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<article article-type="research-article" dtd-version="1.1" specific-use="sps-1.7" xml:lang="en" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">
	<front>
		<journal-meta>
			<journal-id journal-id-type="publisher-id">dyna</journal-id>
			<journal-title-group>
				<journal-title>DYNA</journal-title>
				<abbrev-journal-title abbrev-type="publisher">Dyna rev.fac.nac.minas</abbrev-journal-title>
			</journal-title-group>
			<issn pub-type="ppub">0012-7353</issn>
			<publisher>
				<publisher-name>Universidad Nacional de Colombia</publisher-name>
			</publisher>
		</journal-meta>
		<article-meta>
			<article-id pub-id-type="doi">10.15446/dyna.v85n207.71892</article-id>
			<article-categories>
				<subj-group subj-group-type="heading">
					<subject>Artículos</subject>
				</subj-group>
			</article-categories>
			<title-group>
				<article-title>Experimental assessment of I-shaped steel beams with longitudinal stiffeners under lateral-torsional buckling</article-title>
				<trans-title-group xml:lang="es">
					<trans-title>Evaluación experimental de vigas de acero en I con rigidizadores longitudinales ante el pandeo lateral torsional</trans-title>
				</trans-title-group>
			</title-group>
			<contrib-group>
				<contrib contrib-type="author">
					<name>
						<surname>Prado</surname>
						<given-names>Néstor I.</given-names>
					</name>
					<xref ref-type="aff" rid="aff1"><sup>
 <italic>a</italic>
</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Carrillo</surname>
						<given-names>Julián</given-names>
					</name>
					<xref ref-type="aff" rid="aff2"><sup>
 <italic>b</italic>
</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Ospina</surname>
						<given-names>Gustavo A.</given-names>
					</name>
					<xref ref-type="aff" rid="aff1"><sup>
 <italic>a</italic>
</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Ramirez-Amaya</surname>
						<given-names>Dario</given-names>
					</name>
					<xref ref-type="aff" rid="aff1"><sup>
 <italic>a</italic>
</sup></xref>
				</contrib>
			</contrib-group>
			<aff id="aff1">
				<label>a</label>
				<institution content-type="original"> Facultad de Ingeniería Civil, Universidad Pontificia Bolivariana, Bucaramanga, Colombia. nestor.prado@upb.edu.co, gustavo.ospina@upb.edu.co dario.ramirez@upb.edu.co </institution>
				<institution content-type="normalized">Universidad Pontificia Bolivariana</institution>
				<institution content-type="orgdiv1">Facultad de Ingeniería Civil</institution>
				<institution content-type="orgname">Universidad Pontificia Bolivariana</institution>
				<addr-line>
					<city>Bucaramanga</city>
				</addr-line>
				<country country="CO">Colombia</country>
				<email>nestor.prado@upb.edu.co</email>
				<email>gustavo.ospina@upb.edu.co</email>
				<email>dario.ramirez@upb.edu.co</email>
			</aff>
			<aff id="aff2">
				<label>b</label>
				<institution content-type="original"> Departamento de Ingeniería Civil, Universidad Militar Nueva Granada, Bogotá, Colombia. wjcarrillo@gmail.com</institution>
				<institution content-type="normalized">Universidad Militar Nueva Granada</institution>
				<institution content-type="orgdiv1">Departamento de Ingeniería Civil</institution>
				<institution content-type="orgname">Universidad Militar Nueva Granada</institution>
				<addr-line>
					<city>Bogotá</city>
				</addr-line>
				<country country="CO">Colombia</country>
			</aff>
			<pub-date pub-type="epub-ppub">
				<season>Oct-Dec</season>
				<year>2018</year>
			</pub-date>
			<volume>85</volume>
			<issue>207</issue>
			<fpage>278</fpage>
			<lpage>287</lpage>
			<history>
				<date date-type="received">
					<day>25</day>
					<month>04</month>
					<year>2018</year>
				</date>
				<date date-type="rev-recd">
					<day>16</day>
					<month>11</month>
					<year>2018</year>
				</date>
				<date date-type="accepted">
					<day>30</day>
					<month>11</month>
					<year>2018</year>
				</date>
			</history>
			<permissions>
				<license license-type="open-access" xlink:href="https://creativecommons.org/licenses/by-nc-nd/4.0/" xml:lang="en">
					<license-p>This is an open-access article distributed under the terms of the Creative Commons Attribution License</license-p>
				</license>
			</permissions>
			<abstract>
				<title>Abstract</title>
				<p>This study focused on the experimental assessment of the behavior of I-shaped steel beams with longitudinal stiffeners under the action of lateral-torsional buckling. Thirty-three IPE-140 steel beams with and without longitudinal stiffeners were tested under simple-support conditions with a laterally unbraced length ranging from 0.69 to 6.0 m. The stiffeners spacing was 0.42 m, which represented three times the depth of the section. The structural behavior of the beams is discussed in terms of their flexural capacity, the lateral displacement of the compression flange and the failure twist angle. The results showed that the use of longitudinal stiffeners increased the flexural capacity up to 82%, decreased the lateral displacement of the compression flange and the failure twist angle up to 72 and 90% respectively, with respect to the specimens without stiffeners.</p>
			</abstract>
			<trans-abstract xml:lang="es">
				<title>Resumen</title>
				<p>Este estudio se enfocó en la evaluación experimental del comportamiento de vigas de acero de sección en I con rigidizadores longitudinales bajo la acción del pandeo lateral torsional. Treinta y tres (33) vigas de acero IPE-140 simplemente apoyadas con y sin rigidizadores longitudinales fueron ensayadas con una longitud no soportada lateralmente de 0.69 a 6.0 m. El espaciamiento de los rigidizadores fue de 0.42 m, que representó tres veces el peralte de la sección. El comportamiento estructural de las vigas se analizó en términos de su capacidad a flexión, el desplazamiento lateral del patín a compresión y el ángulo de giro de falla. Los resultados indicaron que el uso de rigidizadores longitudinales aumentó la capacidad a flexión hasta un 82% y disminuyó el desplazamiento lateral del patín a compresión y el ángulo de giro de falla hasta un 72 y 90% respectivamente, con respecto a los especímenes sin rigidizadores.</p>
			</trans-abstract>
			<kwd-group xml:lang="en">
				<title><bold>
 <italic>Keywords</italic>:</bold></title>
				<kwd>longitudinal stiffeners</kwd>
				<kwd>lateral-torsional buckling</kwd>
				<kwd>lateral displacement</kwd>
				<kwd>laterally unbraced length</kwd>
				<kwd>I-shaped beam</kwd>
				<kwd>failure twist angle</kwd>
				<kwd>flexural capacity</kwd>
			</kwd-group>
			<kwd-group xml:lang="es">
				<title><bold>
 <italic>Palabras clave</italic>:</bold></title>
				<kwd>rigidizadores longitudinales</kwd>
				<kwd>pandeo lateral torsional</kwd>
				<kwd>desplazamiento lateral</kwd>
				<kwd>longitud no soportada lateralmente</kwd>
				<kwd>vigas I</kwd>
				<kwd>ángulo de giro de falla</kwd>
				<kwd>capacidad a flexión</kwd>
			</kwd-group>
			<counts>
				<fig-count count="18"/>
				<table-count count="4"/>
				<equation-count count="7"/>
				<ref-count count="23"/>
				<page-count count="10"/>
			</counts>
		</article-meta>
	</front>
	<body>
		<sec sec-type="intro">
			<title>1. Introduction</title>
			<p>In past decades, numerous experimental and numerical investigations on I-shape steel beams with stiffeners have been carried out to improve their behavior to lateral-torsional buckling. Hotchkiss [<xref ref-type="bibr" rid="B1">1</xref>] studied the behavior of I-shaped steel beams with longitudinal stiffeners at the ends only as shown in <xref ref-type="fig" rid="f1">Fig. 1</xref>a. This type of stiffeners and the use of welded plates perpendicular to the flange and web at the beam ends were evaluated by Vacharajittiphan and Trahair [<xref ref-type="bibr" rid="B2">2</xref>,<xref ref-type="bibr" rid="B3">3</xref>]. Plum and Svensson [<xref ref-type="bibr" rid="B4">4</xref>] nalytically studied the resistance of lateral-torsional buckling of I-shaped steel beams with box-type stiffeners welded to web and flanges of sections as shown in <xref ref-type="fig" rid="f1">Fig. 1</xref>b.</p>
			<p>
				<fig id="f1">
					<label>Figure 1</label>
					<caption>
						<title>Type of stiffeners. a) Longitudinal stiffeners, b) Box stiffeners, c) Transversal stiffeners, d) Cross stiffeners, e) Diagonal stiffeners.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gf1.png"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>Szewczak et al. [<xref ref-type="bibr" rid="B5">5</xref>] evaluated numerically the effectiveness of longitudinal, box-type, transversal, and cross stiffeners as shown in <xref ref-type="fig" rid="f1">Fig. 1</xref>a-<xref ref-type="fig" rid="f1">1</xref>d. This study showed that the box-type stiffener was the most efficient, whereas the transversal stiffener was the least efficient in terms of lateral-torsional buckling. Smith [<xref ref-type="bibr" rid="B6">6</xref>] studied the same aforementioned four types of stiffeners, including the effect of using cross stiffeners on both sides of the web, on only one side and alternated. Ojalvo [<xref ref-type="bibr" rid="B7">7</xref>,<xref ref-type="bibr" rid="B8">8</xref>] assessed the use of channels as stiffeners with the web of the channel parallel to the web of the beam, resembling a box-type stiffener. This type of stiffener was evaluated by Heins and Potocko [<xref ref-type="bibr" rid="B9">9</xref>], who presented two analytical methods that included one with rigorous assumptions and the other with approximations.</p>
			<p>Ojalvo and Chambers [<xref ref-type="bibr" rid="B10">10</xref>] studied the effect of box-type stiffeners located only at the ends of the beam. In addition, these authors evaluated the behavior of diagonal stiffeners as shown in <xref ref-type="fig" rid="f1">Fig. 1</xref>e. The lateral buckling of the I-shaped steel beams with longitudinal and transverse stiffeners arranged arbitrarily were demonstrated theoretical and experimentally by Takabatake [<xref ref-type="bibr" rid="B11">11</xref>] and Takabatake et al. [<xref ref-type="bibr" rid="B12">12</xref>], respectively.</p>
			<p>The aforementioned studies concluded that the box-type, longitudinal, diagonal, and cross stiffeners have improved the behavior to the lateral-torsional buckling of I-shaped steel beams. However, the literature review showed that the assessment of the flexural capacity of I-shaped steel beams have not been carried out with different laterally unbraced lengths (<italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> ). Recently, other authors studied the effect of stiffeners in other types of structural elements.</p>
			<p>Erdal [<xref ref-type="bibr" rid="B13">13</xref>] evaluated the use of stiffeners to optimize the behavior in perforated steel beams. Zarsav et al. [<xref ref-type="bibr" rid="B14">14</xref>] assessed the contributions of supplemental stiffeners on the hysteretic behavior of the link-to-column connection. Stavridou et al. [<xref ref-type="bibr" rid="B15">15</xref>] analyzed the structural response of steel wind towers with internal stiffeners. Shaterzadeh and Foroutan [<xref ref-type="bibr" rid="B16">16</xref>] evaluated the post-buckling response of cylindrical shells with spiral stiffeners and Rahmzadeh et al. [<xref ref-type="bibr" rid="B17">17</xref>] studied the effect of the rigidity and arrangement of stiffeners on the buckling behavior of plates.</p>
			<p>Therefore, this work focuses on the experimental evaluation of the flexural capacity improvement of I-shaped steel beams with longitudinal stiffeners and different laterally unbraced lengths (<italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> ). This type of stiffener is chosen for economy and constructive ease, especially in countries where to do this type of work, is better option (economic manpower) than to use an I-shaped steel beam bigger.</p>
			<p>The expected improvement is evaluated in terms of the measured flexural capacity, the lateral displacement of the compression flange, and the failure twist angle of the specimens. These aspects are beneficial for the design of steel beams of large span lateral unbraced, e.g. industrial building roofs.</p>
		</sec>
		<sec>
			<title>2. Experimental program</title>
			<p>The experimental program of this research was carried out in a loading frame at the Universidad Pontificia Bolivariana in Bucaramanga, Colombia. Thirty-three (33) IPE-140 steel beams were tested to bending. Dimensions such as depth (<italic>d</italic>), flange width (<italic>b</italic>
 <sub>
 <italic>f</italic>
</sub> ), flange thickness (<italic>t</italic>
 <sub>
 <italic>f</italic>
</sub> ), and web thickness (<italic>t</italic>
 <sub>
 <italic>w</italic>
</sub> ), are shown in <xref ref-type="fig" rid="f2">Fig. 2</xref>. Cross-sectional properties of the IPE-140 specimens (<xref ref-type="table" rid="t1">Table 1</xref>) such as the gross area (<italic>A</italic>
 <sub>
 <italic>g</italic>
</sub> ), moment of inertia (<italic>I</italic>), elastic section modulus (<italic>S</italic>), radius of gyration (r), plastic modulus (<italic>Z</italic>), torsion constant (<italic>J</italic>), and torsional warping constant (<italic>C</italic>
 <sub>
 <italic>w</italic>
</sub> ) were calculated according to the equations available in the literature [<xref ref-type="bibr" rid="B18">18</xref>,<xref ref-type="bibr" rid="B19">19</xref>].</p>
			<p>
				<table-wrap id="t1">
					<label>Table 1</label>
					<caption>
						<title>Geometrical properties of cross-section.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gt1.png"/>
					<table-wrap-foot>
						<fn id="TFN1">
							<p><bold>Source:</bold> The authors.</p>
						</fn>
					</table-wrap-foot>
				</table-wrap>
			</p>
			<p>
				<fig id="f2">
					<label>Figure 2</label>
					<caption>
						<title>Dimensions of test specimens.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gf2.png"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>Average values of the mechanical properties of steel beams such as yield stress (<italic>f</italic>
 <sub>
 <italic>y</italic>
</sub> ), modulus of elasticity (<italic>E</italic>), and yield strain (<italic>ε</italic>
 <sub>
 <italic>y</italic>
</sub> ) are listed in <xref ref-type="table" rid="t2">Table 2</xref>.</p>
			<p>
				<table-wrap id="t2">
					<label>Table 2</label>
					<caption>
						<title>Mechanical properties.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gt2.png"/>
					<table-wrap-foot>
						<fn id="TFN2">
							<p><bold>Source:</bold> The authors.</p>
						</fn>
					</table-wrap-foot>
				</table-wrap>
			</p>
			<p>These values were measured from tension tests from four samples cut from the IPE-140 beam as shown in <xref ref-type="fig" rid="f3">Fig. 3</xref>a.</p>
			<p>
				<fig id="f3">
					<label>Figure 3</label>
					<caption>
						<title>Tension test. a) Sample extraction, b) Stress-strain relationship.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gf3.png"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>The longitudinal strain of the specimens was measured using YHFLA-5-3L type large strain gauges that were located in half of the reduced section of the samples, whereas the stress was recorded by means of the 500 kN universal machine. <xref ref-type="fig" rid="f3">Fig. 3</xref>b shows the stress-strain relationship of the samples tested. The tension tests were performed according to the requirements outlined in ASTM E8/E8M [<xref ref-type="bibr" rid="B20">20</xref>].</p>
			<p>In accordance with the limit of width-to-thickness ratio of the flanges and the web and using the values of the mechanical properties shown in <xref ref-type="table" rid="t2">Table 2</xref>, the section is classified as compact since the width-to-thickness ratios of the elements are lower than the limit of maximum slenderness ratio for compact elements. The limits of width-to-thickness ratios were calculated using the requirements outline in ANSI/AISC 360 [<xref ref-type="bibr" rid="B21">21</xref>]. These values are summarized in <xref ref-type="table" rid="t3">Table 3</xref>.</p>
			<p>
				<table-wrap id="t3">
					<label>Table 3</label>
					<caption>
						<title>Width-to-thickness ratio.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gt3.jpg"/>
					<table-wrap-foot>
						<fn id="TFN3">
							<p><bold>Source:</bold> The authors.</p>
						</fn>
					</table-wrap-foot>
				</table-wrap>
			</p>
			<p>The I-shaped steel beams satisfied the permissible tolerances in the cross-section and longitudinal straightness (camber and sweep) in accordance with ASTM A6/A6M [<xref ref-type="bibr" rid="B22">22</xref>]. The laterally unbraced length between the plastic and inelastic buckling zones (<italic>L</italic>
 <sub>
 <italic>p</italic>
</sub> = 0.69 m) and between the inelastic and elastic buckling zones (<italic>L</italic>
 <sub>
 <italic>r</italic>
</sub> = 2.40 m) were calculated according to the requirements outlined in ANSI/AISC 360 [<xref ref-type="bibr" rid="B21">21</xref>] using <xref ref-type="disp-formula" rid="e1">eq. (1)</xref>-(<xref ref-type="disp-formula" rid="e3">3</xref>).</p>
			<p>
				<disp-formula id="e1">
					<graphic xlink:href="0012-7353-dyna-85-207-278-e1.png"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e2">
					<graphic xlink:href="0012-7353-dyna-85-207-278-e2.png"/>
				</disp-formula>
			</p>
			<p>Where,</p>
			<p><italic>h</italic>
 <sub>
 <italic>0</italic>
</sub> = distance between flange centroids.</p>
			<p><italic>c</italic>= coefficient equal to 1.0 for doubly symmetric I-shaped beams, and</p>
			<p>
				<disp-formula id="e3">
					<graphic xlink:href="0012-7353-dyna-85-207-278-e3.png"/>
				</disp-formula>
			</p>
			<p>Based on the values above, the bending tests were performed using laterally unbraced lengths (<italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> ) of 0.69, 1.55, 2.40, 3.60, 4.80, and 6.00 m. For each test length, six specimens were considered. The six specimens included three with longitudinal stiffeners and three without stiffeners, except for the length of 0.69 m, which had no lateral displacement problems (plastic buckling zone). For this length, only three specimens with no longitudinal stiffeners were tested. Longitudinal stiffeners consisted of steel plates with widths <italic>b</italic>
 <sub>
 <italic>s</italic>
</sub> = 62 mm, corresponding to 85% of the flange width (<italic>b</italic>
 <sub>
 <italic>f</italic>
</sub> ) and a thickness equal to the thickness of the web of the section (<italic>t</italic>
 <sub>
 <italic>w</italic>
</sub> ) as shown in <xref ref-type="fig" rid="f4">Fig. 4</xref>a.</p>
			<p>
				<fig id="f4">
					<label>Figure 4</label>
					<caption>
						<title>Longitudinal stiffeners. a) Scheme, b) General view.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gf4.png"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>Longitudinal stiffeners were welded to the top and bottom edge of the flanges as shown in <xref ref-type="fig" rid="f4">Fig. 4</xref>b. Stiffeners were spaced following an ratio, <italic>e/d</italic> defined in this research as the center-to-center spacing of the stiffeners divided by the depth of the section. Taking into account the economic factor and a quick constructive process, the authors considered testing an <italic>e/d</italic> ratio of 3, which represented a spacing between the longitudinal stiffeners equal to <italic>e</italic>= 0.42 m.</p>
		</sec>
		<sec>
			<title>3. Test setup and instrumentation</title>
			<p>The typical test setup is shown in <xref ref-type="fig" rid="f5">Fig. 5</xref>a. The specimens were tested in a 1000 kN capacity load frame, which is fixed to the laboratory’s reaction floor. All specimens were tested by applying upward point loads located at one third of the specimen length from each end.</p>
			<p>
				<fig id="f5">
					<label>Figure 5</label>
					<caption>
						<title>Test setup. a) General view, b) Scheme.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gf5.png"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>The vertical load was applied with 200 and 500 kN capacity hydraulic actuators located at a height of 3.4 m from the ground and fixed to the load frame. Each actuator was used depending on the expected load of failure of the specimen. The actuator was connected to a load cell with equal load capacity, and then connected to a transition steel beam (IPE 330) letting the load to be transferred as point loads at the central third of the beam, by means of high-strength threaded rods as shown in <xref ref-type="fig" rid="f5">Fig. 5</xref>b. </p>
			<p>The specimens were supported at their ends on a set of steel plates and a ball joint system as shown in <xref ref-type="fig" rid="f6">Fig. 6</xref>. This arrangement of plates provided both vertical and lateral restraint similar to a pinned support. Therefore, the span between the support was equal to the laterally unbraced length (<italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> ). It is worth noting that the set of steel plates were fixed to the loading frame by means of 4 high-strength steel threaded rods that were 25 mm in diameter and six bolts that were 12 mm in diameter. This setup allowed for the application of an upward load. The threaded rods and bolts satisfied the requirements outlined in ASTM-F3125/F3125M [<xref ref-type="bibr" rid="B23">23</xref>].</p>
			<p>
				<fig id="f6">
					<label>Figure 6</label>
					<caption>
						<title>Support details. a) General view, b) Lateral view, c) Dimensions and thickness.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gf6.png"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>A ball joint system similar to the aforementioned system allowed for lateral-torsional buckling of the specimens at points where the point load was applied as shown in <xref ref-type="fig" rid="f7">Fig. 7</xref>. This ball joint system was connected to the high-strength threaded rods by means of plates with a hole and bolt system, allowing rotation to occur due to the deflection of tested specimens. The reason to apply an upward load was to simplify the manufacturing of all steel pieces with the final purpose of allowing for lateral-torsional buckling of the specimens to occur.</p>
			<p>
				<fig id="f7">
					<label>Figure 7</label>
					<caption>
						<title>Ball joint system of point vertical load. a) General view, b) Dimensions and thickness.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gf7.png"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>The specimens were instrumented by means of 12 displacement transducers. Displacement transducers were placed at halves and quarters of the specimens’ length to record the lateral and vertical displacements of the top and bottom flanges as shown in <xref ref-type="fig" rid="f8">Fig. 8</xref>a.</p>
			<p>
				<fig id="f8">
					<label>Figure 8</label>
					<caption>
						<title>External instrumentation. a) Location of displacement transducer, b) Element connected to displacement transducer.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gf8.png"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>Due to the deflection of the specimens, it was necessary to connect a U-shaped aluminum element to the stem of the displacement transducers to ensure there was permanent contact with the specimens as shown in <xref ref-type="fig" rid="f8">Fig. 8</xref>b.</p>
			<p>Additionally, strain gauges were installed in the half of the specimens’ length with and without stiffeners as shown in <xref ref-type="fig" rid="f9">Fig. 9</xref>a, <xref ref-type="fig" rid="f9">9</xref>b, respectively.</p>
			<p>
				<fig id="f9">
					<label>Figure 9</label>
					<caption>
						<title>Internal instrumentation. a) Specimen with stiffeners, b) Specimen without stiffeners.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gf9.png"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>The vertical load during the tests was displacement-controlled at a rate of 0,5 mm/min, until the lateral-torsional buckling was reached. Data acquisition was carried out by means of a computer-controlled data logger and recorded ever 3 seconds.</p>
			<p>
				<xref ref-type="fig" rid="f10">Fig. 10</xref> shows the lateral-torsional buckling developed by the specimen without stiffeners with a laterally unbraced length of 6.00 m after performing the test.</p>
			<p>
				<fig id="f10">
					<label>Figure 10</label>
					<caption>
						<title>Lateral-torsional buckling of specimen.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gf10.png"/>
					<attrib><bold>Source:</bold> The authors.</attrib>
				</fig>
			</p>
			<p>
				<xref ref-type="table" rid="t4">Table 4</xref> shows the values of the theoretical and measured maximum moments obtained from all tested specimens. The values of theoretical moment were calculated according to the requirements outlined in ANSI/AISC 360 [<xref ref-type="bibr" rid="B21">21</xref>] through the use of <xref ref-type="disp-formula" rid="e4">eq. (4)</xref>-(<xref ref-type="disp-formula" rid="e7">7</xref>).</p>
			<p>
				<disp-formula id="e4">
					<graphic xlink:href="0012-7353-dyna-85-207-278-e4.png"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e5">
					<graphic xlink:href="0012-7353-dyna-85-207-278-e5.png"/>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e6">
					<graphic xlink:href="0012-7353-dyna-85-207-278-e6.png"/>
				</disp-formula>
			</p>
			<p>Where,</p>
			<p><italic>C</italic>
 <sub>
 <italic>b</italic>
</sub> = coefficient equal to 1.0 for the case of uniform moment, and</p>
			<p>
				<disp-formula id="e7">
					<graphic xlink:href="0012-7353-dyna-85-207-278-e7.png"/>
				</disp-formula>
			</p>
			<p>The specimens were designated with a nomenclature where the first three digits represent the laterally unbraced length in millimeters. The fourth digit corresponds to the letter N (without stiffeners) or Y (with stiffeners), and last digit represents the specimen number tested for each length with and without stiffeners as listed in the third column of <xref ref-type="table" rid="t4">Table 4</xref>.</p>
			<p>
				<table-wrap id="t4">
					<label>Table 4</label>
					<caption>
						<title>Theoretical and measured moment.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-85-207-278-gt4.jpg"/>
					<table-wrap-foot>
						<fn id="TFN4">
							<p><bold>Source:</bold> The authors.</p>
						</fn>
					</table-wrap-foot>
				</table-wrap>
			</p>
		</sec>
		<sec sec-type="results|discussion">
			<title>4. Experimental results and discussion</title>
			<sec>
				<title><italic>4.1. Moment capacity versus laterally unbraced length</italic></title>
				<p>
					<xref ref-type="fig" rid="f11">Fig. 11</xref> shows the obtained relationships between the bending moment at failure vs. laterally unbraced length (<italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> ) of all specimens. The theoretical moment (solid line) was calculated according to the specifications outlined in ANSI/AISC 360 [<xref ref-type="bibr" rid="B21">21</xref>], whereas the values of the specimens with and without longitudinal stiffeners (dashed lines), correspond to the average value of the measured moment for each laterally unbraced length.</p>
				<p>
					<fig id="f11">
						<label>Figure 11</label>
						<caption>
							<title>Moment vs. laterally unbraced length relationships.</title>
						</caption>
						<graphic xlink:href="0012-7353-dyna-85-207-278-gf11.png"/>
						<attrib><bold>Source:</bold> The authors.</attrib>
					</fig>
				</p>
				<p>The acting moment was computed as one half of the load recorded by the load cell installed on the actuator times one third of the specimen’s length. Flexural moment of the specimens without longitudinal stiffeners showed an acceptable agreement with respect to theoretical flexural capacity. The moment measured in these specimens was greater than the theoretical moment, except for the laterally unbraced length of 2.40 m.</p>
				<p>On the other hand, the moment developed by the specimens with stiffeners was higher with respect to the specimens without stiffeners for all the laterally unbraced lengths. This evidence supports that the use of longitudinal stiffeners on I-shaped steel beams increases the bending moment capacity in the elastic and inelastic buckling zones.</p>
				<p><italic>It is worth noting that the present study did not evaluate specimens with longitudinal stiffeners for elements with a laterally unbraced length of 0.69 m, given that this length is the upper bound for the plastic buckling zone criterion. This length theoretically represents no issues for the specimens in terms of lateral-torsional buckling.</italic></p>
				<p>The improvement in terms of the percentage of the measured moment capacity of the stiffened specimens with respect to the specimens without stiffeners is shown in <xref ref-type="fig" rid="f12">Fig. 12</xref>. </p>
				<p>
					<fig id="f12">
						<label>Figure 12</label>
						<caption>
							<title>Improved moment.</title>
						</caption>
						<graphic xlink:href="0012-7353-dyna-85-207-278-gf12.png"/>
						<attrib><bold>Source:</bold> The authors.</attrib>
					</fig>
				</p>
				<p>Specimens with laterally unbraced lengths of 2.40 through 6.00 m, increased their flexural capacity from 34 to 82%. These lengths correspond to an elastic buckling zone, as shown in <xref ref-type="fig" rid="f12">Fig. 12</xref>, where lengths are expressed in terms of both laterally unbraced length and <italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> 
 <italic>/L</italic>
 <sub>
 <italic>r</italic>
</sub> ratio.</p>
				<p>An overall positive linear correlation is observed between the increase of the moment capacity and laterally unbraced length, with an exception for the case where <italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> = 3.60 m. At this length the increased capacity was similar to the case where <italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> = 2.40 m. This fact could be attributed to the proximity of the limit between the inelastic and elastic buckling zones.</p>
				<p>On the other hand, for the laterally unbraced length of 1.55 m (inelastic buckling zone), the achieved improvement in moment capacity was 7%, which does not represent a meaningful increase.</p>
			</sec>
			<sec>
				<title><italic>4.2. Lateral displacement of the compression flange</italic></title>
				<p>
					<xref ref-type="fig" rid="f13">Fig. 13</xref> shows the relationship of the moment vs. lateral displacement of the compression flange (lateral-torsional buckling) for all tested specimens in this study. For the laterally unbraced length of 6.0 m, the specimens without stiffeners showed an average value of lateral displacement of the compression flange of 30.85 mm (from 25.76 up to 38.89 mm) as shown in <xref ref-type="fig" rid="f13">Fig. 13</xref>a. Whereas the stiffened specimens exhibited an average value of 8.77 mm, which represented a decrease of 72%.</p>
				<p>
					<fig id="f13">
						<label>Figure 13</label>
						<caption>
							<title>Lateral displacement of the compression flange. a) Specimens with Lb = 6.00 m, b) Specimens with Lb = 4.80 m, c) Specimens with Lb = 3.60 m, d) Specimens with Lb = 2.40 m, e) Specimens with Lb = 1.55 m.</title>
						</caption>
						<graphic xlink:href="0012-7353-dyna-85-207-278-gf13.png"><italic>/</italic></graphic>
						<attrib><bold>Source:</bold> The authors.</attrib>
					</fig>
				</p>
				<p>A similar behavior occurred for the laterally unbraced length of 4.80 m as shown in <xref ref-type="fig" rid="f13">Fig. 13</xref>b. The average value of lateral displacement reached by the specimens without stiffeners (26.20 mm) decreased to an average value of 11.48 mm in the stiffened specimens, which represented a decrease of 56%. Therefore, the use of longitudinal stiffeners results in a noticeable lateral stability in the specimens for laterally unbraced lengths of 4.80 and 6.00 m.</p>
				<p>On the other hand, the average decrease of lateral displacement of the compression flange for the specimens with laterally unbraced lengths of 3.60 and 2.40 m were 44 and 40%, respectively. These results indicate that the use of longitudinal stiffeners exhibited an acceptable lateral stability in these specimens as shown in <xref ref-type="fig" rid="f13">Fig. 13</xref>c, 13d, respectively. <xref ref-type="fig" rid="f13">Fig. 13</xref>e shows that the use of longitudinal stiffeners for the specimens with a laterally unbraced length of 1.55 m, showed a lower decrease (27%) in the lateral displacement of the compression flange.</p>
			</sec>
			<sec>
				<title><italic>4.3. Angle of twist</italic></title>
				<p>The measured twist angle of all specimens with and without longitudinal stiffeners as a function of the applied flexural moment is shown in <xref ref-type="fig" rid="f14">Fig. 14</xref>. The twist angle was calculated as the inverse of the sine function of the difference between the lateral displacement of the top and bottom flanges divided by the depth of the section (<italic>d</italic>= 140 mm).</p>
				<p>
					<fig id="f14">
						<label>Figure 14</label>
						<caption>
							<title>Twist angle of the specimens. a) Specimens with Lb = 6.00 m, b) Specimens with Lb = 4.80 m, c) Specimens with Lb = 3.60 m, d) Specimens with Lb = 2.40 m, e) Specimens with Lb = 1.55 m.</title>
						</caption>
						<graphic xlink:href="0012-7353-dyna-85-207-278-gf14.png"/>
						<attrib><bold>Source:</bold> The authors.</attrib>
					</fig>
				</p>
				<p>The twist angle developed by all specimens presented a similar behavior to the lateral displacement of the compression flange. There was a noteworthy decrease in the angle of twist for laterally unbraced lengths of 6.00 and 4.80 m by using of longitudinal stiffeners as shown in <xref ref-type="fig" rid="f14">Fig. 14</xref>a, <xref ref-type="fig" rid="f14">14</xref>b.</p>
				<p>
					<xref ref-type="fig" rid="f15">Fig. 15</xref> shows the average values for the failure twist angle of all specimens with and without longitudinal stiffeners for each laterally unbraced length studied.</p>
				<p>
					<fig id="f15">
						<label>Figure 15</label>
						<caption>
							<title>Failure twist angle.</title>
						</caption>
						<graphic xlink:href="0012-7353-dyna-85-207-278-gf15.png"><italic>/</italic></graphic>
						<attrib><bold>Source:</bold> The authors.</attrib>
					</fig>
				</p>
				<p>The highest values for the failure twist angle in the specimens without stiffeners were measured for the laterally unbraced lengths of 4.80 and 6.00 m, which developed values of 0.119 and 0.123 rad, respectively. Whereas the specimens with laterally unbraced lengths from 1.55 up to 3.60 m, developed values from 0.020 up to 0.030 rad, respectively, as shown in <xref ref-type="fig" rid="f15">Fig. 15</xref>.</p>
				<p>On the other hand, the values for the failure twist angle of the specimens with longitudinal stiffeners were lower relative to the specimens without stiffeners for all laterally unbraced lengths. These values were kept in an interval narrow from 0.010 up to 0.025 rad.</p>
				<p>These results indicated that the use of longitudinal stiffeners decreased the failure twist angle for all laterally unbraced lengths, reaching a maximum decrease of 79 and 90% for the laterally unbraced lengths of 4.80 m (<italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> 
 <italic>/L</italic>
 <sub>
 <italic>r</italic>
</sub> = 2.0) and 6.0 m (<italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> 
 <italic>/L</italic>
 <sub>
 <italic>r</italic>
</sub> = 2.5), respectively. This percentage is higher than the values reported by Szewczak et al. [<xref ref-type="bibr" rid="B5">5</xref>], who obtained a decrease of 44% in the failure twist angle when considering longitudinal stiffeners at the ends of the beam only and subjected to concentrated torque at the length’s center.</p>
			</sec>
			<sec>
				<title><italic>4.4. Longitudinal strain of the compression flange</italic></title>
				<p>The curves of the longitudinal strain of the compression flange of all specimens is shown in <xref ref-type="fig" rid="f16">Fig. 16</xref>. </p>
				<p>
					<fig id="f16">
						<label>Figure 16</label>
						<caption>
							<title>Longitudinal strain of the compression flange. a) Specimens with Lb = 6.00 m, b) Specimens with Lb = 4.80 m, c) Specimens with Lb = 3.60 m, d) Specimens with Lb = 2.40 m, e) Specimens with Lb = 1.55 m.</title>
						</caption>
						<graphic xlink:href="0012-7353-dyna-85-207-278-gf16.jpg"/>
						<attrib><bold>Source:</bold> The authors</attrib>
					</fig>
				</p>
				<p>These curves were recorded by using two strain gauges located at half of the specimens’ length with a separation of 50 mm and designated as SG1 and SG2 as shown in <xref ref-type="fig" rid="f9">Fig. 9</xref>.</p>
				<p>
					<xref ref-type="fig" rid="f16">Fig. 16</xref>a-<xref ref-type="fig" rid="f16">16</xref>c show that the longitudinal strain of the compression flange of the specimens with and without longitudinal stiffeners corresponding to the laterally unbraced lengths from 6.00 up to 3.60 m, kept values within the elastic limit during the loading and unloading process. According to the mechanical properties of the material, the strain of the elastic limit was estimated as 0.0023 as shown in <xref ref-type="table" rid="t2">Table 2</xref>. Nevertheless, for the laterally unbraced length between the inelastic and elastic buckling zones (<italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> = 2.40 m), some of the specimens with and without longitudinal stiffeners developed an inelastic buckling, presenting a permanent deformation in the compression flange even when the load was removed as shown in <xref ref-type="fig" rid="f16">Fig. 16</xref>d. This mode of failure matches the characteristic described by Salmon and Johnson [<xref ref-type="bibr" rid="B19">19</xref>].</p>
				<p>As expected, the longitudinal strain of the compression flanges of the specimens with and without longitudinal stiffeners corresponding to the laterally unbraced length of 1.55 m, significantly exceeded the elastic limit as shown in <xref ref-type="fig" rid="f16">Fig. 16</xref>e. In <xref ref-type="fig" rid="f16">Fig. 16</xref>a-<xref ref-type="fig" rid="f16">16</xref>e some specimens showed a transition of stresses from compression to tension, which represents the release of the compression load due to lateral bending right after reaching the failure twist angle.</p>
				<p>
					<xref ref-type="fig" rid="f17">Fig. 17</xref> shows the strain of the longitudinal stiffeners of the specimens with laterally unbraced lengths of 6.00 and 1.55 m. The solid line corresponds to the strain of the longitudinal stiffeners that developed concave curvature under lateral-torsional buckling, whereas the dashed line corresponds to the strain of the longitudinal stiffeners that developed convex curvature. All stiffeners developed longitudinal strain under compression stress.</p>
				<p>
					<fig id="f17">
						<label>Figure 17</label>
						<caption>
							<title>Strain of longitudinal stiffeners. a) Specimens with Lb = 6.00 m, b) Specimens with Lb = 1.55 m.</title>
						</caption>
						<graphic xlink:href="0012-7353-dyna-85-207-278-gf17.png"/>
						<attrib><bold>Source:</bold> The authors.</attrib>
					</fig>
				</p>
				<p>The longitudinal stiffeners used in the specimens within the elastic buckling zone (from 2.4 to 6.00 m) presented a similar behavior and their values of strain were lower than 0.00004 as shown in <xref ref-type="fig" rid="f17">Fig. 17</xref>a, which corresponds particularly to the specimen with a laterally unbraced length of 6.00 m. Whereas for the laterally unbraced length of 1.55 m, which belong to the inelastic buckling zone, the strain reached values up to 0.00016 as shown in <xref ref-type="fig" rid="f17">Fig. 17</xref>b.</p>
				<p>Therefore, the longitudinal stiffeners used in all tested specimens of this research were subjected to compression low stresses, in such a way that the elastic limit of the material was not exceeded.</p>
			</sec>
			<sec>
				<title><italic>4.5. Longitudinal strain of the web</italic></title>
				<p>
					<xref ref-type="fig" rid="f18">Fig. 18</xref> shows the strain of the web of the specimens with and without longitudinal stiffeners for the laterally unbraced lengths of 6.00 and 1.55 m. The use of longitudinal stiffeners did not modify the behavior of the strain in the web of the specimens in the elastic buckling zone. In this buckling zone, the strain in the web was similar for all specimens and did not exceed a value of 0.00005 as shown in <xref ref-type="fig" rid="f18">Fig. 18</xref>a, which corresponds particularly to the specimen with laterally unbraced length of 6.00 m.</p>
				<p>
					<fig id="f18">
						<label>Figure 18</label>
						<caption>
							<title>Strain of the web. a) Specimens with Lb = 6.00 m, b) Specimens with Lb = 1.55 m.</title>
						</caption>
						<graphic xlink:href="0012-7353-dyna-85-207-278-gf18.png"/>
						<attrib><bold>Source:</bold> The authors.</attrib>
					</fig>
				</p>
				<p>Nonetheless, the strain in the web of the specimens with stiffeners for a laterally unbraced length of 1.55 m (inelastic buckling zone) was slight higher with respect to specimens without stiffeners. This increase continues within the elastic limit of the material reaching a value up to 0.0002 as shown in <xref ref-type="fig" rid="f18">Fig. 18</xref>b. Hence, the use of longitudinal stiffeners did not affect the behavior of the web of the tested specimens in this study.</p>
			</sec>
		</sec>
		<sec sec-type="conclusions">
			<title>5. Conclusions</title>
			<p>The performed tests in this study showed that the use of longitudinal stiffeners on I-shaped steel beam increased the moment capacity in the elastic buckling zone in an interval from 34 up to 82%, for specimens with a <italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> 
 <italic>/L</italic>
 <sub>
 <italic>r</italic>
</sub> ratio of 1.0 and 2.5, respectively. Nonetheless, for the inelastic buckling zone (<italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> = 1.55 m), although the results indicated an increase in the moment capacity of 7%, this value does not represent a significant increase.</p>
			<p>In addition, the use of longitudinal stiffeners provided an acceptable lateral stability on I-shaped steel beams subjected to bending stresses. The use of these elements decreased the lateral displacement of the compression flange in an interval from 40 up to 72% for specimens with a <italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> 
 <italic>/L</italic>
 <sub>
 <italic>r</italic>
</sub> ratio of 1.0 and 2.5, respectively, corresponding to the elastic buckling zone. Whereas for the specimens in the inelastic buckling zone with a <italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> 
 <italic>/L</italic>
 <sub>
 <italic>r</italic>
</sub> ratio of 0.65, showed that there was a low decrease of the lateral displacement of the compression flange of 27%.</p>
			<p>Another advantage of using longitudinal stiffeners on I-shaped steel beam was the decrease in the failure twist angle both in the elastic and inelastic buckling zones. This decrease reached a maximum value of 79 and 90% for specimens with a <italic>L</italic>
 <sub>
 <italic>b</italic>
</sub> 
 <italic>/L</italic>
 <sub>
 <italic>r</italic>
</sub> ratio of 2.0 and 2.5, respectively.</p>
			<p>According to the experimental results of this research, the use of longitudinal stiffeners could be a good solution to improve the bending moment capacity and to provide better lateral stability of I-shaped steel beams, especially in countries where manpower is low-cost, allowing the manufacturing of stiffening plates which represent an option for reducing costs, rather than using I-shaped beams with higher moments of inertia (heavier elements). Nevertheless, it is advisable to carry out these tests on I-shaped steel beams at greater depths.</p>
		</sec>
	</body>
	<back>
		<ack>
			<title>Acknowledgments</title>
			<p>This study was possible due to the financial support of the Universidad Pontificia Bolivariana Bucaramanga, through grant number 079-0815-2300. The authors also would like to thank the technical staff at the Structures Laboratory at the Universidad Pontificia Bolivariana Bucaramanga for their continuous support during the experimental tests.</p>
		</ack>
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		<fn-group>
			<fn fn-type="other" id="fn1">
				<label>How to cite:</label>
				<p> Prado, N.I., Carrillo J., Ospina, G. and Ramirez-Amaya, D., Experimental assessment of I-shaped steel beams with longitudinal stiffeners under lateral-torsional buckling. DYNA, 85(207), pp. 278-287, Octubre - Diciembre, 2018.</p>
			</fn>
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		<fn-group>
			<fn fn-type="other" id="fn2">
				<label>N.I. Prado,</label>
				<p> received his PhD degree in Structural Engineering in 2014 from Universidad Nacional Autónoma de México, México D.F., México. Since 2001, he has been professor of Facultad de Ingeniería Civil at Universidad Pontificia Bolivariana, Bucaramanga, Colombia. His research interests include the study of reinforced concrete and steel structures behavior. ORCID: 0000-0002-8259-8995</p>
			</fn>
			<fn fn-type="other" id="fn3">
				<label>J. Carrillo,</label>
				<p> has been associate professor in the Department of Civil Engineering at Universidad Militar Nueva Granada, Bogotá, Colombia since 2004. He received his PhD degree in Structural Engineering from Universidad Nacional Autónoma de México, UNAM in 2010. He is member of ACI Committees 314, Simplified Design of Concrete Building; 369, Seismic Repair and Rehabilitation; and 374, Performance-Based Seismic Design of Concrete Buildings. His research interests include the behavior, design and rehabilitation of structures under seismic actions. ORCID: 0000-0002-8274-5414</p>
			</fn>
			<fn fn-type="other" id="fn4">
				<label>G.A. Ospina,</label>
				<p> received his PhD in Structures from University of South Carolina in 2013. His current position is assistant professor at the Civil Engineering Department at Universidad Pontificia Bolivariana in Bucaramanga, Colombia (January 2014-Present). His research background and interests cover several areas of structural engineering: structural dynamic, structural health monitoring (SHM), numerical modeling, deterministic and probabilistic model updating, data acquisition and system identification. ORCID: 0000-0002-4966-2190</p>
			</fn>
			<fn fn-type="other" id="fn5">
				<label>D. Ramirez-Amaya,</label>
				<p> received the BSc. in Civil Engineer and Electronic Engineer, both degrees in 2014 from Universidad Pontificia Bolivariana, Bucaramanga, Colombia, where he is professor and MSc. student at the Civil Engineering program. His research background and interests are: structural dynamic, mechanics of materials, instrumentation and automation of laboratory tests. ORCID: 0000-0002-6493-1678</p>
			</fn>
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</article>