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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Built Environ.</journal-id>
<journal-title>Frontiers in Built Environment</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Built Environ.</abbrev-journal-title>
<issn pub-type="epub">2297-3362</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">783051</article-id>
<article-id pub-id-type="doi">10.3389/fbuil.2021.783051</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Built Environment</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Comparison Between Numerical Modeling Approaches of Infilled Frames Under In-Plane Load</article-title>
<alt-title alt-title-type="left-running-head">Bouarroudj and Boudaoud</alt-title>
<alt-title alt-title-type="right-running-head">Numerical Modeling of Masonry Infills</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Bouarroudj</surname>
<given-names>Mohammed Amin</given-names>
</name>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1408738/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Boudaoud</surname>
<given-names>Zeineddine</given-names>
</name>
</contrib>
</contrib-group>
<aff>
<institution>Department of Civil Engineering</institution>, <institution>University of Larbi Ben M&#x2019;Hidi</institution>, <addr-line>Oum El Bouaghi</addr-line>, <country>Algeria</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/276945/overview">Fabio Mazza</ext-link>, University of Calabria, Italy</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/504416/overview">Gabriele Milani</ext-link>, Politecnico di Milano, Italy</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/386527/overview">Andr&#xe9; Furtado</ext-link>, University of Porto, Portugal</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/869321/overview">Maria Teresa De Risi</ext-link>, University of Naples Federico II, Italy</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Mohammed Amin Bouarroudj, <email>bouarroudjmohammedamin@gmail.com</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Earthquake Engineering, a section of the journal Frontiers in Built Environment</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>25</day>
<month>02</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>7</volume>
<elocation-id>783051</elocation-id>
<history>
<date date-type="received">
<day>25</day>
<month>09</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>15</day>
<month>12</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Bouarroudj and Boudaoud.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Bouarroudj and Boudaoud</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these&#x20;terms.</p>
</license>
</permissions>
<abstract>
<p>In the last few decades, important attention was given to infill masonry panels due to their worldwide uses. Many experimental and numerical studies were conducted to study their effect on the behavior of RC frames. In general, three modeling strategies are widely applied to model infill masonry, namely, micro-models, meso-models, and macro-models. This study investigates the accuracy of the width models to predict the behavior of masonry infills using the meso-modeling technique. To this aim, the masonry infills are modeled as an equivalent homogenized diagonal element in order to represent the diagonal action of masonry infills. The width models used to determine the width of the diagonal strut are used in meso-modeling. In addition, the study contains comparisons between different modeling techniques to predict the global behavior of the infilled frames. Experimental tests conducted on two infilled frames from the literature are considered to calibrate the numerical simulations. The results indicate that the micro-modeling approach gives a good agreement with the experimental tests in terms of lateral force and deformation shapes, the related errors varying between 0.12 and 2.8%. Using single strut models, the differences between numerical and experimental results vary from 1.1 to 20%. On the other hand, the errors obtained from multiple strut models are varying between 9 and&#x20;40%.</p>
</abstract>
<kwd-group>
<kwd>finite element analysis</kwd>
<kwd>infilled frame</kwd>
<kwd>masonry</kwd>
<kwd>nonlinear analysis</kwd>
<kwd>reinforced concrete</kwd>
<kwd>micro model</kwd>
<kwd>meso model</kwd>
<kwd>macro model</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>Infill masonry panels are used worldwide for reinforced concrete buildings. This heterogeneous material is used for internal and external separations, which provide thermal and acoustic insulation. During earthquakes, infill panels are subjected to in-plane lateral forces received from the frame-infill connections. These forces imply different failure modes to a masonry infill. According to the experimental investigation conducted by <xref ref-type="bibr" rid="B42">Mehrabi et&#x20;al. (1996)</xref>, five different failure modes are observed. At lower displacement, diagonal/sliding cracks are started to develop along the infills. This failure is recorded in all specimens tested. During the increase of the displacement, the first mode is followed by a slip failure along with beam-infill connection for specimens with a strong frame and then followed by shear cracks developed in the columns when strong infills are used. On the other hand, a slip along the bed joints is developed instead of column shear cracks for specimens with weak infills. At higher displacement amplitudes, corner crushing appears to all tested specimens. More recent classification is made by <xref ref-type="bibr" rid="B7">Asteris P. G. et&#x20;al. (2011)</xref> based on the experimental investigation conducted by <xref ref-type="bibr" rid="B27">Kakaletsis and Karayannis (2007)</xref>. The masonry in-plane damages are classified to five different failure modes: sliding shear (SS), diagonal cracking (DK), diagonal compression (DC), corner crushing (CC), and frame failure (FF). In addition to in-plane loading, the infill masonry can be subjected to out-of-plane loads. This type of loads is applied in the perpendicular direction of the frame which can cause collapse of the infill out of the plane of the&#x20;frame.</p>
<p>During the last few decades, important attention is given to the effect of masonry infill walls on responses of steel and reinforced concrete (R/C) frames. Experimental studies demonstrated that the existence of masonry infills affects the global response of structures by increasing the strength and the stiffness. The effect of masonry infills is directly affected by several parameters such as the existence of openings, the frame-infill connection, type of units (solid or hollow), and type of mortar (weak or strong). <xref ref-type="bibr" rid="B69">Zarnic and Tomazevic&#x2019;s (1988)</xref> experimental study showed that the effect of masonry infills is related to the masonry units&#x2019; type and the presence of openings. A similar investigation conducted by <xref ref-type="bibr" rid="B27">Kakaletsis and Karayannis (2007)</xref> indicates that the presence of an opening in the infill masonry panel reduces the strength and the stiffness of the infilled frames whereas the reduction rate is related to the size, position, and type of the opening. Moreover, the frame-infill connection has an important role in the force transferring between the two elements. Based on an experimental study, <xref ref-type="bibr" rid="B52">Pires and Carvalho (1992)</xref> concluded that a strong frame-infill connection leads to higher strength and stiffness of the infilled frames rather than a poor connection. Besides, the study also showed that the mechanical characteristics of masonry affect both the behavior and the failure mode mechanisms. In addition, <xref ref-type="bibr" rid="B42">Mehrabi et&#x20;al. (1996)</xref> concluded that the aspect ratio of infills and the distribution of the vertical loads affect the global behavior of infilled frames.</p>
<p>Furthermore, numerical studies are introduced to investigate the in-plane and out-of-plane behaviors of masonry infills using different modeling techniques. <xref ref-type="bibr" rid="B49">Nicola et&#x20;al. (2015)</xref> and <xref ref-type="bibr" rid="B51">Petracca et&#x20;al. (2017)</xref> classified three main strategies, namely, micro-modeling, meso-modeling, and macro-modeling. In the first technique, the masonry infill is divided into numerous elements (<xref ref-type="bibr" rid="B12">Crisafulli et&#x20;al. (2000)</xref>). Two strategies can be distinguished, detailed micro-modeling, where the units, mortar, and unit&#x2013;mortar interfaces are modeled separately. This method is used by <xref ref-type="bibr" rid="B57">Riddington and Naom (1994)</xref> to predict the compressive strength of masonry. On the other hand, the complexity is reduced by replacing the mortar joints with zero-thickness elements [<xref ref-type="bibr" rid="B34">Louren&#xe7;o Paulo and Rots. (1997)</xref>]. This method is classified as the simplified micro-model, as mentioned by <xref ref-type="bibr" rid="B49">Nicola et&#x20;al. (2015)</xref>. <xref ref-type="bibr" rid="B43">Mehrabi and Benson Shing (1997)</xref> developed a cohesive dilatant interface model to represent the behavior of mortar joints using finite element code FEAP. A similar approach is used by <xref ref-type="bibr" rid="B2">Al-Chaar et&#x20;al. (2008)</xref> to simulate the behavior of infilled reinforced concrete (R/C) frames using the commercial finite element software DIANA. More recently, <xref ref-type="bibr" rid="B46">Mohyeddin et&#x20;al. (2013)</xref> suggested adding an elastic mortar band in the center of each brick element in order to eliminate the penetration and the complete loss of contact elements during the analysis.</p>
<p>The previous method takes into account all masonry infill details by modeling each component as a separate element. This approach makes the modeling process more complex and difficult to realize. Alternatively, the meso-modeling approach treats the masonry infills as one single element. The masonry infill components are smeared out as one equivalent element using the homogenization technique. This technique is based on selecting a periodic unit cell that includes all component types. The periodic unit cell should be selected in a way where its repetition generates the entire masonry panel [<xref ref-type="bibr" rid="B55">Quinteros et&#x20;al. (2012)</xref>]. This technique was used by several researchers. Based on numerical simulation, (<xref ref-type="bibr" rid="B36">Ma et&#x20;al. (2001)</xref> applied the homogenization concept on a representative volume element, equivalent to a periodic unit cell, to determine the equivalent properties of masonry infills with various boundary conditions. The authors report that the homogenized properties can be employed to simulate large masonry panels by using a small unit cell concept and when the stress and strain field does not vary intensively. <xref ref-type="bibr" rid="B55">Quinteros et&#x20;al. (2012)</xref> used the homogenization technique proposed by <xref ref-type="bibr" rid="B33">Lopez et&#x20;al. (1999)</xref>, which is based on the periodic unit cell, to study the behavior of masonry walls subjected to a combination of in-plane and out-of-plane loads. The authors conclude that the homogenization procedure can be developed to include the effect of compressive strength and the tensile failure of bricks and can be used to study the out-of-plane behavior of masonry panels. For masonry panels subjected to in-plane loads, <xref ref-type="bibr" rid="B24">Houda et&#x20;al. (2017)</xref> applied the homogenization method to estimate the strength of masonry panels constructed with a periodic concrete hollow block. The previous homogenization is applied for masonry walls with periodic patterns. In the case of non-periodic masonry walls, masonry walls without regular distribution of brick units, and mortar joints, such as old buildings, the homogenization technique can be applied using the concept of test-window [<xref ref-type="bibr" rid="B62">Tiberti and Milani (2020a)</xref>]. <xref ref-type="bibr" rid="B63">Tiberti and Milani (2020b)</xref> applied this technique to investigate the out-of-plane collapse behavior of old European structures with multi-leaf masonry&#x20;walls.</p>
<p>The macro-modeling strategy adopts different modeling techniques. A simplification comprises the use of a single strut or multi-diagonal struts. The first appearance of this technique is established based on the observation made by <xref ref-type="bibr" rid="B53">Polyakove (1957)</xref> [as reported by <xref ref-type="bibr" rid="B18">Furtado et&#x20;al. (2015)</xref>] who observed during a series of experimental tests on infilled steel frames that the infills behave as a compression element in a diagonal direction when the surrounding frame is subjected to lateral in-plane forces. Later, the studies conducted by <xref ref-type="bibr" rid="B22">Holmes (1961)</xref> and by <xref ref-type="bibr" rid="B37">Mainstone and Weeks (1970)</xref> confirmed the diagonal behaving action of masonry infills. Recently, different macro models are proposed in the literature. <xref ref-type="bibr" rid="B22">Holmes (1961)</xref>, <xref ref-type="bibr" rid="B38">Mainstone RJ.&#x20;(1974)</xref>, <xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref>, <xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref>, and <xref ref-type="bibr" rid="B65">Turgay et&#x20;al. (2014)</xref> suggested that the representation of masonry infills with a single diagonal strut is appropriate to capture the global behavior of infilled frames. On the contrary, <xref ref-type="bibr" rid="B16">El-Dakhakhni et&#x20;al. (2003)</xref>, <xref ref-type="bibr" rid="B11">Crisafulli and Carr, (2007)</xref>, and <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref> suggested that multi-diagonal struts are more accurate to capture the internal effects of infills on R/C or a steel frame. Considering the out-of-plane behavior, <xref ref-type="bibr" rid="B50">Pant&#xf2; et&#x20;al. (2018)</xref> developed a three-dimension macro-model to represent the out-of-plane behavior of infilled frame structures. Other researchers developed macro-models to account both the in-plane and the out-of-plane. Among them, <xref ref-type="bibr" rid="B26">Kadysiewski and Mosalam (2009)</xref> proposed a model to describe the combined behaviors with single strut models. Meanwhile, <xref ref-type="bibr" rid="B54">Pradhan and Cavaleri (2020)</xref> used the multi-strut model proposed by <xref ref-type="bibr" rid="B58">Rodrigues et&#x20;al. (2010)</xref> to account the in-plane and out-of-plane behaviors of infilled masonry.</p>
<p>The first main contribution proposed in this study is the use of the meso-modeling approach to investigate the accuracy of several width models proposed in the literature. To this aim, the masonry infills are modeled as an equivalent homogenized diagonal element. The width in meso-modeling is calculated according to several models selected for macro-modeling. The equivalent properties are defined from the experimental behaviors of masonry infills.</p>
<p>In addition, this study contains a comparison between the accuracy of micro-, meso-, and macro-modeling techniques. In micro-modeling, the infills are modeled with the simplified approach where the units are extended to the half-thick of joints in each direction. In macro-modeling, the diagonal strut is modeled with a 3D spar element that works only in compression and has no tension or bending resistance. The numerical simulation is carried out using the finite element software ANSYS. Two specimens experimented by <xref ref-type="bibr" rid="B42">Mehrabi et&#x20;al. (1996)</xref> subjected to monotonic increasing loads are selected to validate the numerical simulations. Thus, the comparisons are performed by comparing the numerical and the experimental results in terms of maximum force, initial stiffness, and stiffness at the peak force, followed by comparing the behavior of the force&#x2013;displacement curves after reaching the maximum force. In addition, the deformation shape obtained from the micro-modeling is compared to that of the experimental.</p>
</sec>
<sec id="s2">
<title>2 Modeling Techniques of Masonry Infills</title>
<p>From the literature, three different modeling techniques can be classified to model masonry infills, known as micro-, meso-, and macro-modeling. These techniques are different in terms of complexity, computational time, and accuracy. The micro-modeling technique is more accurate among the two other methods. The consideration of details in the modeling process makes this method more useful for research purposes which can capture the local phenomena and the failure modes of the interaction between the different components. The complexity and the computational time make micro-modeling inappropriate in large structures. The meso-modeling approach is less complicated than micro-modeling. These modeling techniques are based on modeling the masonry infill as one homogenized element. This simplification is useful to study the frame-infill contacts. A more practical method is known as macro-modeling. The simplicity makes this method more appropriate for large structures.</p>
<sec id="s2-1">
<title>2.1&#x20;Micro-Modeling</title>
<p>
<xref ref-type="fig" rid="F1">Figure&#x20;1A</xref> illustrates the micro-modeling approach of infilled frames. As mentioned above, this method can be classified into detailed and simplified micro-modeling. In detailed micro-modeling, all components of the masonry infill are modeled with separate elements. The masonry units and mortar joints are considered continuum elements, while the interaction surfaces are described with contact or interface elements. In the simplified method [<xref ref-type="bibr" rid="B34">Louren&#xe7;o Paulo and Rots (1997)</xref>], the mortar joints are replaced with a zero-thickness element (contact or interface element), and each masonry unit is extended on each side to the mid-thickness of the adjacent mortar joints. This method was used in most numerical investigations <xref ref-type="bibr" rid="B43">Mehrabi and Benson Shing (1997)</xref>, <xref ref-type="bibr" rid="B2">Al-Chaar et&#x20;al. (2008)</xref>, <xref ref-type="bibr" rid="B35">Kong et al. (2015)</xref>, <xref ref-type="bibr" rid="B35">LouziRabab Abdel Karim, (2015)</xref>, and <xref ref-type="bibr" rid="B47">Mohyeddin-Kermani, (2011)</xref>. <xref ref-type="fig" rid="F1">Figure&#x20;1B</xref> illustrates the transformation from a detailed to a simplified&#x20;model.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Micro and meso modeling approaches <bold>(A)</bold> infilled frame <bold>(B)</bold> transforming detailed to simplified micro modeling according to <xref ref-type="bibr" rid="B34">Louren&#xe7;o Paulo and Rots. (1997)</xref> <bold>(C)</bold> homogenization procedure.</p>
</caption>
<graphic xlink:href="fbuil-07-783051-g001.tif"/>
</fig>
</sec>
<sec id="s2-2">
<title>2.2&#x20;Meso-Modeling</title>
<p>In meso-modeling, the masonry infills are considered homogenized elements. This method required the definition of equivalent material properties that can produce the same behavior as the masonry infill. To this aim, <xref ref-type="bibr" rid="B33">Lopez et&#x20;al. (1999)</xref>, <xref ref-type="bibr" rid="B5">Anthoine (1995)</xref>, <xref ref-type="bibr" rid="B59">Sacco (2009)</xref>, <xref ref-type="bibr" rid="B55">Quinteros et&#x20;al. (2012)</xref>, and <xref ref-type="bibr" rid="B24">Houda et&#x20;al. (2017)</xref> used the concept of the periodic unit cell to homogenize the masonry walls, also known as the representative element of volume (REV) such as in <xref ref-type="bibr" rid="B36">Ma et&#x20;al. (2001)</xref> and <xref ref-type="bibr" rid="B62">Tiberti and Milani (2020a)</xref>. This procedure is based on selecting a small element from the masonry wall that contains all the components and can generate the all-masonry wall with repetition of this element. The previous concept required regular distribution of the brick units and mortar joints. On the other hand, when the masonry panel is not periodically arranged, <xref ref-type="bibr" rid="B63">Tiberti and Milani (2020b)</xref> used the concept of test-window to employ the homogenized procedure. <xref ref-type="fig" rid="F1">Figure&#x20;1C</xref> illustrates the homogenization procedure for a periodic masonry&#x20;panel.</p>
</sec>
<sec id="s2-3">
<title>2.3&#x20;Macro-Modeling</title>
<p>The previous method is a complex task. The long computational time needed to solve the models made it inappropriate in engineering practice. Otherwise, the macro-modeling approach simplifies the contribution of the masonry infill on the global behavior based on its physical acting when the surrounded frame is subjected to lateral loads (<xref ref-type="fig" rid="F2">Figure&#x20;2A</xref>). The masonry infills are treated as single or multiple diagonal struts. Besides, it represents a more practical tool in engineering practice. The main geometric property required is the width of the&#x20;strut.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Macro models: <bold>(A)</bold> one diagonal strut model <bold>(B)</bold> multi-strut model of <xref ref-type="bibr" rid="B9">Chrysostomou (1991)</xref> <bold>(C)</bold> <xref ref-type="bibr" rid="B16">El-Dakhakhni and Hamid (2003)</xref> <bold>(D)</bold> <xref ref-type="bibr" rid="B11">Crisafulli and Carr (2007)</xref> <bold>(E)</bold> <xref ref-type="bibr" rid="B58">Rodrigues and Costa (2010)</xref> <bold>(F)</bold> <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref> Developed macro model to consider in-plane and out-of-plane interactions: <bold>(G)</bold> <xref ref-type="bibr" rid="B26">Kadysiewski and Mosalam (2009)</xref> <bold>(H)</bold> <xref ref-type="bibr" rid="B15">Don&#xe0; et&#x20;al. (2017)</xref> <bold>(I)</bold> <xref ref-type="bibr" rid="B64">Trapani et al. (2018)</xref> <bold>(J)</bold> <xref ref-type="bibr" rid="B18">Furtado et al. (2016)</xref> <bold>(K)</bold> <xref ref-type="bibr" rid="B20">Gesualdi et al. (2020)</xref>.</p>
</caption>
<graphic xlink:href="fbuil-07-783051-g002.tif"/>
</fig>
<p>Several equations proposed to calculate the width of the diagonal strut are reported in this section. The selected equations relate the width of the strut to the diagonal length and inclination, the thickness, and the mechanical properties of the masonry and concrete materials. In addition, the dimensions and the type of brick units can affect the width of the strut, where larger brick units will affect the total arrangement of the masonry infill, which implies an effect on the diagonal behavior of the masonry wall. The first expression suggested is that proposed by <xref ref-type="bibr" rid="B22">Holmes (1961)</xref>, known as the one-third rule. The width of the strut <xref ref-type="disp-formula" rid="e1">Eq. (1)</xref> is considered to be one-third the diagonal length of the masonry infill.<disp-formula id="e1">
<mml:math id="m80">
<mml:mrow>
<mml:mi mathvariant="normal">w</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="italic">d</mml:mi>
<mml:mi mathvariant="normal">m</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mn>3</mml:mn>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>
<disp-formula id="e2">
<mml:math id="m81">
<mml:mrow>
<mml:mi>w</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mn>0.115</mml:mn>
<mml:mrow>
<mml:msub>
<mml:mi>d</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:msubsup>
<mml:mi>&#x3bb;</mml:mi>
<mml:mi>h</mml:mi>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>0.4</mml:mn>
</mml:mrow>
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</mml:math>
<label>(2)</label>
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</p>
<p>According to <xref ref-type="bibr" rid="B39">Mainstone R. J.&#x20;(1974)</xref>, the width of the strut (<xref ref-type="disp-formula" rid="e2">Eq. 2</xref>) is related to masonry unit types (Bricks units or concrete blocks). This equation is adopted by the Federal Emergency Management Agency [<xref ref-type="bibr" rid="B17">FEMA (2000)</xref>]. The proposed expression is related to a dimensionless parameter <inline-formula id="inf7">
<mml:math id="m7">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">&#x3bb;</mml:mi>
<mml:mi mathvariant="normal">h</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (relative stiffness); this parameter is introduced to consider the relative stiffness of the infill and the frame. The relative stiffness is given by Stafford <xref ref-type="bibr" rid="B61">Smith (1962)</xref> as indicated in <xref ref-type="disp-formula" rid="e3">Eqs. 3</xref>, <xref ref-type="disp-formula" rid="e4">4</xref>:<disp-formula id="e3">
<mml:math id="m8">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">&#x3bb;</mml:mi>
<mml:mi mathvariant="normal">h</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mi mathvariant="normal">h</mml:mi>
<mml:msup>
<mml:mrow>
<mml:mrow>
<mml:mo>[</mml:mo>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">E</mml:mi>
<mml:mi mathvariant="normal">m</mml:mi>
</mml:msub>
<mml:mi mathvariant="normal">t</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:mi>sin</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:mn>2</mml:mn>
<mml:mi mathvariant="normal">&#x3b8;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>4</mml:mn>
<mml:msub>
<mml:mi mathvariant="normal">E</mml:mi>
<mml:mi mathvariant="normal">c</mml:mi>
</mml:msub>
<mml:msub>
<mml:mi mathvariant="normal">I</mml:mi>
<mml:mi mathvariant="normal">c</mml:mi>
</mml:msub>
<mml:msub>
<mml:mi mathvariant="normal">h</mml:mi>
<mml:mi mathvariant="normal">m</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
<mml:mo>]</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mrow>
<mml:mfrac bevelled="true">
<mml:mn>1</mml:mn>
<mml:mn>4</mml:mn>
</mml:mfrac>
</mml:mrow>
</mml:msup>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
<label>(3)</label>
</disp-formula>
<disp-formula id="e4">
<mml:math id="m9">
<mml:mrow>
<mml:mi mathvariant="normal">&#x3b8;</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mi>tan</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:msup>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">h</mml:mi>
<mml:mi mathvariant="normal">m</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">l</mml:mi>
<mml:mi mathvariant="normal">m</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
<label>(4)</label>
</disp-formula>where <inline-formula id="inf8">
<mml:math id="m10">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">E</mml:mi>
<mml:mi mathvariant="normal">c</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> and <inline-formula id="inf9">
<mml:math id="m11">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">E</mml:mi>
<mml:mi mathvariant="normal">m</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> are the concrete and the masonry elastic modulus, respectively, <inline-formula id="inf10">
<mml:math id="m12">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">I</mml:mi>
<mml:mi mathvariant="normal">c</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the moment of inertia of concrete column, <inline-formula id="inf11">
<mml:math id="m13">
<mml:mi mathvariant="normal">H</mml:mi>
</mml:math>
</inline-formula> and <inline-formula id="inf12">
<mml:math id="m14">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mi mathvariant="normal">m</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> are the height of the frame and the masonry infill, respectively, <inline-formula id="inf13">
<mml:math id="m15">
<mml:mi mathvariant="normal">l</mml:mi>
</mml:math>
</inline-formula> and <inline-formula id="inf14">
<mml:math id="m16">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">l</mml:mi>
<mml:mi mathvariant="normal">m</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the length of the frame and the masonry infill, respectively, <inline-formula id="inf15">
<mml:math id="m17">
<mml:mi mathvariant="normal">t</mml:mi>
</mml:math>
</inline-formula> is the thickness of the masonry wall, and <inline-formula id="inf16">
<mml:math id="m18">
<mml:mi mathvariant="normal">&#x3b8;</mml:mi>
</mml:math>
</inline-formula> is the diagonal inclination.</p>
<p>
<xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref> relate the width to the angle of the diagonal strut, as indicated in <xref ref-type="disp-formula" rid="e5">Eq. (5)</xref>. This equation is applied when the diagonal strut inclination ranges between 25&#xb0; and 50&#xb0; <xref ref-type="bibr" rid="B49">Nicola et&#x20;al. (2015)</xref>. <xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref> suggestion (<xref ref-type="disp-formula" rid="e6">Eq. 6</xref>) takes into account the status of the masonry infill wall and cracked or uncracked masonry infills (as reported in <xref ref-type="bibr" rid="B23">Hossameldeen Mohamed Ahmed, (2017)</xref>). <xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref>&#x2019;s expression (<xref ref-type="disp-formula" rid="e7">Eq. 7</xref>) is independent of the relative stiffness. More recently, <xref ref-type="bibr" rid="B65">Turgay et&#x20;al. (2014)</xref> proposed an expression (<xref ref-type="disp-formula" rid="e8">Eq. 8</xref>) that is dependent on the height&#x2013;length ratio of masonry. The equation is applicable when the ratio is between 1.2 and&#x20;2.<disp-formula id="e5">
<mml:math id="m82">
<mml:mrow>
<mml:mi>w</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:mn>0.95</mml:mn>
<mml:mi mathvariant="italic">sin</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:mn>2</mml:mn>
<mml:mi>&#x3b8;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:msqrt>
<mml:msub>
<mml:mi>&#x3bb;</mml:mi>
<mml:mi>h</mml:mi>
</mml:msub>
</mml:msqrt>
</mml:mrow>
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</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>d</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(5)</label>
</disp-formula>
<disp-formula id="e6">
<mml:math id="m83">
<mml:mrow>
<mml:mi>w</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mn>0.01</mml:mn>
<mml:mo>&#x002B;</mml:mo>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:mn>0.707</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>&#x3bb;</mml:mi>
<mml:mi>h</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(6)</label>
</disp-formula>
<disp-formula id="e7">
<mml:math id="m84">
<mml:mrow>
<mml:mi>w</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>d</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(7)</label>
</disp-formula>
<disp-formula id="e8">
<mml:math id="m85">
<mml:mrow>
<mml:mi>w</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:mn>0.18</mml:mn>
<mml:msub>
<mml:mi>d</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mn>4</mml:mn>
<mml:mrow>
<mml:msqrt>
<mml:msub>
<mml:mi>&#x3bb;</mml:mi>
<mml:mi>h</mml:mi>
</mml:msub>
</mml:msqrt>
</mml:mrow>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(8)</label>
</disp-formula>
</p>
<p>As mentioned by <xref ref-type="bibr" rid="B6">Asteris Panagiotis G. et&#x20;al. (2011)</xref>, the shortcoming of the single strut models is the incapability to capture the internal effects of masonry (frame-infill interaction, bending moments, and shear forces in the frame elements.). More complex models are proposed to represent the masonry infills with multi-struts. According to <xref ref-type="bibr" rid="B16">El-Dakhakhni et&#x20;al. (2003)</xref>, the complexity and the accuracy of macro-models are dependent on the number of struts. As an example, a three-strut model is more complicated and accurate than the single and two-strut models. <xref ref-type="bibr" rid="B9">Chrysostomou (1991)</xref> suggested a six-strut model (<xref ref-type="fig" rid="F2">Figure&#x20;2B</xref>), three struts in each direction. The model contains one diagonal strut and two off-diagonal struts positioned at the critical points of frame members. <xref ref-type="fig" rid="F2">Figure&#x20;2C</xref> illustrates the multi-strut model proposed by <xref ref-type="bibr" rid="B16">El-Dakhakhni et&#x20;al. (2003)</xref> to include the effects of masonry infills on the stiffness and strength of the infilled steel frames. Another multiple strut model is proposed by <xref ref-type="bibr" rid="B11">Crisafulli and Carr (2007)</xref>. The masonry infills are represented with two diagonal struts connected by a shear spring, as shown in <xref ref-type="fig" rid="F2">Figure&#x20;2D</xref>. The objective of the shear spring is to represent the shear behavior of the masonry wall. The model by <xref ref-type="bibr" rid="B58">Rodrigues et&#x20;al. (2010)</xref> is formed by four struts related to each other with a horizontal central element (<xref ref-type="fig" rid="F2">Figure&#x20;2E</xref>).</p>
<p>Based on a numerical study using ABAQUS <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref>, proposed a multi-strut model. At a lower drift level, the authors observed the formation of a single diagonal strut. At high drifts, the single strut developed into two diagonal struts. Based on these observations, <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref> proposed a three-strut model. The model is composed of one diagonal and two off-diagonal struts, as shown in <xref ref-type="fig" rid="F2">Figure&#x20;2F</xref>. <xref ref-type="disp-formula" rid="e9">Equation (9)</xref> is proposed to calculate the width of the off-diagonal struts. This equation is related to the model proposed by <xref ref-type="bibr" rid="B39">Mainstone R. J.&#x20;(1974)</xref>. For the diagonal strut, the width is considered to be one-half the off-diagonal width. <xref ref-type="disp-formula" rid="e12">Equation (12)</xref> defines the positions of the off-diagonal struts.<disp-formula id="e9">
<mml:math id="m19">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="italic">w</mml:mi>
<mml:mi mathvariant="italic">p</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.001</mml:mn>
<mml:msub>
<mml:mi mathvariant="italic">w</mml:mi>
<mml:mi mathvariant="italic">M</mml:mi>
</mml:msub>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mn>6</mml:mn>
<mml:mi mathvariant="italic">&#x3b8;</mml:mi>
<mml:mo>&#x2b;</mml:mo>
<mml:mn>7.5</mml:mn>
<mml:msub>
<mml:mi mathvariant="italic">&#x3b1;</mml:mi>
<mml:mi mathvariant="italic">p</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
<label>(9)</label>
</disp-formula>
<disp-formula id="e10">
<mml:math id="m20">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="italic">&#x3b1;</mml:mi>
<mml:mi mathvariant="italic">p</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mi mathvariant="italic">&#x3b1;</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mi mathvariant="italic">&#x3bb;</mml:mi>
<mml:mi mathvariant="italic">h</mml:mi>
</mml:msub>
<mml:mi mathvariant="italic">h,</mml:mi>
</mml:mrow>
</mml:math>
<label>(10)</label>
</disp-formula>
<disp-formula id="e11">
<mml:math id="m21">
<mml:mrow>
<mml:mi mathvariant="italic">&#x3b1;</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mi mathvariant="italic">tan</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:msup>
<mml:mfrac>
<mml:mn>1</mml:mn>
<mml:mi mathvariant="italic">&#x3bc;</mml:mi>
</mml:mfrac>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
<label>(11)</label>
</disp-formula>
<disp-formula id="e12">
<mml:math id="m22">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="italic">l</mml:mi>
<mml:mrow>
<mml:mi mathvariant="italic">ceff</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mi mathvariant="italic">p</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.006</mml:mn>
<mml:mi mathvariant="italic">h</mml:mi>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mi mathvariant="bold-italic">&#x3b8;</mml:mi>
<mml:mo>&#x2b;</mml:mo>
<mml:msub>
<mml:mi mathvariant="bold-italic">&#x3b1;</mml:mi>
<mml:mi mathvariant="italic">p</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>10</mml:mn>
<mml:msub>
<mml:mi mathvariant="bold-italic">&#x3bb;</mml:mi>
<mml:mi mathvariant="italic">h</mml:mi>
</mml:msub>
<mml:mi mathvariant="italic">h</mml:mi>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
<label>(12)</label>
</disp-formula>where <inline-formula id="inf17">
<mml:math id="m23">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="italic">w</mml:mi>
<mml:mi mathvariant="italic">p</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the width of the off-diagonal strut, <inline-formula id="inf18">
<mml:math id="m24">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="italic">w</mml:mi>
<mml:mi mathvariant="italic">M</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the width calculated from the model proposed by <xref ref-type="bibr" rid="B38">Mainstone RJ.&#x20;(1974)</xref>and, <inline-formula id="inf19">
<mml:math id="m25">
<mml:mi mathvariant="bold-italic">&#x3b8;</mml:mi>
</mml:math>
</inline-formula> and <inline-formula id="inf20">
<mml:math id="m26">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="italic">&#x3b1;</mml:mi>
<mml:mi mathvariant="italic">p</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> are the inclination of the diagonal and off-diagonal struts (in degrees), respectively. <inline-formula id="inf21">
<mml:math id="m27">
<mml:mi mathvariant="bold-italic">&#x3bc;</mml:mi>
</mml:math>
</inline-formula> is the friction coefficient between brick units and <inline-formula id="inf22">
<mml:math id="m28">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="italic">l</mml:mi>
<mml:mrow>
<mml:mi mathvariant="italic">ceff</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mi mathvariant="italic">p</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the contact length between the struts and the column.</p>
<p>Other researchers improved the macro-modeling technique to account for both the in-plane and the out-of-plane behaviors. <xref ref-type="bibr" rid="B26">Kadysiewski and Mosalam (2009)</xref> developed a practical model to include the effect of the in-plane and the out-of-plane behaviors of the masonry infill. The proposed model is based on representing the masonry infill with a single diagonal strut, which is sufficient to represent both behaviors of the masonry infill, works in tension and compression, and has a lumped mass at the mid of the diagonal length that works in the out-of-plane direction. <xref ref-type="fig" rid="F2">Figure&#x20;2G</xref> illustrates the model proposed by <xref ref-type="bibr" rid="B26">Kadysiewski and Mosalam (2009)</xref>. <xref ref-type="bibr" rid="B48">Mosalam and G&#xfc;nay (2015)</xref> developed a single strut macro-model that can account for the in-plane and out-of-plane interaction. Furthermore, <xref ref-type="bibr" rid="B32">Longo et&#x20;al. (2018)</xref> used the principle of the single diagonal strut to model the in-plane and out-of-plane behaviors. <xref ref-type="bibr" rid="B32">Longo et&#x20;al. (2018)</xref> adopted the model proposed by <xref ref-type="bibr" rid="B48">Mosalam and G&#xfc;nay (2015)</xref>. In addition to that, the authors assigned elastic springs at the column-beam joints in order to reproduce a realistic out-of-plane stiffness. <xref ref-type="bibr" rid="B15">Don&#xe0; et&#x20;al. (2017)</xref> proposed a two-strut model to combine both behaviors (<xref ref-type="fig" rid="F2">Figure&#x20;2H</xref>). The model is developed based on the model proposed by <xref ref-type="bibr" rid="B48">Mosalam and G&#xfc;nay (2015)</xref>. This model contains two diagonal struts modeled as the same way as <xref ref-type="bibr" rid="B11">Crisafulli and Carr (2007)</xref>&#x2019;s model. <xref ref-type="bibr" rid="B15">Don&#xe0; et&#x20;al. (2017)</xref> assigned two types of weights. The first type works in the in-plane direction, located at each beam-column joint. The second type works in the out-of-plane direction located at the mid-length of each strut and connected with a rigid link element. <xref ref-type="bibr" rid="B64">Trapani and Cavaleri, (2018)</xref> developed a macro-model that is applicable in static and dynamic analyses. The proposed model contains four struts, a vertical and a horizontal strut, and two diagonal struts, one in each direction. Each strut represents two beam-column elements with fiber cross sections. The authors report that the model can capture the arching action of the out-of-plane deformation and the interaction of the in-plane and out-of-plane behaviors. <xref ref-type="fig" rid="F2">Figure&#x20;2I</xref> illustrates the model proposed by <xref ref-type="bibr" rid="B64">Trapani and Cavaleri, (2018)</xref>. <xref ref-type="bibr" rid="B19">Furtado et&#x20;al. (2016)</xref> developed the multi-strut model proposed by <xref ref-type="bibr" rid="B58">Rodrigues et&#x20;al. (2010)</xref> to account for the in-plane and out-of-plane interaction. Using OpenSees software, <xref ref-type="bibr" rid="B19">Furtado et&#x20;al. (2016)</xref> connected the diagonal strut with a nonlinear link element. The out-of-plane masses are assigned to the two extremity nodes of the horizontal element, as illustrated in <xref ref-type="fig" rid="F2">Figure&#x20;2J</xref>. After, Al <xref ref-type="bibr" rid="B1">Hanoun and Schwarz, (2019)</xref> implemented the model to a practical graphical user interface software (SAP 2000).</p>
<p>Moreover, <xref ref-type="bibr" rid="B40">Mazza (2021)</xref> and <xref ref-type="bibr" rid="B41">Mazza and Donnici (2021)</xref> modeled the in-plane and the out-of-plane behaviors and their interaction with the same multi-strut model. In the studies, the in-plane behavior is described with the horizontal truss, and the out-of-plane response is represented with four diagonal elements (<xref ref-type="fig" rid="F2">Figure&#x20;2J</xref>). The lateral stiffness of the in-plane behavior is defined by <xref ref-type="bibr" rid="B39">Mainstone R. J.&#x20;(1974)</xref>&#x2019;s model, while the out-of-plane initial stiffness was defined by deriving the lumped masses and the vibration frequency of the masonry infill. <xref ref-type="bibr" rid="B20">Gesualdi et&#x20;al. (2020)</xref> studied the seismic performance of residential RC buildings by considering the two behaviors. The masonry infill is modeled with four diagonal struts forming two V-shapes. The V-shapes are connected with nonlinear zero-length link elements to reproduce the in-plane degradation due to the cyclic load. The same link element type is used to model the out-of-plane degradation. A lumped mass represents the out-of-plane mass that is assigned to the node that connects V-shapes. <xref ref-type="fig" rid="F2">Figure&#x20;2K</xref> illustrates the model with V-shapes.</p>
<p>
<xref ref-type="fig" rid="F3">Figure&#x20;3</xref> illustrates the variation of the strut width models according to the relative stiffness. The strut width models could be classified according to the relative stiffness as dependent and independent equations. For the equations related to the relative stiffness [<xref ref-type="bibr" rid="B38">Mainstone RJ.&#x20;(1974)</xref>, <xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref>, <xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref>; <xref ref-type="bibr" rid="B65">Turgay et&#x20;al. (2014)</xref>], the increase of the relative stiffness leads to decrease in the w/d ratio which applies a decrease in the width of the strut. After the relative stiffness exceeds a value of six, the variation is almost considered constant. On the other hand, the independent expressions indicate constant values during the variation of the relative stiffness. A high strut width value is presented by the equation proposed by <xref ref-type="bibr" rid="B22">Holmes (1961)</xref> when the relative stiffness exceeds a value of 3, which is the case in the considered experimental value (4.7). However, the expressions proposed by <xref ref-type="bibr" rid="B39">Mainstone R. J.&#x20;(1974)</xref> and <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref> indicate the lowest strut widths during the variation of the relative stiffness.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Comparison between difference strut width equations according to the variation of the relative stiffness for the frame of Specimen 9 (<xref ref-type="bibr" rid="B42">Mehrabi et al., 1996</xref>).</p>
</caption>
<graphic xlink:href="fbuil-07-783051-g003.tif"/>
</fig>
</sec>
</sec>
<sec id="s3">
<title>3 Description of the Experimental Study</title>
<p>Twelve experimental tests on one-story, one-bay, 1/2 scale R/C frames infilled with concrete masonry units are tested by <xref ref-type="bibr" rid="B42">Mehrabi et&#x20;al. (1996)</xref> to investigate the effect of four different parameters: the masonry unit type, aspect ratio, lateral load type, and distribution of vertical force on the behavior of the infilled frames. Two infilled frames with the same geometric characteristics, namely, specimens 8 and 9 are selected from the experimental test to calibrate the numerical simulation. The specimens have an aspect ratio of 0.67 and are subjected to in-plane monotonic lateral loads and vertical loads distributed on beams and columns. The frames are designed according to <xref ref-type="bibr" rid="B25">Institute American Concrete (1989)</xref> to resist lateral wind loads. The masonry infills are constructed with (92 &#xd7; 92&#x20;&#xd7; 194)&#xa0;mm<sup>3</sup> hollow and solid units in specimens 8 and 9, respectively. A type S mortar is used to connect the brick units. The joint&#x2019;s thickness is 10&#xa0;mm. According to <xref ref-type="bibr" rid="B42">Mehrabi et&#x20;al. (1996)</xref>, the compression stress of the solid units is higher than that of hollow units by 1.5 times. For the concrete, the compressive strength and the elastic modulus are 26.8 and 17225 MPa, respectively. For masonry infills, the compression strengths are 9.5 and 14.2 MPa and the elastic modulus are 5089.6 and 8233.6 MPa for specimens 8 and 9, respectively. The geometry of the infilled frame and the details of the frame elements are illustrated in <xref ref-type="fig" rid="F4">Figures&#x20;4A&#x2013;C</xref>.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Details and results of specimens 8 and 9 (units in N and mm): <bold>(A)</bold> R/C frame <bold>(B)</bold> column and beam cross-sections (units in mm) <bold>(C)</bold> brick units geometry <bold>(D)</bold> Force displacement curve <bold>(E)</bold> and <bold>(F)</bold> failure modes at the end of experimental tests (<xref ref-type="bibr" rid="B42">Mehrabi et al., (1996)</xref>).</p>
</caption>
<graphic xlink:href="fbuil-07-783051-g004.tif"/>
</fig>
<p>
<xref ref-type="fig" rid="F4">Figure&#x20;4D</xref> illustrates the force&#x2013;displacement curves obtained from the experimental test for specimens 8 and 9. <xref ref-type="fig" rid="F4">Figure&#x20;4E, F</xref> illustrates the failure modes at the end of each test, where the solid line and areas represent the cracks and the crushes, respectively. Before reaching the maximum loads, minor diagonal and sliding cracks start to develop along with the infill panel. In the case of specimen 8, the former failure modes were followed by sliding in the bed joints, and at high displacement amplitudes, crushing failure at the masonry panel occurred (<xref ref-type="fig" rid="F4">Figure&#x20;4E</xref>). In the case of specimen 9, the diagonal cracks were followed by shear cracks that appeared in the columns. These cracks are extended until the end of the test (<xref ref-type="fig" rid="F4">Figure&#x20;4F</xref>).</p>
</sec>
<sec id="s4">
<title>4 Finite Element Modeling</title>
<sec id="s4-1">
<title>4.1 Reinforced Concrete Frame Modeling</title>
<sec id="s4-1-1">
<title>4.1.1 Concrete</title>
<p>The concrete material is modeled using the SOLID65 element available in the ANSYS library. This element has cracking and crushing capabilities in case of tension or compression, respectively [<xref ref-type="bibr" rid="B4">ANSYS Mechanical APDL Element Reference (2013)</xref>].</p>
<p>The failure surface used in ANSYS for brittle materials is that proposed by <xref ref-type="bibr" rid="B67">Willam (1975)</xref>. At least four parameters are required to define the model: the shear transferring coefficients for open and closed cracks and compression and tension stresses. The limitation of <xref ref-type="bibr" rid="B67">Willam (1975)</xref>&#x2019;s model is the linear behavior, where the material behaves linearly until it is cracked or crushed [<xref ref-type="bibr" rid="B4">ANSYS (2013)</xref>]. In order to overcome this issue, the compressive stress is deactivated and replaced by non-linear stress&#x2013;strain relationships [<xref ref-type="bibr" rid="B46">Mohyeddin et&#x20;al. (2013)</xref>]. The nonlinear relationships (<xref ref-type="fig" rid="F5">Figure&#x20;5A</xref>) are obtained using the confined concrete model proposed by <xref ref-type="bibr" rid="B60">Scott et&#x20;al. (1982)</xref>, known as the modified <xref ref-type="bibr" rid="B28">Kent and Park (1971)</xref> model. In tension, the material is considered to behave linearly. The tension stress is assumed to be 10% the compressive stress [<xref ref-type="bibr" rid="B47">Mohyeddin-Kermani, (2011)</xref>]. The mechanical properties adopted for concrete are 26.8 and 17225 MPa for compressive and elastic modulus, respectively.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Adopted nonlinear Stress-strain relationships for: <bold>(A)</bold> confined concrete (Modified <xref ref-type="bibr" rid="B28">Kent and Park, 1971</xref>) <bold>(B)</bold> longitudinal reinforcements <bold>(C)</bold> masonry infill (micro-model) <bold>(D)</bold> diagonal strut (macro-model) <bold>(E)</bold> cohesive zone material (CZM) for contact pairs (<xref ref-type="bibr" rid="B4">ANSYS, 2013</xref>).</p>
</caption>
<graphic xlink:href="fbuil-07-783051-g005.tif"/>
</fig>
</sec>
<sec id="s4-1-2">
<title>4.1.2 Reinforcement</title>
<p>The reinforcements are modeled with a LINK180. This element is used to model trusses, cables, springs, and links. It has the capability to represent the tension and/or compression elements with no bending resistance [<xref ref-type="bibr" rid="B4">ANSYS Mechanical APDL Element Reference (2013)</xref>]. The nonlinear behavior of this element is defined by the bilinear behavior (<xref ref-type="fig" rid="F5">Figure&#x20;5B</xref>). The second slope (<inline-formula id="inf23">
<mml:math id="m29">
<mml:mrow>
<mml:msub>
<mml:mi>E</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>) is considered to be 2.5% of the elastic modulus (<inline-formula id="inf24">
<mml:math id="m30">
<mml:mrow>
<mml:msub>
<mml:mi>E</mml:mi>
<mml:mi>s</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>). The elastic modulus and the Poisson ratio coefficient of reinforcement are assumed to be 2e<sup>5</sup> MPa and 0.3, respectively. The yield stresses for bare sizes #2, #4, and #5 are 368, 421, and 414 MPa, respectively. While the ultimate stresses are 449, 662, and 662 MPa for bare sizes #2, #4, and #5, respectively.</p>
</sec>
</sec>
<sec id="s4-2">
<title>4.2 Masonry Infills</title>
<sec id="s4-2-1">
<title>4.2.1&#x20;Micro-Model</title>
<p>The masonry infills are modeled using the simplified micro modeling approach where the mortar thickness is halved and assigned to the adjacent unit. The element and procedure used to model the concrete material are used to model the masonry material. The tensile stress of masonry is considered to be 10% the compressive strength [<xref ref-type="bibr" rid="B47">Mohyeddin-Kermani, (2011)</xref>]. The nonlinear stress&#x2013;strain relationships (<xref ref-type="fig" rid="F5">Figure&#x20;5C</xref>) implemented in ANSYS for masonry material are calculated from <xref ref-type="bibr" rid="B21">Hendry (1990)</xref>&#x2019;s model (<xref ref-type="disp-formula" rid="e13">Eq. (13)</xref>). The strains at the peak stress are considered the same as those obtained from <xref ref-type="bibr" rid="B42">Mehrabi et&#x20;al. (1996)</xref>. The values are 0.0027 and 0.0026 for specimens 8 and 9, respectively.<disp-formula id="e13">
<mml:math id="m31">
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<mml:mn>2</mml:mn>
</mml:msup>
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</mml:mrow>
<mml:mo>,</mml:mo>
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<label>(13)</label>
</disp-formula>where, <inline-formula id="inf25">
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<mml:mi mathvariant="italic">&#x3c3;</mml:mi>
<mml:mi mathvariant="italic">m</mml:mi>
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</inline-formula> is the stress, <inline-formula id="inf26">
<mml:math id="m33">
<mml:mrow>
<mml:msubsup>
<mml:mi mathvariant="italic">f</mml:mi>
<mml:mrow>
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<mml:mi mathvariant="normal">&#x27;</mml:mi>
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</inline-formula> is the compressive stress of the masonry prism, <inline-formula id="inf27">
<mml:math id="m34">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="bold-italic">&#x3b5;</mml:mi>
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<mml:math id="m35">
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</inline-formula> is the strain at the peak stress.</p>
</sec>
<sec id="s4-2-2">
<title>4.2.2 Contact Elements</title>
<p>The frame-infill interactions and that between masonry units are modeled with contact elements. Surface-to-surface contact elements CONTA174 combined with a target element TARGE170 are used. The contact elements are used to represent the contact and sliding between two element surfaces. The elements are defined with six or eight nodes depending on the shape of the contact surface. These elements support isotropic and orthotropic Coulomb friction, shear stress friction. In ANSYS, the cohesive zone material model (CZM) is combined with contact pairs to define the separation between two elements. The CZM model (<xref ref-type="fig" rid="F5">Figure&#x20;5E</xref>) is identified by bilinear stress-separation relationships proposed by <xref ref-type="bibr" rid="B3">Alfano and Crisfield (2001)</xref>. The contact tensile and shear behaviors are illustrated in <xref ref-type="fig" rid="F5">Figure&#x20;5E</xref>. <inline-formula id="inf29">
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</inline-formula>): normal (tangential) contact stiffness. The values adopted to define the contact behaviors are those used in the study by <xref ref-type="bibr" rid="B47">Mohyeddin-Kermani, (2011)</xref>.</p>
</sec>
<sec id="s4-2-3">
<title>4.2.3 Macro- and Meso-Models</title>
<p>In the macro-modeling approach, the masonry infills are modeled with the LINK180 element from ANSYS library. This element is a 3D spar that can be used in a variety of engineering applications (<xref ref-type="bibr" rid="B4">ANSYS Mechanical APDL Element Reference (2013)</xref>). <xref ref-type="fig" rid="F6">Figure&#x20;6A</xref> illustrates the macro-modeling of masonry infills. To adapt this element as a diagonal strut, the compression-only option is activated by turning the third key option (KEYOPT (3)) to 2 (<xref ref-type="bibr" rid="B4">ANSYS Mechanical APDL Element Reference (2013)</xref>). The nonlinearity in this model is distributed along the length of the element.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>Modeling techniques of masonry infill: <bold>(A)</bold> Macro modeling <bold>(B)</bold> Meso modeling.</p>
</caption>
<graphic xlink:href="fbuil-07-783051-g006.tif"/>
</fig>
<p>In meso-modeling, the masonry infills are modeled as a single homogenized diagonal element using the SOLID65 element. The diagonal element is modeled in the same direction of the stresses and strain distributions obtained. <xref ref-type="fig" rid="F6">Figure&#x20;6B</xref> illustrates the meso-modeling of the masonry infills. The width is calculated according to <xref ref-type="disp-formula" rid="e1">Eqs. 1</xref>&#x2013;<xref ref-type="disp-formula" rid="e8">8</xref>. The frame-homogenized element contacts are modeled with bonded contacts. The procedure used to model the concrete material is implemented to model the diagonal element.</p>
<p>The mechanical properties of the diagonal elements are defined from the behavior of the masonry infill. The masonry infill response is subtracted from the behavior of the infilled frame based on the hypotheses that consider the behavior of the infilled frame as a combination of its two components frame and infill [<xref ref-type="bibr" rid="B45">Mohamed and Xavier (2018)</xref>]. This method is used by many researchers such as <xref ref-type="bibr" rid="B8">Asteris et&#x20;al. (2016)</xref>, <xref ref-type="bibr" rid="B31">Liberatore et&#x20;al. (2018)</xref>, <xref ref-type="bibr" rid="B13">De Risi et&#x20;al. (2018)</xref>, and <xref ref-type="bibr" rid="B45">Mohamed and Xavier (2018)</xref>. The infill force&#x2013;displacement curves are projected to the diagonal direction to define the stress&#x2013;strain relationships. The nonlinear behavior (<xref ref-type="fig" rid="F5">Figure&#x20;5D</xref>) is obtained by dividing the forces and displacements by the diagonal length and the cross section of the diagonal strut. The elastic modulus is defined at 45% of the maximum stress. In this study, the tensile strength is removed. For multi strut models, the models proposed by <xref ref-type="bibr" rid="B10">Chrysostomou et&#x20;al. (2002)</xref> and <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref> are used in this investigation. The behavior of the masonry infills is distributed between the diagonal and off-diagonal struts according to the method used by <xref ref-type="bibr" rid="B66">Verderame et&#x20;al. (2019)</xref>. The forces, displacements, and stiffnesses for each strut are calculated according to the equations (<xref ref-type="disp-formula" rid="e14">Eqs. (14)</xref>&#x2013;<xref ref-type="disp-formula" rid="e20">(20</xref>) proposed by <xref ref-type="bibr" rid="B10">Chrysostomou et&#x20;al. (2002)</xref>.<disp-formula id="e14">
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</mml:mrow>
</mml:mfrac>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
<label>(17)</label>
</disp-formula>
<disp-formula id="e18">
<mml:math id="m46">
<mml:mrow>
<mml:msub>
<mml:mi>F</mml:mi>
<mml:mrow>
<mml:mi>o</mml:mi>
<mml:mi>f</mml:mi>
<mml:mi>f</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:msub>
<mml:mi>F</mml:mi>
<mml:mi>d</mml:mi>
</mml:msub>
<mml:mfrac>
<mml:mrow>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mi>&#x3b3;</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:mfrac>
<mml:mfrac>
<mml:mn>1</mml:mn>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>&#x3b1;</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
<label>(18)</label>
</disp-formula>
<disp-formula id="e19">
<mml:math id="m47">
<mml:mrow>
<mml:msub>
<mml:mi>D</mml:mi>
<mml:mrow>
<mml:mi>o</mml:mi>
<mml:mi>f</mml:mi>
<mml:mi>f</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:msub>
<mml:mi>D</mml:mi>
<mml:mi>d</mml:mi>
</mml:msub>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>&#x3b1;</mml:mi>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
<label>(19)</label>
</disp-formula>
<disp-formula id="e20">
<mml:math id="m48">
<mml:mrow>
<mml:mi>&#x3b1;</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>Z</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>H</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfrac>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
<label>(20)</label>
</disp-formula>where <inline-formula id="inf35">
<mml:math id="m49">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mi mathvariant="normal">d</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>, <inline-formula id="inf36">
<mml:math id="m50">
<mml:mrow>
<mml:msub>
<mml:mi>F</mml:mi>
<mml:mi>d</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>, and <inline-formula id="inf37">
<mml:math id="m51">
<mml:mrow>
<mml:msub>
<mml:mi>D</mml:mi>
<mml:mi>d</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> are initial stiffness, force, and displacement of the masonry infill in the diagonal direction, respectively. <inline-formula id="inf38">
<mml:math id="m52">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mi mathvariant="normal">c</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> and <inline-formula id="inf39">
<mml:math id="m53">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">off</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> are the initial stiffnesses of diagonal and off-diagonal struts, respectively. <inline-formula id="inf40">
<mml:math id="m54">
<mml:mrow>
<mml:msub>
<mml:mi>D</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> and <inline-formula id="inf41">
<mml:math id="m55">
<mml:mrow>
<mml:msub>
<mml:mi>D</mml:mi>
<mml:mrow>
<mml:mi>o</mml:mi>
<mml:mi>f</mml:mi>
<mml:mi>f</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> are displacements of diagonal and off-diagonal struts. <inline-formula id="inf42">
<mml:math id="m56">
<mml:mrow>
<mml:msub>
<mml:mi>F</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> and <inline-formula id="inf43">
<mml:math id="m57">
<mml:mrow>
<mml:msub>
<mml:mi>F</mml:mi>
<mml:mrow>
<mml:mi>o</mml:mi>
<mml:mi>f</mml:mi>
<mml:mi>f</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> are the forces in the diagonal and off-diagonal struts. <inline-formula id="inf44">
<mml:math id="m58">
<mml:mrow>
<mml:msub>
<mml:mi>&#x3b3;</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the portion absorbed by the diagonal strut. <inline-formula id="inf45">
<mml:math id="m59">
<mml:mrow>
<mml:msub>
<mml:mi>Z</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the infill-column contact length.</p>
<p>The total width and the contact length in <xref ref-type="bibr" rid="B10">Chrysostomou et&#x20;al. (2002)</xref>&#x2019;s model are calculated using <xref ref-type="disp-formula" rid="e21">Eq. (21)</xref> [<xref ref-type="bibr" rid="B31">Liberatore et&#x20;al. (2018)</xref>] and <xref ref-type="disp-formula" rid="e22">Eq. (22)</xref> [<xref ref-type="bibr" rid="B31">Stafford Smith (1976)</xref>]. The axial stiffness is obtained from the subtracted response of the infill masonry at 45% of the maximum load. Meanwhile, <xref ref-type="disp-formula" rid="e9">Eq. (9</xref>) and <xref ref-type="disp-formula" rid="e12">(12</xref>) are used to determine the width and the contact length in <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref>&#x2019;s model. The absorbed portion (<inline-formula id="inf46">
<mml:math id="m60">
<mml:mrow>
<mml:msub>
<mml:mi>&#x3b3;</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>) is considered to be 35 and 33% for the models of <xref ref-type="bibr" rid="B10">Chrysostomou et&#x20;al. (2002)</xref> and <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref>, respectively.<disp-formula id="e21">
<mml:math id="m61">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="italic">K</mml:mi>
<mml:mi mathvariant="italic">d</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>E</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
<mml:mi>t</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>d</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfrac>
<mml:mi mathvariant="italic">w,</mml:mi>
</mml:mrow>
</mml:math>
<label>(21)</label>
</disp-formula>
<disp-formula id="e22">
<mml:math id="m62">
<mml:mrow>
<mml:msub>
<mml:mi>Z</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mi>&#x3c0;</mml:mi>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:msub>
<mml:mi>&#x3bb;</mml:mi>
<mml:mi>h</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfrac>
<mml:mi>h</mml:mi>
</mml:mrow>
</mml:math>
<label>(22)</label>
</disp-formula>
</p>
<p>
<xref ref-type="table" rid="T1">Table&#x20;1</xref> summarizes the width strut values obtained for specimens 8 and 9. As can be observed, similar values are presented in both specimens by using the models of <xref ref-type="bibr" rid="B22">Holmes (1961)</xref> and <xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref> because the width models are only related to the geometric properties. Otherwise, the other models indicate diverse values. The values obtained from the expression of <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref> represent the width of an off-diagonal strut. The width of the diagonal strut represents 50% of the presented&#x20;value.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Strut width values for specimen 8&#x2013;9 (units in mm).</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Author</th>
<th align="center">Specimen 8</th>
<th align="center">Specimen 9</th>
<th align="center">Number of strut (s)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">
<xref ref-type="bibr" rid="B22">Holmes (1961)</xref>
</td>
<td align="center">855</td>
<td align="center">855</td>
<td align="center">1</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B38">Mainstone (1974a)</xref>
</td>
<td align="center">167</td>
<td align="center">159</td>
<td align="center">1</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref>
</td>
<td align="center">552</td>
<td align="center">520</td>
<td align="center">1</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref>
</td>
<td align="center">463</td>
<td align="center">413</td>
<td align="center">1</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref>
</td>
<td align="center">427</td>
<td align="center">427</td>
<td align="center">1</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B65">Turgay et&#x20;al. (2014)</xref>
</td>
<td align="center">323</td>
<td align="center">314</td>
<td align="center">1</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref>
</td>
<td align="center">92</td>
<td align="center">87</td>
<td align="center">3</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</sec>
</sec>
<sec sec-type="results|discussion" id="s5">
<title>5 Results and Discussion</title>
<p>The results obtained from this analytical study are presented and discussed in this section. The dissection is split into two phases: 1) before reaching the maximum lateral load and 2) after reaching the maximum lateral load. Before the peak load, the results are compared in terms of maximum force (<inline-formula id="inf47">
<mml:math id="m63">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">F</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">max</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>), initial stiffness (<inline-formula id="inf48">
<mml:math id="m64">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">in</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>), and stiffness at the peak load (<inline-formula id="inf49">
<mml:math id="m65">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">peak</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>), where the initial stiffness is defined at 45% of the maximum load. The second comparison is based on the behavior of each model after the force reaches its maximum value<bold>.</bold>
</p>
<sec id="s5-1">
<title>5.1&#x20;Micro-Model Results</title>
<p>
<xref ref-type="fig" rid="F7">Figures&#x20;7A,B</xref> compare the experimental and FE force&#x2013;displacement curves for specimens 8 and 9, respectively. It is clearly shown that the numerical model can predict the force and the stiffness of the infilled frames in both specimens. The deformation shapes of FE analyses are illustrated in <xref ref-type="fig" rid="F7">Figure&#x20;7C, D</xref> for specimens 8 and 9, respectively. In numerical results, the cracks are presented as the separation between two different elements (units-frame elements or units-units). As indicated at the end of the experimental tests, different failure modes (shear sliding, diagonal cracking, minor compression crushing, damage within masonry wedge, and cracks in windward and leeward columns) are observed in specimen 8 (with weak infill). On the other hand, diagonal cracks, shear sliding of bed joints, crushing of masonry, and windward column are observed in specimen 9 (with strong infill). The numerical model presents only separations along bed joints which represent the shear sliding mode. Otherwise, the deformation shape obtained from specimen 9 presents diagonal and horizontal separations between masonry units which represent the diagonal cracking and the shear sliding compared to the experimental failure. The numerical models fail to represent the diagonal cracking in specimen 8 and crushing damages in both specimens.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Results obtained from micro modeling: <bold>(A)</bold> <bold>(B)</bold> force-displacement curve comparison between experimental and numerical micro model specimens 8 and 9 <bold>(C)</bold> <bold>(D)</bold> deformation shapes of specimen 8 and 9 (units in N/mm).</p>
</caption>
<graphic xlink:href="fbuil-07-783051-g007.tif"/>
</fig>
<p>The diagonal distributions of the stresses and the strains in the infilled frames, when the systems reach their peak strength, are illustrated in <xref ref-type="fig" rid="F8">Figure&#x20;8</xref>. The diagonal distribution resulted in stress concentration in the top and bottom corners of windward and leeward columns, respectively. The figure also indicates that the distributions of the stresses and strains along the beam-infill contact are longer than the column-infill contact length; this is due to the vertical loads applied on the&#x20;beam.</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>Distribution of stresses and strains: <bold>(A)</bold> <bold>(B)</bold> specimen 8 <bold>(C)</bold> <bold>(D)</bold> specimen 9.</p>
</caption>
<graphic xlink:href="fbuil-07-783051-g008.tif"/>
</fig>
</sec>
<sec id="s5-2">
<title>5.2 Macro- and Meso-Models</title>
<sec id="s5-2-1">
<title>5.2.1 Before the Maximum Load</title>
<p>
<xref ref-type="table" rid="T2">Tables 2</xref>&#x2013;<xref ref-type="table" rid="T4">4</xref> summarize the analytical results before the curves reach maximum lateral force in each model. The micro-model results are presented in the first row. Since the force&#x2013;displacement curves obtained from modeling the diagonal strut with an axial element are the same, the results are summarized in the second row. Otherwise, the other rows outline results obtained from meso-modeling.</p>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>The results obtained from modeling specimen 8.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Modeling method</th>
<th align="center">Strut models</th>
<th align="center">
<inline-formula id="inf50">
<mml:math id="m66">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">F</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">max</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (KN)</th>
<th align="center">
<inline-formula id="inf51">
<mml:math id="m67">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">initial</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (KN/m)</th>
<th align="center">
<inline-formula id="inf52">
<mml:math id="m68">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">peak</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (KN/m)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Micro-model</td>
<td align="left">&#x2014;</td>
<td align="center">184</td>
<td align="char" char=".">54.5</td>
<td align="char" char=".">9.10</td>
</tr>
<tr>
<td align="left">Macro-model</td>
<td align="left">All models</td>
<td align="center">183</td>
<td align="char" char=".">102</td>
<td align="char" char=".">27.5</td>
</tr>
<tr>
<td rowspan="6" align="left">Meso-model</td>
<td align="left">
<xref ref-type="bibr" rid="B22">Holmes (1961)</xref>
</td>
<td align="center">160</td>
<td align="char" char=".">81.2</td>
<td align="char" char=".">18.0</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B38">Mainstone (1974a)</xref>
</td>
<td align="center">177</td>
<td align="char" char=".">75.3</td>
<td align="char" char=".">19.1</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref>
</td>
<td align="center">170</td>
<td align="char" char=".">77.9</td>
<td align="char" char=".">17.6</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref>
</td>
<td align="center">172</td>
<td align="char" char=".">78.2</td>
<td align="char" char=".">18.3</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref>
</td>
<td align="center">173</td>
<td align="char" char=".">78.1</td>
<td align="char" char=".">18.7</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B65">Turgay et&#x20;al. (2014)</xref>
</td>
<td align="center">175</td>
<td align="char" char=".">78.2</td>
<td align="char" char=".">18.9</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="T3" position="float">
<label>TABLE 3</label>
<caption>
<p>The results obtained from modeling specimen 9.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Modeling method</th>
<th align="center">Strut models</th>
<th align="center">
<inline-formula id="inf53">
<mml:math id="m69">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">F</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">max</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (KN)</th>
<th align="center">
<inline-formula id="inf54">
<mml:math id="m70">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">initial</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (KN/m)</th>
<th align="center">
<inline-formula id="inf55">
<mml:math id="m71">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">peak</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (KN/m)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Micro-model</td>
<td align="left">&#x2014;</td>
<td align="center">292</td>
<td align="char" char=".">207</td>
<td align="char" char=".">33.6</td>
</tr>
<tr>
<td align="left">Macro-model</td>
<td align="left">All models</td>
<td align="center">297</td>
<td align="char" char=".">115</td>
<td align="char" char=".">20.9</td>
</tr>
<tr>
<td rowspan="6" align="left">Meso-model</td>
<td align="left">
<xref ref-type="bibr" rid="B22">Holmes (1961)</xref>
</td>
<td align="center">288</td>
<td align="char" char=".">90.8</td>
<td align="char" char=".">33.8</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B38">Mainstone (1974a)</xref>
</td>
<td align="center">273</td>
<td align="char" char=".">88.8</td>
<td align="char" char=".">32.5</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref>
</td>
<td align="center">265</td>
<td align="char" char=".">95.0</td>
<td align="char" char=".">30.6</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref>
</td>
<td align="center">270</td>
<td align="char" char=".">93.3</td>
<td align="char" char=".">32.1</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref>
</td>
<td align="center">269</td>
<td align="char" char=".">93.3</td>
<td align="char" char=".">32.0</td>
</tr>
<tr>
<td align="left">
<xref ref-type="bibr" rid="B65">Turgay et&#x20;al. (2014)</xref>
</td>
<td align="center">272</td>
<td align="char" char=".">92.1</td>
<td align="char" char=".">32.4</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="T4" position="float">
<label>TABLE 4</label>
<caption>
<p>The results of the multi-strut&#x20;model.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th rowspan="3" align="left">Models</th>
<th rowspan="2" align="center">Modeling method</th>
<th colspan="3" align="center">Specimen 8</th>
<th colspan="3" align="center">Specimen 9</th>
</tr>
<tr>
<th align="center">
<inline-formula id="inf56">
<mml:math id="m72">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">F</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">max</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (KN)</th>
<th align="center">
<inline-formula id="inf57">
<mml:math id="m73">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">initial</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (KN/m)</th>
<th align="center">
<inline-formula id="inf58">
<mml:math id="m74">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">peak</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (KN/m)</th>
<th align="center">
<inline-formula id="inf59">
<mml:math id="m75">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">F</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">max</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (KN)</th>
<th align="center">
<inline-formula id="inf60">
<mml:math id="m76">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">initial</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (KN/m)</th>
<th align="center">
<inline-formula id="inf61">
<mml:math id="m77">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">K</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">peak</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (KN/m)</th>
</tr>
<tr>
<th align="center">Micro-model</th>
<th align="center">184</th>
<th align="center">54.5</th>
<th align="center">9.10</th>
<th align="center">292</th>
<th align="center">207</th>
<th align="center">33.6</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td rowspan="2" align="left">
<xref ref-type="bibr" rid="B10">Chrysostomou et&#x20;al. (2002)</xref>
</td>
<td align="left">Meso-model</td>
<td align="center">179</td>
<td align="char" char=".">71.0</td>
<td align="char" char=".">14.5</td>
<td align="center">278</td>
<td align="char" char=".">79.5</td>
<td align="char" char=".">18.4</td>
</tr>
<tr>
<td align="left">Macro-model</td>
<td align="center">179</td>
<td align="char" char=".">58.0</td>
<td align="char" char=".">11.0</td>
<td align="center">250</td>
<td align="char" char=".">69.7</td>
<td align="char" char=".">13.3</td>
</tr>
<tr>
<td rowspan="2" align="left">
<xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref>
</td>
<td align="left">Meso-model</td>
<td align="center">197</td>
<td align="char" char=".">83.6</td>
<td align="char" char=".">18.2</td>
<td align="center">261</td>
<td align="char" char=".">84.1</td>
<td align="char" char=".">26.3</td>
</tr>
<tr>
<td align="left">Macro-model</td>
<td align="center">203</td>
<td align="char" char=".">69.4</td>
<td align="char" char=".">16.8</td>
<td align="center">272</td>
<td align="char" char=".">72.0</td>
<td align="char" char=".">25.5</td>
</tr>
</tbody>
</table>
</table-wrap>
<sec id="s5-2-1-1">
<title>5.2.1.1 Specimen 8</title>
<p>As indicated in <xref ref-type="table" rid="T2">Table&#x20;2</xref>, the micro-model gives good approximation in terms of force. The micro-model underestimates the experimental lateral force (184 KN) of the infilled frame by 2.8%. In terms of initial stiffness, the calculated stiffness is 54.5&#xa0;KN/mm which represents 0.8 the experimental value. The experimental stiffness at peak force is 1.5&#x20;times higher than that obtained from the micro-model. By modeling the masonry infill with the macro-model, the maximum force (183&#xa0;KN) is reached at a displacement of 6.77&#xa0;mm. This model gives stiffness, at peak force, the value that is 2&#x20;times higher than that of the experimental. In the case of the initial stiffness, the numerical model shows a value 1.5&#x20;times higher than that of the experimental.</p>
<p>The results obtained from meso-modeling indicate that the width models of <xref ref-type="bibr" rid="B22">Holmes (1961)</xref> and <xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref> show higher errors than the other models; the models underestimate the lateral force by 15.3 and 10%, respectively. In terms of initial stiffness, the models show differences of 17.6 and 12.8%, respectively. The numerical stiffness at the peak load is 1.1 higher than the experimental values for both models. Using the model proposed by <xref ref-type="bibr" rid="B39">Mainstone R. J.&#x20;(1974)</xref>, the maximum lateral force is more approximate to the experimental value. The lateral force is 177&#xa0;KN which is 6.2% lower than that of the experimental value. While the initial stiffnesses and the stiffness at the peak force are 1.1 and 1.4&#x20;times higher.</p>
<p>The maximum forces record from <xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref>&#x2019;s, and <xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref>&#x2019;s models are lower by around 8% than that in the experimental test. The difference is reduced to 7% in case of using the model of <xref ref-type="bibr" rid="B65">Turgay et&#x20;al. (2014)</xref>. The initial stiffness is overestimated by around 13% in the models of <xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref> and <xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref> and <xref ref-type="bibr" rid="B65">Turgay et&#x20;al. (2014)</xref>, while the stiffness at the peak force is 1.13&#x20;times the experimental&#x20;value.</p>
</sec>
<sec id="s5-2-1-2">
<title>5.2.1.2 Specimen 9</title>
<p>The width models used to model specimen 8 are used for specimen 9. The results obtained from the numerical analyses are summarized in <xref ref-type="table" rid="T3">Table&#x20;3</xref>. As presented, the micro model results overestimate the lateral force by 0.12%. The maximum force that reached at a displacement 8.68&#xa0;mm implies a difference of 16% in the stiffness at the peak load compared to the experimental value. However, the numerical initial stiffness is 2.3&#x20;times higher.</p>
<p>Using macro-models, the numerical force is 297&#xa0;KN, which reached at a displacement of 14.2&#xa0;mm. The stiffness obtained at the peak force is around 2&#x20;times lower than the experimental value. In terms of initial stiffness, the numerical value is 28% lower. Using meso-modeling, the width models proposed by <xref ref-type="bibr" rid="B22">Holmes (1961)</xref> show the approximate lateral force (1%) compared to the other width models. The initial stiffness is overestimated by 1.6%. Meanwhile, the stiffness at the peak load is underestimated by 16%. In terms of lateral force, the models of <xref ref-type="bibr" rid="B38">Mainstone RJ.&#x20;(1974)</xref> and <xref ref-type="bibr" rid="B65">Turgay et&#x20;al. (2014)</xref> show a difference of 6%. This difference is decreased to around 7.5% by using <xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref>&#x2019;s and <xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref>&#x2019;s models. The higher difference is obtained from using <xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref>&#x2019;s model&#x20;(9%).</p>
<p>In terms of initial stiffness, the model of <xref ref-type="bibr" rid="B39">Mainstone R. J.&#x20;(1974)</xref> gives the approximate value where a difference of 0.5% is obtained. The models of <xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref> and <xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref> overestimate the initial stiffness by 4.5%. A higher value is obtained by <xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref>. The model of <xref ref-type="bibr" rid="B65">Turgay et&#x20;al. (2014)</xref> shows a value of 92.1&#xa0;KN/m. In terms of stiffness at the peak load, the models of <xref ref-type="bibr" rid="B22">Holmes (1961)</xref>, <xref ref-type="bibr" rid="B38">Mainstone RJ.&#x20;(1974</xref>, <xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref>, <xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref>, <xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref>, and <xref ref-type="bibr" rid="B65">Turgay et&#x20;al. (2014)</xref> are 15.5, 19, 23.5, 20, 20, and 19%, respectively.</p>
<p>The results obtained from modeling the masonry infills with three-strut models are presented in <xref ref-type="table" rid="T4">Table&#x20;4</xref>. In terms of maximum lateral force, the values obtained from macro-modeling [<xref ref-type="bibr" rid="B10">Chrysostomou et&#x20;al. (2002)</xref>&#x2019;s model] are 179&#xa0;KN and 250&#xa0;KN for specimen 8 and 9, respectively. The values underestimated the experimental force by 5 and 14%, respectively. Using <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref>&#x2019;s model, the lateral strength is overestimated by 7% in specimen 8 and underestimated in specimen 9 by 6%. In meso-modeling, the errors are around 5% using <xref ref-type="bibr" rid="B10">Chrysostomou et&#x20;al. (2002)</xref>&#x2019;s model. Meanwhile, in <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref>&#x2019;s model, the differences between experimental end numerical results are 4 and 10% for specimen 8 and 9, respectively.</p>
<p>In terms of stiffness, both models overestimate the initial stiffness and stiffness at the peak load of the specimen 8 with difference varying between 0.5 and 35%; only in macro-modeling of <xref ref-type="bibr" rid="B10">Chrysostomou et&#x20;al. (2002)</xref>&#x2019;s model, the stiffnesses are underestimated by 19 and 16%, respectively. In specimen 9, the numerical stiffnesses underestimated experimental values with difference varying between 8 and&#x20;67%.</p>
</sec>
</sec>
<sec id="s5-2-2">
<title>5.2.2&#x20;Post-peak Behavior</title>
<p>
<xref ref-type="fig" rid="F9">Figures&#x20;9</xref>&#x2013;<xref ref-type="fig" rid="F11">11</xref> illustrate the force&#x2013;displacement curves obtained from numerical analyses. In <xref ref-type="fig" rid="F11">Figure&#x20;11</xref>, the results obtained from <xref ref-type="bibr" rid="B10">Chrysostomou et&#x20;al. (2002)</xref> are presented in green color, and the blue color represents the results of using <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref>. In general, the lateral force decreases when the peak force is reached for all numerical models. In the micro-model, the numerical model of specimen 8 presents a slight decrease compared to the experimental curve where the numerical curve records a reduction of 6% while the experimental decreasing is around 20% at the end of the test. However, the numerical results of specimen 9 show a significant decrease in the lateral force. The numerical force is dropped to 39% of the maximum load whereas the experimental results show a reduction of&#x20;19%.</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>Comparison between experimental and numerical macro models for specimen 8: <bold>(A)</bold> <xref ref-type="bibr" rid="B22">Holmes (1961)</xref> <bold>(B)</bold> Mainstone (1974) <bold>(C)</bold> <xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref> <bold>(D)</bold> <xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref> <bold>(E)</bold> <xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref> <bold>(F)</bold> <xref ref-type="bibr" rid="B65">Turgay et al. (2014)</xref>.</p>
</caption>
<graphic xlink:href="fbuil-07-783051-g009.tif"/>
</fig>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>Comparison between experimental and numerical macro models for specimen 9: <bold>(A)</bold> <xref ref-type="bibr" rid="B22">Holmes (1961)</xref> <bold>(B)</bold> Mainstone (1974) <bold>(C)</bold> <xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref> <bold>(D)</bold> <xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref> <bold>(E)</bold> <xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref> <bold>(F)</bold> <xref ref-type="bibr" rid="B65">Turgay et al. (2014)</xref>.</p>
</caption>
<graphic xlink:href="fbuil-07-783051-g010.tif"/>
</fig>
<fig id="F11" position="float">
<label>FIGURE 11</label>
<caption>
<p>Comparison between experimental and multi-strut models: <bold>(A)</bold> Specimen 8 <bold>(B)</bold> Specimen 9.</p>
</caption>
<graphic xlink:href="fbuil-07-783051-g011.tif"/>
</fig>
<p>In macro- and meso-models, the curves obtained from analyzing specimen 8 (<xref ref-type="fig" rid="F9">Figure&#x20;9</xref>) show approximate behavior after the lateral load reaches its maximum value compared to the experimental and micro-model results. The same note can be observed in specimen 9 (<xref ref-type="fig" rid="F10">Figure&#x20;10</xref>). The lateral forces at the end of analyses are approximately the same as the experimental values, 150&#xa0;KN in specimen 8 and 237&#xa0;KN in specimen 9. The lateral forces are reduced by 19% in both specimens.</p>
</sec>
</sec>
</sec>
<sec id="s6">
<title>6 Conclusion</title>
<p>This work contains a numerical investigation on the accuracy of width strut models using meso-modeling. The homogenized concept is used to model the masonry infill as a diagonal element. In addition, the work contains a comparison between micro-, meso-, and macro-modeling techniques of infills surrounded by reinforced concrete frames using the finite element software ANSYS. Two experimental specimens with weak and strong infill panels subjected to monotonic increasing lateral loading are selected to calibrate the numerical&#x20;study.</p>
<p>First, seven width models are selected. The variation of the strut width equation according to the relative stiffness indicates that the selected equations can be classified according to the relative stiffness to dependent and independent equations. The dependent equations show constant width values during the variation of the relative stiffness. Otherwise, the independent equations show a reduction of width values during the increase of the relative stiffness.</p>
<p>Next, the masonry is modeled using a simplified micro-model. The global responses of the infilled frames of the experimental test are well predicted using the simplified micro-modeling approach (in terms of strength and stiffness). The deformation shapes of the numerical models can capture the shear sliding in specimen 8. While in specimen 9, the numerical model can capture the diagonal and sliding cracks. In macro-modeling, the masonry infills are modeled using a 3D spar, known as LINK180. In meso-modeling, the masonry infills are modeled as an equivalent homogenized diagonal element using SOLID65. The width is calculated according to the models used in macro-models.</p>
<p>In general, the macro-modeling with a single-strut model indicates the capability of the single strut to capture the global behavior of the infill frames. The force-deformation curves obtained from different macro-modeling show the same curve. Using meso-modeling, the single-strut models are more predictable to the global response by using <xref ref-type="bibr" rid="B39">Mainstone R. J.&#x20;(1974)</xref> and <xref ref-type="bibr" rid="B65">Turgay et&#x20;al. (2014)</xref>&#x2019;s models in specimens 8 and 9. The model of <xref ref-type="bibr" rid="B22">Holmes (1961)</xref> gives the approximate behavior in specimen 9 compared to other models. Moreover, the models of <xref ref-type="bibr" rid="B30">Liauw and Kwan (1984)</xref>, <xref ref-type="bibr" rid="B14">Decanini and Fantin (1986)</xref>, and <xref ref-type="bibr" rid="B44">Moghaddam and Dowling (1988)</xref> show acceptable results. In the case of the multi-strut model, the models of <xref ref-type="bibr" rid="B10">Chrysostomou et&#x20;al. (2002)</xref> and <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref> show approximate behavior using meso- and macro-modeling techniques. The models underestimate the lateral behavior of infill masonry in both modeling techniques, except for the model of <xref ref-type="bibr" rid="B68">Yekrangnia and Mohammadi (2017)</xref> where the behavior is overestimated in specimen 8 using meso- and macro-modeling. Finally, the modeling of the diagonal strut (s) with the meso-modeling technique presents an acceptable tool to study the diagonal behaving infill masonry. Further works are needed to investigate the application of the meso-modeling technique on infilled frames subjected to cyclic loading.</p>
</sec>
</body>
<back>
<sec id="s7">
<title>Data Availability Statement</title>
<p>The original contributions presented in the study are included in the article/Supplementary Material, further inquiries can be directed to the corresponding author.</p>
</sec>
<sec id="s8">
<title>Author Contributions</title>
<p>MB was responsible for writing, methodology, software, and validation. ZB carried out the methodology, writing, and supervision.</p>
</sec>
<sec sec-type="COI-statement" id="s9">
<title>Conflict of Interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="s10">
<title>Publisher&#x2019;s Note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors, and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
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