sub> - 400.33<italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>b2</italic>
</sub> = 943.58 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>d2</italic>
</sub> = 692.53 <italic>kN-m</italic>; <italic>M</italic>
 <sub>
 <italic>max12</italic> 
</sub> 
 <italic>= - 1540.55kN-m</italic> (maximum bending moment between the column 1 and column 2) in <italic>x</italic>
 <sub>
 <italic>max12</italic>
</sub> = 1.37 <italic>m</italic> (position of the maximum bending moment between the column 1 and column 2).</p>
				<p>The maximum bending moment between the column 1 and column 2 is obtained as follows: First, the position of the maximum bending moment is located from the equation of the shear forces, i.e., when the shear force is zero, the maximum moment is obtained. </p>
				<p>After making different proposals, the effective depth is <italic>d</italic> = 72.00 <italic>cm</italic>, <italic>r</italic> = 8.00 <italic>cm</italic>, <italic>t</italic> = 80.00 <italic>cm</italic>.</p>
				<p>The bending shear forces that act on the critical sections of the rectangular combined footing by <xref ref-type="disp-formula" rid="e17">eq. (19)</xref>-(<xref ref-type="disp-formula" rid="e9">11</xref>), and the allowable bending shear forces for the concrete by the code are obtained [<xref ref-type="bibr" rid="B26">26</xref>] (see <xref ref-type="table" rid="t1">Table 1</xref>). </p>
				<p>
					<table-wrap id="t1">
						<label>Table 1</label>
						<caption>
							<title>Bending shear forces of the example 2. </title>
						</caption>
						<table frame="hsides" rules="groups">
							<colgroup>
								<col/>
								<col/>
								<col/>
								<col/>
							</colgroup>
							<thead>
								<tr>
									<th align="center">Axis</th>
									<th align="center">Shear force that acts (kN)</th>
									<th align="center">Allowable shear force (kN)</th>
									<th align="center">Width of analysis (m)</th>
								</tr>
							</thead>
							<tbody>
								<tr>
									<td align="center"><italic>e</italic>
 <sub>1</sub></td>
									<td align="center">−319.05</td>
									<td align="center">467.79</td>
									<td align="center">0.76</td>
								</tr>
								<tr>
									<td align="center"><italic>e</italic>
 <sub>2</sub></td>
									<td align="center">−638.10</td>
									<td align="center">689.37</td>
									<td align="center">1.12</td>
								</tr>
								<tr>
									<td align="center"><italic>f</italic>
 <sub>1</sub></td>
									<td align="center">0*</td>
									<td align="center">1692.65</td>
									<td align="center">2.75</td>
								</tr>
								<tr>
									<td align="center"><italic>g</italic>
 <sub>1</sub></td>
									<td align="center">687.96</td>
									<td align="center">1692.65</td>
									<td align="center">2.75</td>
								</tr>
								<tr>
									<td align="center"><italic>f</italic>
 <sub>2</sub></td>
									<td align="center">−1165.61</td>
									<td align="center">1692.65</td>
									<td align="center">2.75</td>
								</tr>
								<tr>
									<td align="center"><italic>g</italic>
 <sub>2</sub></td>
									<td align="center">422.02</td>
									<td align="center">1692.65</td>
									<td align="center">2.75</td>
								</tr>
							</tbody>
						</table>
						<table-wrap-foot>
							<fn id="TFN1">
								<p>* The axis falls outside of the footing</p>
							</fn>
							<fn id="TFN2">
								<p>Source: Prepared by the author.</p>
							</fn>
						</table-wrap-foot>
					</table-wrap>
				</p>
				<p>Then, the bending shear forces satisfy with the ACI code [<xref ref-type="bibr" rid="B16">26</xref>].</p>
				<p>The punching shear force that act on the critical sections of the rectangular combined footing by <xref ref-type="disp-formula" rid="e19">eq. (22)</xref> and (<xref ref-type="disp-formula" rid="e20">24</xref>), and the allowable punching shear forces for the concrete by the code are obtained [<xref ref-type="bibr" rid="B16">26</xref>] (see <xref ref-type="table" rid="t2">Table 2</xref>).</p>
				<p>
					<table-wrap id="t2">
						<label>Table 2</label>
						<caption>
							<title>Punching shear forces of the example 2. </title>
						</caption>
						<table frame="hsides" rules="groups">
							<colgroup>
								<col/>
								<col/>
								<col/>
								<col/>
							</colgroup>
							<thead>
								<tr>
									<th align="center">Analysis section</th>
									<th align="center">Shear force that acts (kN)</th>
									<th align="center">Allowable shear force (kN)</th>
									<th align="center">Critical perimeter (m)</th>
								</tr>
							</thead>
							<tbody>
								<tr>
									<td align="center" rowspan="3">Column 1 (boundary column)</td>
									<td align="center" rowspan="3">1057.24</td>
									<td align="center">4948.69</td>
									<td align="center" rowspan="3">2.68</td>
								</tr>
								<tr>
									<td align="center">8101.84</td>
								</tr>
								<tr>
									<td align="center">3202.09</td>
								</tr>
								<tr>
									<td align="center" rowspan="3">Column 2 (inner column)</td>
									<td align="center" rowspan="3">2198.61</td>
									<td align="center">8272.44</td>
									<td align="center" rowspan="3">4.48</td>
								</tr>
								<tr>
									<td align="center">11347.38</td>
								</tr>
								<tr>
									<td align="center">5352.76</td>
								</tr>
							</tbody>
						</table>
						<table-wrap-foot>
							<fn id="TFN3">
								<p>Source: Prepared by the author.</p>
							</fn>
						</table-wrap-foot>
					</table-wrap>
				</p>
				<p>Then, the two punching shear forces satisfy with the ACI code [<xref ref-type="bibr" rid="B26">26</xref>]. </p>
				<p>The reinforcement steel areas for the rectangular combined footing that result of the bending moments are shown below (see <xref ref-type="table" rid="t3">Table 3</xref>).</p>
				<p>
					<table-wrap id="t3">
						<label>Table 3</label>
						<caption>
							<title>Reinforcement steel of the example 2. </title>
						</caption>
						<table frame="hsides" rules="groups">
							<colgroup>
								<col/>
								<col/>
								<col span="2"/>
							</colgroup>
							<thead>
								<tr>
									<th align="center">Direction of the steel</th>
									<th align="center">Steel location</th>
									<th align="center" colspan="2">Steel area (cm<sup>2</sup>)</th>
								</tr>
							</thead>
							<tbody>
								<tr>
									<td align="center" rowspan="10">Y axis</td>
									<td align="center" rowspan="3">Under column 1 (width of <italic>c</italic>
 <sub>
 <italic>1</italic>
</sub> 
 <italic>+ s + d</italic>/2)</td>
									<td align="center">Main steel</td>
									<td align="center">17.21</td>
								</tr>
								<tr>
									<td align="center">Minimum steel</td>
									<td align="center">18.24</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">20.28(4Ø1”)</td>
								</tr>
								<tr>
									<td align="center" rowspan="3">Under column 2 (width of <italic>c</italic>
 <sub>
 <italic>3</italic>
</sub> 
 <italic>+ d</italic>)</td>
									<td align="center">Main steel</td>
									<td align="center">34.70</td>
								</tr>
								<tr>
									<td align="center">Minimum steel</td>
									<td align="center">26.88</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">35.49(7Ø1”)</td>
								</tr>
								<tr>
									<td align="center" rowspan="2">Steel at the bottom (width of <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> 
 <italic>− c</italic>
 <sub>
 <italic>1</italic>
</sub> 
 <italic>− c</italic>
 <sub>
 <italic>3</italic>
</sub> 
 <italic>− s −</italic> 3<italic>d</italic>/2)</td>
									<td align="center">Temperature steel</td>
									<td align="center">89.57</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">91.20(32Ø3/4”)</td>
								</tr>
								<tr>
									<td align="center" rowspan="2">Steel at the top (width of <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> )</td>
									<td align="center">Temperature steel</td>
									<td align="center">116.64</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">116.85(41Ø3/4”)</td>
								</tr>
								<tr>
									<td align="center" rowspan="6">X axis</td>
									<td align="center" rowspan="3">Steel at the Bottom (width of <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> )</td>
									<td align="center">Main steel</td>
									<td align="center">35.11</td>
								</tr>
								<tr>
									<td align="center">Minimum steel</td>
									<td align="center">66.00</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">70.98(14Ø1”)</td>
								</tr>
								<tr>
									<td align="center" rowspan="3">Steel at the Top (width of <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> )</td>
									<td align="center">Main steel</td>
									<td align="center">57.80</td>
								</tr>
								<tr>
									<td align="center">Minimum steel</td>
									<td align="center">66.00</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">70.98(14Ø1”)</td>
								</tr>
							</tbody>
						</table>
						<table-wrap-foot>
							<fn id="TFN4">
								<p>Source: Prepared by the author.</p>
							</fn>
						</table-wrap-foot>
					</table-wrap>
				</p>
			</sec>
			<sec>
				<title>4.3. Example 3</title>
				<p>Substituting the corresponding values into <xref ref-type="disp-formula" rid="e8">eq. (9)</xref>, (<xref ref-type="disp-formula" rid="e13">15</xref>) and (<xref ref-type="disp-formula" rid="e15">17</xref>) to obtain the bending moments that act on the critical sections of the rectangular combined footing are shown below: Ma1 = 433.44 kN-m; Ma2 = 866.88 kN-m; Ma3 = 866.88 kN-m; Mb1 = 0.08 kN-m; Md1 = − 406.22 kN-m; Mb2 = − 73.36 kN-m; Md2 = 448.43 kN-m; Mb3 = 198.02 kN-m; Md3 = − 123.47 kN-m; Mmax12 = − 1797.11 kN-m (maximum bending moment between the column 1 and column 2) in xmax12 = 4.17 m (position of the maximum bending moment between the column 1 and column 2); Mmax23 = − 1794.99 kN-m (maximum bending moment between the column 2 and column 3) in xmax23 = − 1.71 m (position of the maximum bending moment between the column 2 and column 3).</p>
				<p>The maximum bending moment between the two columns is obtained as follows: First, the position of the maximum bending moment is located from the equation of the shear forces, i.e., when the shear force is zero, the maximum moment is obtained.</p>
				<p>After making different proposals, the effective depth is <italic>d</italic> = 72.00 <italic>cm</italic>, <italic>r</italic> = 8.00 <italic>cm</italic>, <italic>t</italic> = 80.00 <italic>cm</italic>.</p>
				<p>The bending shear forces that act on the critical sections of the rectangular combined footing by <xref ref-type="disp-formula" rid="e17">eq. (19)</xref>, (<xref ref-type="disp-formula" rid="e18">20</xref>) and (<xref ref-type="disp-formula" rid="e11">11</xref>), and the allowable bending shear forces for the concrete by the code are obtained [<xref ref-type="bibr" rid="B26">26</xref>] (see <xref ref-type="table" rid="t4">Table 4</xref>).</p>
				<p>
					<table-wrap id="t4">
						<label>Table 4</label>
						<caption>
							<title>Bending shear forces of the example 3. </title>
						</caption>
						<table frame="hsides" rules="groups">
							<colgroup>
								<col/>
								<col/>
								<col/>
								<col/>
							</colgroup>
							<thead>
								<tr>
									<th align="center">Axis</th>
									<th align="center">Shear force that acts (kN)</th>
									<th align="center">Allowable shear force (kN)</th>
									<th align="center">Width of analysis (m)</th>
								</tr>
							</thead>
							<tbody>
								<tr>
									<td align="center"><italic>e</italic>1</td>
									<td align="center">−290.58</td>
									<td align="center">467.79</td>
									<td align="center">0.76</td>
								</tr>
								<tr>
									<td align="center"><italic>e</italic>2</td>
									<td align="center">−581.16</td>
									<td align="center">689.37</td>
									<td align="center">1.12</td>
								</tr>
								<tr>
									<td align="center"><italic>e</italic>3</td>
									<td align="center">−581.16</td>
									<td align="center">689.37</td>
									<td align="center">1.12</td>
								</tr>
								<tr>
									<td align="center"><italic>f</italic>1</td>
									<td align="center">0*</td>
									<td align="center">1600.32</td>
									<td align="center">2.60</td>
								</tr>
								<tr>
									<td align="center"><italic>g</italic>1</td>
									<td align="center">768.99</td>
									<td align="center">1600.32</td>
									<td align="center">2.60</td>
								</tr>
								<tr>
									<td align="center"><italic>f</italic>2</td>
									<td align="center">−879.44</td>
									<td align="center">1600.32</td>
									<td align="center">2.60</td>
								</tr>
								<tr>
									<td align="center"><italic>g</italic>2</td>
									<td align="center">759.28</td>
									<td align="center">1600.32</td>
									<td align="center">2.60</td>
								</tr>
								<tr>
									<td align="center"><italic>f</italic>3</td>
									<td align="center">−988.95</td>
									<td align="center">1600.32</td>
									<td align="center">2.60</td>
								</tr>
								<tr>
									<td align="center"><italic>g</italic>3</td>
									<td align="center">601.45</td>
									<td align="center">1600.32</td>
									<td align="center">2.60</td>
								</tr>
							</tbody>
						</table>
						<table-wrap-foot>
							<fn id="TFN5">
								<p>* The axis falls outside of the footing</p>
							</fn>
							<fn id="TFN6">
								<p>Source: Prepared by the author.</p>
							</fn>
						</table-wrap-foot>
					</table-wrap>
				</p>
				<p>Then, the bending shear forces satisfy with the code [<xref ref-type="bibr" rid="B26">26</xref>].</p>
				<p>The punching shear forces acting on the critical section of the rectangular combined footing by <xref ref-type="disp-formula" rid="e19">eq. (22)</xref> and (<xref ref-type="disp-formula" rid="e20">24</xref>) are obtained, and the allowable punching shear forces for the concrete by the code are obtained [<xref ref-type="bibr" rid="B26">26</xref>] (see <xref ref-type="table" rid="t5">Table 5</xref>). </p>
				<p>
					<table-wrap id="t5">
						<label>Table 5</label>
						<caption>
							<title>Punching shear forces of the example 3. </title>
						</caption>
						<table frame="hsides" rules="groups">
							<colgroup>
								<col/>
								<col/>
								<col/>
								<col/>
							</colgroup>
							<thead>
								<tr>
									<th align="center">Analysis section</th>
									<th align="center">Shear force that acts (kN)</th>
									<th align="center">Allowable shear force (kN)</th>
									<th align="center">Critical perimeter (m)</th>
								</tr>
							</thead>
							<tbody>
								<tr>
									<td align="center" rowspan="3">Column 1 (boundary column)</td>
									<td align="center" rowspan="3">1070.95</td>
									<td align="center">4948.69</td>
									<td align="center" rowspan="3">2.68</td>
								</tr>
								<tr>
									<td align="center">8101.84</td>
								</tr>
								<tr>
									<td align="center">3202.09</td>
								</tr>
								<tr>
									<td align="center" rowspan="3">Column 2 (inner column)</td>
									<td align="center" rowspan="3">2202.51</td>
									<td align="center">8272.44</td>
									<td align="center" rowspan="3">4.48</td>
								</tr>
								<tr>
									<td align="center">11347.38</td>
								</tr>
								<tr>
									<td align="center">5352.76</td>
								</tr>
								<tr>
									<td align="center" rowspan="3">Column 3 (inner column)</td>
									<td align="center" rowspan="3">2189.98</td>
									<td align="center">8272.44</td>
									<td align="center" rowspan="3">4.48</td>
								</tr>
								<tr>
									<td align="center">11347.38</td>
								</tr>
								<tr>
									<td align="center">5352.76</td>
								</tr>
							</tbody>
						</table>
						<table-wrap-foot>
							<fn id="TFN7">
								<p>Source: Prepared by the author.</p>
							</fn>
						</table-wrap-foot>
					</table-wrap>
				</p>
				<p>Then, the two punching shear forces satisfy with the ACI code [<xref ref-type="bibr" rid="B26">26</xref>].</p>
				<p>The reinforcement steel areas for the rectangular combined footing that result of the bending moments are shown below (see <xref ref-type="table" rid="t6">Table 6</xref>).</p>
				<p>
					<table-wrap id="t6">
						<label>Table 6</label>
						<caption>
							<title>Reinforcement steel of the example 3. </title>
						</caption>
						<table frame="hsides" rules="groups">
							<colgroup>
								<col/>
								<col/>
								<col span="2"/>
							</colgroup>
							<thead>
								<tr>
									<th align="center">Direction of the steel</th>
									<th align="center">Steel location</th>
									<th align="center" colspan="2">Steel area (cm<sup>2</sup>)</th>
								</tr>
							</thead>
							<tbody>
								<tr>
									<td align="center" rowspan="13">Y axis</td>
									<td align="center" rowspan="3">Under column 1 (width of <italic>c</italic>
 <sub>
 <italic>1</italic>
</sub> 
 <italic>+ s + d</italic>/2)</td>
									<td align="center">Main steel</td>
									<td align="center">16.27</td>
								</tr>
								<tr>
									<td align="center">Minimum steel</td>
									<td align="center">18.24</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">20.28(4Ø1”)</td>
								</tr>
								<tr>
									<td align="center" rowspan="3">Under column 2 (width of <italic>c</italic>
 <sub>
 <italic>3</italic>
</sub> 
 <italic>+ d</italic>)</td>
									<td align="center">Main steel</td>
									<td align="center">32.79</td>
								</tr>
								<tr>
									<td align="center">Minimum steel</td>
									<td align="center">26.88</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">35.49(7Ø1”)</td>
								</tr>
								<tr>
									<td align="center" rowspan="3">Under column 3 (width of <italic>c</italic>
 <sub>
 <italic>5</italic>
</sub> 
 <italic>+ d</italic>)</td>
									<td align="center">Main steel</td>
									<td align="center">32.79</td>
								</tr>
								<tr>
									<td align="center">Minimum steel</td>
									<td align="center">26.88</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">35.49(7Ø1”)</td>
								</tr>
								<tr>
									<td align="center" rowspan="2">Steel at the bottom (width of <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> 
 <italic>− c</italic>
 <sub>
 <italic>1</italic>
</sub> 
 <italic>− c</italic>
 <sub>
 <italic>3</italic>
</sub> 
 <italic>- c</italic>
 <sub>
 <italic>5</italic>
</sub> 
 <italic>− s −</italic> 5<italic>d</italic>/2)</td>
									<td align="center">Temperature steel</td>
									<td align="center">165.60</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">168.15(59Ø3/4”)</td>
								</tr>
								<tr>
									<td align="center" rowspan="2">Steel at the top (width of <italic>L</italic>
 <sub>
 <italic>x</italic>
</sub> )</td>
									<td align="center">Temperature steel</td>
									<td align="center">208.80</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">210.90(74Ø3/4”)</td>
								</tr>
								<tr>
									<td align="center" rowspan="6">X axis</td>
									<td align="center" rowspan="3">Steel at the Bottom (width of <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> )</td>
									<td align="center">Main steel</td>
									<td align="center">16.58</td>
								</tr>
								<tr>
									<td align="center">Minimum steel</td>
									<td align="center">62.40</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">65.91(13Ø1”)</td>
								</tr>
								<tr>
									<td align="center" rowspan="3">Steel at the Top (width of <italic>L</italic>
 <sub>
 <italic>y</italic>
</sub> )</td>
									<td align="center">Main steel</td>
									<td align="center">67.76</td>
								</tr>
								<tr>
									<td align="center">Minimum steel</td>
									<td align="center">62.40</td>
								</tr>
								<tr>
									<td align="center">Proposed steel</td>
									<td align="center">70.98(14Ø1”)</td>
								</tr>
							</tbody>
						</table>
						<table-wrap-foot>
							<fn id="TFN8">
								<p>Source: Prepared by the author.</p>
							</fn>
						</table-wrap-foot>
					</table-wrap>
				</p>
			</sec>
		</sec>
		<sec sec-type="conclusions">
			<title>5. Conclusions</title>
			<p>The model presented in this paper applies only for design of the rectangular footings that support <italic>n</italic> columns aligned on a longitudinal axis, this model assumes that the footings should be rigid and the supporting soil layers elastic, which meet expression of the bidirectional bending, i.e., the pressure variation behaves linearly.</p>
			<p>This paper concludes the following:</p>
			<p>
				<list list-type="order">
					<list-item>
						<p>The thickness for the rectangular isolated footing is governed by the bending shear on the e1 axis, and the thicknesses for the rectangular combined footings that support two and three columns are governed by the bending shear on the e2 axes.</p>
					</list-item>
					<list-item>
						<p>This document is not limited as those presented by other authors such as: “Design of isolated footings of rectangular form using a new model” by Luévanos-Rojas [<xref ref-type="bibr" rid="B12">12</xref>], this model considers only a column. “A new model for the design of rectangular combined footings of boundary with two opposite sides restricted” by Luévanos-Rojas [<xref ref-type="bibr" rid="B19">19</xref>], this model considers only two columns.</p>
					</list-item>
					<list-item>
						<p>The proposed model is more suited to the real conditions with respect to the classical model, because the proposed model takes into account the linear soil pressure and the classical model considers a uniform pressure (maximum pressure) in all the contact surface, when the loads and moments act on the footing.</p>
					</list-item>
					<list-item>
						<p>The proposed model for design of rectangular footings subjected to an axial load and two moments in orthogonal directions in each column can be used for the following considerations:</p>
					</list-item>
				</list>
			</p>
			<p>
				<list list-type="simple">
					<list-item>
						<p>a) Without restrictions on their sides</p>
					</list-item>
					<list-item>
						<p>b) One side restricted</p>
					</list-item>
					<list-item>
						<p>c) Two restricted opposite sides</p>
					</list-item>
				</list>
			</p>
			<p>The main advantage of this document over other documents is that this model can be applied to one (rectangular isolated footings), two or more columns that are supported by a rectangular footing, and it is also not restricted to that the resultant force must be located on a longitudinal axis.</p>
			<p>The next investigations can be: 1) Modeling for the design of foundation slabs and/or rafts. 2) When another type of soil is presented under the footing, by example in 100% cohesive soils (clay soils) or in 100% granular soils (sandy soils), the pressure diagram is different (nonlinear) and should be treated as shown in <xref ref-type="fig" rid="f1">Fig. 1</xref>.</p>
		</sec>
	</body>
	<back>
		<ref-list>
			<title>References</title>
			<ref id="B1">
				<label>1</label>
				<mixed-citation>Bowles, J.E., Foundation analysis and design. McGraw-Hill, New York, 2001.</mixed-citation>
				<element-citation publication-type="book">
					<person-group person-group-type="author">
						<name>
							<surname>Bowles</surname>
							<given-names>J.E</given-names>
						</name>
					</person-group>
					<source>Foundation analysis and design</source>
					<publisher-name>McGraw-Hill</publisher-name>
					<publisher-loc>New York</publisher-loc>
					<year>2001</year>
				</element-citation>
			</ref>
			<ref id="B2">
				<label>2</label>
				<mixed-citation>Guler, K. and Celep, Z., Response of a rectangular plate-column system on a tensionless Winkler foundation subjected to static and dynamic loads. Structural Engineering and Mechanics, 21(6), pp. 699-712, 2005. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2005.21.6.699">https://doi.org/10.12989/sem.2005.21.6.699 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Guler</surname>
							<given-names>K.</given-names>
						</name>
						<name>
							<surname>Celep</surname>
							<given-names>Z</given-names>
						</name>
					</person-group>
					<article-title>Response of a rectangular plate-column system on a tensionless Winkler foundation subjected to static and dynamic loads</article-title>
					<source>Structural Engineering and Mechanics</source>
					<volume>21</volume>
					<issue>6</issue>
					<fpage>699</fpage>
					<lpage>712</lpage>
					<year>2005</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2005.21.6.699">https://doi.org/10.12989/sem.2005.21.6.699 </ext-link>
				</element-citation>
			</ref>
			<ref id="B3">
				<label>3</label>
				<mixed-citation>Chen, W-R., Chen, C-S. and Yu, S-Y., Nonlinear vibration of hybrid composite plates on elastic foundations. Structural Engineering and Mechanics, 37(4), pp. 367-383, 2011. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2011.37.4.367">https://doi.org/10.12989/sem.2011.37.4.367 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Chen</surname>
							<given-names>W-R.</given-names>
						</name>
						<name>
							<surname>Chen</surname>
							<given-names>C-S.</given-names>
						</name>
						<name>
							<surname>Yu</surname>
							<given-names>S-Y</given-names>
						</name>
					</person-group>
					<article-title>Nonlinear vibration of hybrid composite plates on elastic foundations</article-title>
					<source>Structural Engineering and Mechanics</source>
					<volume>37</volume>
					<issue>4</issue>
					<fpage>367</fpage>
					<lpage>383</lpage>
					<year>2011</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2011.37.4.367">https://doi.org/10.12989/sem.2011.37.4.367 </ext-link>
				</element-citation>
			</ref>
			<ref id="B4">
				<label>4</label>
				<mixed-citation>Smith-Pardo, J.P., Performance-based framework for soil-structure systems using simplified rocking foundation models. Structural Engineering and Mechanics, 40(6), pp. 763-782, 2011. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2011.40.6.763">https://doi.org/10.12989/sem.2011.40.6.763 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Smith-Pardo</surname>
							<given-names>J.P</given-names>
						</name>
					</person-group>
					<article-title>Performance-based framework for soil-structure systems using simplified rocking foundation models</article-title>
					<source>Structural Engineering and Mechanics</source>
					<volume>40</volume>
					<issue>6</issue>
					<fpage>763</fpage>
					<lpage>782</lpage>
					<year>2011</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2011.40.6.763">https://doi.org/10.12989/sem.2011.40.6.763 </ext-link>
				</element-citation>
			</ref>
			<ref id="B5">
				<label>5</label>
				<mixed-citation>Shahin, M.A. and Cheung, E.M., Stochastic design charts for bearing capacity of strip footings. Geomechanics and Engineering, 3(2), pp. 153-167, 2011. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/gae.2011.3.2.153">https://doi.org/10.12989/gae.2011.3.2.153</ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Shahin</surname>
							<given-names>M.A.</given-names>
						</name>
						<name>
							<surname>Cheung</surname>
							<given-names>E.M</given-names>
						</name>
					</person-group>
					<article-title>Stochastic design charts for bearing capacity of strip footings</article-title>
					<source>Geomechanics and Engineering</source>
					<volume>3</volume>
					<issue>2</issue>
					<fpage>153</fpage>
					<lpage>167</lpage>
					<year>2011</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/gae.2011.3.2.153">https://doi.org/10.12989/gae.2011.3.2.153</ext-link>
				</element-citation>
			</ref>
			<ref id="B6">
				<label>6</label>
				<mixed-citation>Zhang, L., Zhao, M.H., Xiao, Y. and Ma, B.H., Nonlinear analysis of finite beam resting on Winkler with consideration of beam-soil interface resistance effect. Structural Engineering and Mechanics, 38(5), pp. 573-592, 2011. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2011.38.5.573">https://doi.org/10.12989/sem.2011.38.5.573 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Zhang</surname>
							<given-names>L.</given-names>
						</name>
						<name>
							<surname>Zhao</surname>
							<given-names>M.H.</given-names>
						</name>
						<name>
							<surname>Xiao</surname>
							<given-names>Y.</given-names>
						</name>
						<name>
							<surname>Ma</surname>
							<given-names>B.H</given-names>
						</name>
					</person-group>
					<article-title>Nonlinear analysis of finite beam resting on Winkler with consideration of beam-soil interface resistance effect.</article-title>
					<source>Structural Engineering and Mechanics</source>
					<volume>38</volume>
					<issue>5</issue>
					<fpage>573</fpage>
					<lpage>592</lpage>
					<year>2011</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2011.38.5.573">https://doi.org/10.12989/sem.2011.38.5.573 </ext-link>
				</element-citation>
			</ref>
			<ref id="B7">
				<label>7</label>
				<mixed-citation>Agrawal, R. and Hora, M.S., Nonlinear interaction behaviour of infilled frame-isolated footings-soil system subjected to seismic loading. Structural Engineering and Mechanics, 44(1), pp. 85-107, 2012. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2012.44.1.085">https://doi.org/10.12989/sem.2012.44.1.085 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Agrawal</surname>
							<given-names>R.</given-names>
						</name>
						<name>
							<surname>Hora</surname>
							<given-names>M.S</given-names>
						</name>
					</person-group>
					<article-title>Nonlinear interaction behaviour of infilled frame-isolated footings-soil system subjected to seismic loading</article-title>
					<source>Structural Engineering and Mechanics</source>
					<volume>44</volume>
					<issue>1</issue>
					<fpage>85</fpage>
					<lpage>107</lpage>
					<year>2012</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2012.44.1.085">https://doi.org/10.12989/sem.2012.44.1.085 </ext-link>
				</element-citation>
			</ref>
			<ref id="B8">
				<label>8</label>
				<mixed-citation>Rad, A.B., Static response of 2-D functionally graded circular plate with gradient thickness and elastic foundations to compound loads. Structural Engineering and Mechanics, 44(2), pp. 139-161, 2012. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2012.44.2.139">https://doi.org/10.12989/sem.2012.44.2.139 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Rad</surname>
							<given-names>A.B</given-names>
						</name>
					</person-group>
					<article-title>Static response of 2-D functionally graded circular plate with gradient thickness and elastic foundations to compound loads</article-title>
					<source>Structural Engineering and Mechanics</source>
					<volume>44</volume>
					<issue>2</issue>
					<fpage>139</fpage>
					<lpage>161</lpage>
					<year>2012</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2012.44.2.139">https://doi.org/10.12989/sem.2012.44.2.139 </ext-link>
				</element-citation>
			</ref>
			<ref id="B9">
				<label>9</label>
				<mixed-citation>Orbanich, C.J., Dominguez, P.N. and Ortega, N.F., Strenghtening and repair of concrete foundation beams whit fiber composite materials. Materials and Structures, 45, pp. 1693-1704, 2012. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1617/s11527-012-9866-6">https://doi.org/10.1617/s11527-012-9866-6 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Orbanich</surname>
							<given-names>C.J.</given-names>
						</name>
						<name>
							<surname>Dominguez</surname>
							<given-names>P.N.</given-names>
						</name>
						<name>
							<surname>Ortega</surname>
							<given-names>N.F</given-names>
						</name>
					</person-group>
					<article-title>Strenghtening and repair of concrete foundation beams whit fiber composite materials</article-title>
					<source>Materials and Structures</source>
					<issue>45</issue>
					<fpage>1693</fpage>
					<lpage>1704</lpage>
					<year>2012</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1617/s11527-012-9866-6">https://doi.org/10.1617/s11527-012-9866-6 </ext-link>
				</element-citation>
			</ref>
			<ref id="B10">
				<label>10</label>
				<mixed-citation>Mohamed, F.M.O., Vanapalli, S.K. and Saatcioglu, M. Generalized Schmertmann equation for settlement estimation of shallow footings in saturated and unsaturated sands. Geomechanics and Engineering, 5(4), pp. 363-377, 2013. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/gae.2013.5.4.343">https://doi.org/10.12989/gae.2013.5.4.343 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Mohamed</surname>
							<given-names>F.M.O.</given-names>
						</name>
						<name>
							<surname>Vanapalli</surname>
							<given-names>S.K.</given-names>
						</name>
						<name>
							<surname>Saatcioglu</surname>
							<given-names>M</given-names>
						</name>
					</person-group>
					<article-title>Generalized Schmertmann equation for settlement estimation of shallow footings in saturated and unsaturated sands</article-title>
					<source>Geomechanics and Engineering</source>
					<volume>5</volume>
					<issue>4</issue>
					<fpage>363</fpage>
					<lpage>377</lpage>
					<year>2013</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/gae.2013.5.4.343">https://doi.org/10.12989/gae.2013.5.4.343 </ext-link>
				</element-citation>
			</ref>
			<ref id="B11">
				<label>11</label>
				<mixed-citation>Orbanich, C.J. and Ortega, N.F., Analysis of elastic foundation plates with internal and perimetric stiffening beams on elastic foundations by using Finite Differences Method. Structural Engineering and Mechanics, 45(2), pp. 169-182, 2013. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2013.45.2.169.">https://doi.org/10.12989/sem.2013.45.2.169.</ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Orbanich</surname>
							<given-names>C.J.</given-names>
						</name>
						<name>
							<surname>Ortega</surname>
							<given-names>N.F</given-names>
						</name>
					</person-group>
					<article-title>Analysis of elastic foundation plates with internal and perimetric stiffening beams on elastic foundations by using Finite Differences Method</article-title>
					<source>Structural Engineering and Mechanics</source>
					<volume>45</volume>
					<issue>2</issue>
					<fpage>169</fpage>
					<lpage>182</lpage>
					<year>2013</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2013.45.2.169.">https://doi.org/10.12989/sem.2013.45.2.169.</ext-link>
				</element-citation>
			</ref>
			<ref id="B12">
				<label>12</label>
				<mixed-citation>Luévanos-Rojas, A., Faudoa-Herrera, J.G., Andrade-Vallejo, R.A. and Cano-Alvarez M.A., Design of isolated footings of rectangular form using a new model. International Journal of Innovative Computing, Information and Control, 9(10), pp. 4001-4022, 2013. DOI: <ext-link ext-link-type="uri" xlink:href="http://www.ijicic.org/ijicic-12-10031.pdf">http://www.ijicic.org/ijicic-12-10031.pdf </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Luévanos-Rojas</surname>
							<given-names>A.</given-names>
						</name>
						<name>
							<surname>Faudoa-Herrera</surname>
							<given-names>J.G.</given-names>
						</name>
						<name>
							<surname>Andrade-Vallejo</surname>
							<given-names>R.A.</given-names>
						</name>
						<name>
							<surname>Cano-Alvarez</surname>
							<given-names>M.A</given-names>
						</name>
					</person-group>
					<article-title>Design of isolated footings of rectangular form using a new model</article-title>
					<source>International Journal of Innovative Computing, Information and Control</source>
					<volume>9</volume>
					<issue>10</issue>
					<fpage>4001</fpage>
					<lpage>4022</lpage>
					<year>2013</year>
					<ext-link ext-link-type="uri" xlink:href="http://www.ijicic.org/ijicic-12-10031.pdf">http://www.ijicic.org/ijicic-12-10031.pdf </ext-link>
				</element-citation>
			</ref>
			<ref id="B13">
				<label>13</label>
				<mixed-citation>Aristizabal-Ochoa, J.D., Stability of slender columns on an elastic foundation with generalised end conditions. Ingeniería e Investigación, 33(3), pp. 34-40, 2013.</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Aristizabal-Ochoa</surname>
							<given-names>J.D</given-names>
						</name>
					</person-group>
					<article-title>Stability of slender columns on an elastic foundation with generalised end conditions</article-title>
					<source>Ingeniería e Investigación</source>
					<volume>33</volume>
					<issue>3</issue>
					<fpage>34</fpage>
					<lpage>40</lpage>
					<year>2013</year>
				</element-citation>
			</ref>
			<ref id="B14">
				<label>14</label>
				<mixed-citation>Barreto-Maya, A.P., Valencia-González, Y. y Echeverri-Ramírez, O., Evaluación comparativa de la capacidad de carga en cimentaciones profundas. Fórmulas analíticas y ensayos de carga. Boletín Ciencias de la Tierra, 33, pp. 93-110, 2013.</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Barreto-Maya</surname>
							<given-names>A.P.</given-names>
						</name>
						<name>
							<surname>Valencia-González</surname>
							<given-names>Y.</given-names>
						</name>
						<name>
							<surname>Echeverri-Ramírez</surname>
							<given-names>O</given-names>
						</name>
					</person-group>
					<article-title>Evaluación comparativa de la capacidad de carga en cimentaciones profundas. Fórmulas analíticas y ensayos de carga</article-title>
					<source>Boletín Ciencias de la Tierra</source>
					<issue>33</issue>
					<fpage>93</fpage>
					<lpage>110</lpage>
					<year>2013</year>
				</element-citation>
			</ref>
			<ref id="B15">
				<label>15</label>
				<mixed-citation>Luévanos-Rojas, A., Design of isolated footings of circular form using a new model. Structural Engineering and Mechanics, 52(4), pp. 767-786, 2014. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2014.52.4.767">https://doi.org/10.12989/sem.2014.52.4.767 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Luévanos-Rojas</surname>
							<given-names>A</given-names>
						</name>
					</person-group>
					<article-title>Design of isolated footings of circular form using a new model</article-title>
					<source>Structural Engineering and Mechanics</source>
					<volume>52</volume>
					<issue>4</issue>
					<fpage>767</fpage>
					<lpage>786</lpage>
					<year>2014</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2014.52.4.767">https://doi.org/10.12989/sem.2014.52.4.767 </ext-link>
				</element-citation>
			</ref>
			<ref id="B16">
				<label>16</label>
				<mixed-citation>Uncuoğlu, E., The bearing capacity of square footings on a sand layer overlying clay. Geomechanics and Engineering, 9(3), pp. 287-311, 2015. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/gae.2015.9.3.287">https://doi.org/10.12989/gae.2015.9.3.287 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Uncuoğlu</surname>
							<given-names>E</given-names>
						</name>
					</person-group>
					<article-title>The bearing capacity of square footings on a sand layer overlying clay</article-title>
					<source>Geomechanics and Engineering</source>
					<volume>9</volume>
					<issue>3</issue>
					<fpage>287</fpage>
					<lpage>311</lpage>
					<year>2015</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/gae.2015.9.3.287">https://doi.org/10.12989/gae.2015.9.3.287 </ext-link>
				</element-citation>
			</ref>
			<ref id="B17">
				<label>17</label>
				<mixed-citation>Luévanos-Rojas, A., Design of boundary combined footings of trapezoidal form using a new model. Structural Engineering and Mechanics, 56(5), pp. 745-765, 2015. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2015.56.5.745">https://doi.org/10.12989/sem.2015.56.5.745 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Luévanos-Rojas</surname>
							<given-names>A</given-names>
						</name>
					</person-group>
					<article-title>Design of boundary combined footings of trapezoidal form using a new model</article-title>
					<source>Structural Engineering and Mechanics</source>
					<volume>56</volume>
					<issue>5</issue>
					<fpage>745</fpage>
					<lpage>765</lpage>
					<year>2015</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/sem.2015.56.5.745">https://doi.org/10.12989/sem.2015.56.5.745 </ext-link>
				</element-citation>
			</ref>
			<ref id="B18">
				<label>18</label>
				<mixed-citation>Camero, H.E., A novel finite element method for designing floor slabs on grade and pavements with loads at edges. Ingeniería e Investigación, 35(2), pp. 15-22, 2015. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.15446/ing.investig.v35n2.45603">https://doi.org/10.15446/ing.investig.v35n2.45603 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Camero</surname>
							<given-names>H.E</given-names>
						</name>
					</person-group>
					<article-title>A novel finite element method for designing floor slabs on grade and pavements with loads at edges</article-title>
					<source>Ingeniería e Investigación</source>
					<volume>35</volume>
					<issue>2</issue>
					<fpage>15</fpage>
					<lpage>22</lpage>
					<year>2015</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.15446/ing.investig.v35n2.45603">https://doi.org/10.15446/ing.investig.v35n2.45603 </ext-link>
				</element-citation>
			</ref>
			<ref id="B19">
				<label>19</label>
				<mixed-citation>Luévanos-Rojas, A., A new model for the design of rectangular combined boundary footings with two restricted opposite sides. Revista ALCONPAT, 6(2), pp. 172-187, 2016. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.21041/ra.v6i2.137">https://doi.org/10.21041/ra.v6i2.137 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Luévanos-Rojas</surname>
							<given-names>A.</given-names>
						</name>
					</person-group>
					<article-title>A new model for the design of rectangular combined boundary footings with two restricted opposite sides</article-title>
					<source>Revista ALCONPAT</source>
					<volume>6</volume>
					<issue>2</issue>
					<fpage>172</fpage>
					<lpage>187</lpage>
					<year>2016</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.21041/ra.v6i2.137">https://doi.org/10.21041/ra.v6i2.137 </ext-link>
				</element-citation>
			</ref>
			<ref id="B20">
				<label>20</label>
				<mixed-citation>Mohebkhah, A., Bearing capacity of strip footings on a stone masonry trench in clay. Geomechanics and Engineering, 13(2), pp. 255-267, 2017. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/gae.2017.13.2.255">https://doi.org/10.12989/gae.2017.13.2.255 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Mohebkhah</surname>
							<given-names>A</given-names>
						</name>
					</person-group>
					<article-title>Bearing capacity of strip footings on a stone masonry trench in clay</article-title>
					<source>Geomechanics and Engineering</source>
					<volume>13</volume>
					<issue>2</issue>
					<fpage>255</fpage>
					<lpage>267</lpage>
					<year>2017</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/gae.2017.13.2.255">https://doi.org/10.12989/gae.2017.13.2.255 </ext-link>
				</element-citation>
			</ref>
			<ref id="B21">
				<label>21</label>
				<mixed-citation>López-Chavarría, S., Luévanos-Rojas, A. and Medina-Elizondo, M., A new mathematical model for design of square isolated footings for general case. International Journal of Innovative Computing, Information and Control, 13(4), pp. 1149-1168, 2017. DOI: <ext-link ext-link-type="uri" xlink:href="http://www.ijicic.org/ijicic-130406.pdf">http://www.ijicic.org/ijicic-130406.pdf </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>López-Chavarría</surname>
							<given-names>S.</given-names>
						</name>
						<name>
							<surname>Luévanos-Rojas</surname>
							<given-names>A.</given-names>
						</name>
						<name>
							<surname>Medina-Elizondo</surname>
							<given-names>M</given-names>
						</name>
					</person-group>
					<article-title>A new mathematical model for design of square isolated footings for general case</article-title>
					<source>International Journal of Innovative Computing, Information and Control</source>
					<volume>13</volume>
					<issue>4</issue>
					<fpage>1149</fpage>
					<lpage>1168</lpage>
					<year>2017</year>
					<ext-link ext-link-type="uri" xlink:href="http://www.ijicic.org/ijicic-130406.pdf">http://www.ijicic.org/ijicic-130406.pdf </ext-link>
				</element-citation>
			</ref>
			<ref id="B22">
				<label>22</label>
				<mixed-citation>Anil, Ö, Akbaş, S.O., BabagĪray, S., Gel, A.C. and Durucan, C., Experimental and finite element analyses of footings of varying shapes on sand. Geomechanics and Engineering, 12(2), pp. 223-238, 2017. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/gae.2017.12.2.223">https://doi.org/10.12989/gae.2017.12.2.223 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Anil</surname>
							<given-names>Ö</given-names>
						</name>
						<name>
							<surname>Akbaş</surname>
							<given-names>S.O.</given-names>
						</name>
						<name>
							<surname>BabagĪray</surname>
							<given-names>S.</given-names>
						</name>
						<name>
							<surname>Gel</surname>
							<given-names>A.C.</given-names>
						</name>
						<name>
							<surname>Durucan</surname>
							<given-names>C</given-names>
						</name>
					</person-group>
					<article-title>Experimental and finite element analyses of footings of varying shapes on sand</article-title>
					<source>Geomechanics and Engineering</source>
					<volume>12</volume>
					<issue>2</issue>
					<fpage>223</fpage>
					<lpage>238</lpage>
					<year>2017</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/gae.2017.12.2.223">https://doi.org/10.12989/gae.2017.12.2.223 </ext-link>
				</element-citation>
			</ref>
			<ref id="B23">
				<label>23</label>
				<mixed-citation>Luévanos-Rojas, A., Barquero-Cabrero, J.D., López-Chavarría, S. and Medina-Elizondo, M., A comparative study for design of boundary combined footings of trapezoidal and rectangular forms using new models. Coupled Systems Mechanics, 6(4), pp. 417-437, 2017. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/csm.2017.6.4.417">https://doi.org/10.12989/csm.2017.6.4.417 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Luévanos-Rojas</surname>
							<given-names>A.</given-names>
						</name>
						<name>
							<surname>Barquero-Cabrero</surname>
							<given-names>J.D.</given-names>
						</name>
						<name>
							<surname>López-Chavarría</surname>
							<given-names>S.</given-names>
						</name>
						<name>
							<surname>Medina-Elizondo</surname>
							<given-names>M</given-names>
						</name>
					</person-group>
					<article-title>A comparative study for design of boundary combined footings of trapezoidal and rectangular forms using new models</article-title>
					<source>Coupled Systems Mechanics</source>
					<volume>6</volume>
					<issue>4</issue>
					<fpage>417</fpage>
					<lpage>437</lpage>
					<year>2017</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/csm.2017.6.4.417">https://doi.org/10.12989/csm.2017.6.4.417 </ext-link>
				</element-citation>
			</ref>
			<ref id="B24">
				<label>24</label>
				<mixed-citation>Luévanos-Rojas, A., López-Chavarría, S. and Medina-Elizondo, M., A new model for T-shaped combined footings. Part II: mathematical model for design. Geomechanics and Engineering, 14(1), pp. 61-69, 2018. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/gae.2018.14.1.061">https://doi.org/10.12989/gae.2018.14.1.061 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Luévanos-Rojas</surname>
							<given-names>A.</given-names>
						</name>
						<name>
							<surname>López-Chavarría</surname>
							<given-names>S.</given-names>
						</name>
						<name>
							<surname>Medina-Elizondo</surname>
							<given-names>M</given-names>
						</name>
					</person-group>
					<article-title>A new model for T-shaped combined footings. Part II: mathematical model for design</article-title>
					<source>Geomechanics and Engineering</source>
					<volume>14</volume>
					<issue>1</issue>
					<fpage>61</fpage>
					<lpage>69</lpage>
					<year>2018</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/gae.2018.14.1.061">https://doi.org/10.12989/gae.2018.14.1.061 </ext-link>
				</element-citation>
			</ref>
			<ref id="B25">
				<label>25</label>
				<mixed-citation>Yáñez-Palafox, J.A., Luévanos-Rojas, A., López-Chavarría, S. and Medina-Elizondo, M., Modeling for the strap combined footings. Part II: mathematical model for design. Steel Composite Structures, 30(2), pp. 109-121, 2019. DOI: <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/scs.2019.30.2.109">https://doi.org/10.12989/scs.2019.30.2.109 </ext-link>
				</mixed-citation>
				<element-citation publication-type="journal">
					<person-group person-group-type="author">
						<name>
							<surname>Yáñez-Palafox</surname>
							<given-names>J.A.</given-names>
						</name>
						<name>
							<surname>Luévanos-Rojas</surname>
							<given-names>A.</given-names>
						</name>
						<name>
							<surname>López-Chavarría</surname>
							<given-names>S.</given-names>
						</name>
						<name>
							<surname>Medina-Elizondo</surname>
							<given-names>M</given-names>
						</name>
					</person-group>
					<article-title>Modeling for the strap combined footings. Part II: mathematical model for design</article-title>
					<source>Steel Composite Structures</source>
					<volume>30</volume>
					<issue>2</issue>
					<fpage>109</fpage>
					<lpage>121</lpage>
					<year>2019</year>
					<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.12989/scs.2019.30.2.109">https://doi.org/10.12989/scs.2019.30.2.109 </ext-link>
				</element-citation>
			</ref>
			<ref id="B26">
				<label>26</label>
				<mixed-citation>American Concrete Institute. Building Code requirements for structural concrete and commentary. Committee 318. New York, 2019.</mixed-citation>
				<element-citation publication-type="book">
					<person-group person-group-type="author">
						<collab>American Concrete Institute</collab>
					</person-group>
					<source>Building Code requirements for structural concrete and commentary. Committee 318</source>
					<publisher-loc>New York</publisher-loc>
					<year>2019</year>
				</element-citation>
			</ref>
		</ref-list>
		<fn-group>
			<fn fn-type="other" id="fn1">
				<label>How to cite:</label>
				<p> Rivera-Mendoza, J.B., Arnulfo Luévanos-Rojas, A., López-Chavarría, S., Medina-Elizondo, M. and García-Galván, M. A general model for rectangular footings part II: modeling for design. DYNA, 89(223), pp. 9-18, July - September, 2022.</p>
			</fn>
			<fn fn-type="other" id="fn2">
				<label>J.B. Rivera-Mendoza, </label>
				<p>received a MSc. in Business Administration in 1985, and the PhD in Administration and Senior Management in 2018, all of thrm from the Facultad de Contaduría y Administración of the Universidad Autónoma de Coahuila, Torreón, Coahuila, Mexico. He is professor and researcher of the Universidad Autónoma de Coahuila (2018-Current). His research interests are mathematical models applied to Administration. He has 5 papers published in international scientific research Journals. ORCID-iD: 0000-0002-0514-0796</p>
			</fn>
			<fn fn-type="other" id="fn3">
				<label>A. Luévanos-Rojas,</label>
				<p> received his BSc. Eng. in Civil Engineering in 1981, his MSc. in Planning and Construction in 1996, and the PhD Engineering in Planning and Construction in 2009, all of them from the Facultad de Ingeniería, Ciencias y Arquitectura of the Universidad Juárez del Estado de Durango, Gómez Palacio, Durango, México. He received the MSc. in Structures in 1983, from the Escuela Superior de Ingeniería y Arquitectura the Instituto Politécnico Nacional, Distrito Federal, México. Also, he received the MSc. in Administration in 2004, from the Facultad de Contaduría y Administración of the Universidad Autónoma de Coahuila, Torreón, Coahuila, Mexico. He is professor and researcher of the Universidad Autónoma de Coahuila (2015-Current). He has more than 100 papers published in international scientific research Journals. His research interests include: mathematical models applied to structures. He is a member of the National System of Researchers of Mexico. ORCID-iD: 0000-0002-0198-3614 </p>
			</fn>
			<fn fn-type="other" id="fn4">
				<label>S. López-Chavarría,</label>
				<p> received his BSc. in Public Accountant, his MSc. in Administration, and the PhD in Administration and Senior Management from the Facultad de Contaduría y Administración of the Universidad Autónoma de Coahuila, Torreón, Coahuila, Mexico. She is professor and researcher of the Universidad Autónoma de Coahuila (2000-Current). His research interests include mathematical models applied to structures, methods of structural analysis, design of concrete and steel structural members, and analysis of non-prismatic members. She has more than 50 papers published in national and international scientific research Journals. She has been a speaker at scientific meetings in España, Colombia, Argentina. She is a member of the National System of Researchers of Mexico. ORCID-iD: 0000-0001-8909-1794</p>
			</fn>
			<fn fn-type="other" id="fn5">
				<label>M. Medina-Elizondo, </label>
				<p>received his BSc. in Public Accountant, his MSc. in Administration from the Facultad de Contaduría y Administración of the Universidad Autónoma de Coahuila, Torreón, Coahuila, Mexico. He received the PhD in Administration Sciences from the Universidad Nacional Autónoma de México, Distrito Federal, Mexico. Also, he received the PhD in Administration Sciences from the Universidad de Newport, U.S.A. He is professor and researcher of the Universidad Autónoma de Coahuila (1988-Current). His research interests include mathematical models applied to structures, methods of structural analysis, design of concrete and steel structural members, and analysis of non-prismatic members. He has more than 80 papers published in national and international scientific research Journals. ORCID-iD: 0000-0002-6113-4964</p>
			</fn>
			<fn fn-type="other" id="fn6">
				<label>M. García-Galván,</label>
				<p> received a MSc. in International Business Law in 2002, from the ITESM in Monterrey Campus, and the PhD in Administration and Senior Management in 2018, from the Facultad de Contaduría y Administración of the Universidad Autónoma de Coahuila, Torreón, Coahuila, Mexico. She is professor and researcher of the Universidad Autónoma de Coahuila (2018-Current). His research interests are mathematical models applied to Administration. She has 5 papers published in international scientific research Journals. ORCID-iD: 0000-0001-8854-0930</p>
			</fn>
		</fn-group>
	</back>
</article>