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<article xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="1.3" article-type="research-article" xml:lang="en"><front><journal-meta><journal-id journal-id-type="issn">2357-0857</journal-id><journal-title-group><journal-title>Environmental Science &amp; Sustainable Development</journal-title><abbrev-journal-title>ESSD</abbrev-journal-title></journal-title-group><issn pub-type="epub">2357-0857</issn><issn pub-type="ppub">2357-0849</issn><publisher><publisher-name>IEREK Press</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.21625/essd.v10i4.1211</article-id><article-categories><subj-group><subject>Structural Engineering</subject></subj-group></article-categories><title-group><article-title>Topology Optimization of Horizontal Links in Multi-story Eccentric Braced Frames</article-title></title-group><contrib-group><contrib contrib-type="author"><name><surname>Ibrahim</surname><given-names>Amr M.</given-names></name><address><country>Lebanon</country></address><xref ref-type="aff" rid="AFF-1"/></contrib><contrib contrib-type="author"><name><surname>Ashraf</surname><given-names>Ahmed</given-names></name><address><country>Egypt</country></address><xref ref-type="aff" rid="AFF-2"/></contrib><contrib contrib-type="author"><name><surname>Saleh</surname><given-names>Yasser N.</given-names></name><address><country>Egypt</country></address><xref ref-type="aff" rid="AFF-3"/></contrib></contrib-group><contrib-group><contrib contrib-type="editor"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0001-8754-3523</contrib-id><name><surname>Spina</surname><given-names>Professor Lucia Della</given-names></name><address><country>Italy</country></address></contrib><contrib contrib-type="editor"><name><surname>Trovato</surname><given-names>Maria Rosa</given-names></name></contrib></contrib-group><aff id="AFF-1">Assistant Professor, Civil Engineering Department, The British University in Egypt, Cairo, Egypt</aff><aff id="AFF-2">Undergraduate student, Civil Engineering Department, The British University in Egypt, Cairo, Egypt</aff><aff id="AFF-3">Assistant Lecturer, Civil Engineering Department, The British University in Egypt, Cairo, Egypt</aff><pub-date date-type="pub" iso-8601-date="2025-12-31" publication-format="electronic"><day>31</day><month>12</month><year>2025</year></pub-date><pub-date date-type="collection" iso-8601-date="2025-12-31" publication-format="electronic"><day>31</day><month>12</month><year>2025</year></pub-date><volume>10</volume><issue>4</issue><fpage>40</fpage><lpage>50</lpage><history><date date-type="received" iso-8601-date="2025-6-3"><day>3</day><month>6</month><year>2025</year></date><date date-type="accepted" iso-8601-date="2025-8-7"><day>7</day><month>8</month><year>2025</year></date></history><permissions><copyright-statement>Copyright (c) 2025 Amr M. Ibrahim, Ahmed Ashraf, Yasser N. Saleh</copyright-statement><copyright-year>2025</copyright-year><copyright-holder>Amr M. Ibrahim, Ahmed Ashraf, Yasser N. Saleh</copyright-holder><license license-type="open-access" xlink:href="https://creativecommons.org/licenses/by/4.0/"><ali:license_ref xmlns:ali="http://www.niso.org/schemas/ali/1.0/">https://creativecommons.org/licenses/by/4.0/</ali:license_ref><license-p>LicenseThe Author shall grant to the Publisher and its agents the nonexclusive perpetual right and license to publish, archive, and make accessible the Work in whole or in part in all forms of media now or hereafter known under a Creative Commons Attribution 4.0 License or its equivalent, which, for the avoidance of doubt, allows others to copy, distribute, and transmit the Work under the following conditions:Attribution: other users must attribute the Work in the manner specified by the author as indicated on the journal Web site;With the understanding that the above condition can be waived with permission from the Author and that where the Work or any of its elements is in the public domain under applicable law, that status is in no way affected by the license.The Author is able to enter into separate, additional contractual arrangements for the nonexclusive distribution of the journal's published version of the Work (e.g., post it to an institutional repository or publish it in a book), as long as there is provided in the document an acknowledgement of its initial publication in this journal.Authors are permitted and encouraged to post online a pre-publication manuscript (but not the Publisher's final formatted PDF version of the Work) in institutional repositories or on their Websites prior to and during the submission process, as it can lead to productive exchanges, as well as earlier and greater citation of published work (see The Effect of Open Access). 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The integration of topology optimization and additive manufacturing techniques has paved the way for the fabrication of complex geometries that are both <bold><italic>cost-effective</italic></bold> and material efficient, enabling structures that would be challenging to produce using traditional manufacturing methods. Concurrently, the application of eccentric braced frames with link elements has seen a notable increase, attributed to their enhanced seismic resistance capabilities compared to concentric braced frames. This study integrates topology optimization and AM to design optimized shear links for EBFs that outperform standard HEB European sections. Finite Element Models were developed in Abaqus to simulate both monotonic and cyclic loading scenarios. Pushover and cyclic analyses were performed on single-, two-, and three-story frames to assess the performance of the optimized links. Through pushover analysis, the results show that employing optimized HEB sections leads to a significant reduction in steel volume while simultaneously enhancing both the yielding and ultimate strength of the structure, with some multi-story frames demonstrating a twofold increase in performance over standard designs. Moreover, cyclic performance analysis of models with optimized links underscores a notable increase in the base shear ultimate force with marked improvement in the effective stiffness compared to models with standard sections. However, this was accompanied by a reduction in energy dissipation and the viscous damping coefficient.</p></abstract><kwd-group><kwd>Eccentrically braced frames</kwd><kwd>Shear link</kwd><kwd>Topology optimization</kwd><kwd>Pushover analysis</kwd><kwd>Cyclic loading.</kwd></kwd-group><funding-group><funding-statement>The authors would like to acknowledge the British University in Egypt for the travel grant that supported the publication of this document.</funding-statement></funding-group><custom-meta-group><custom-meta><meta-name>File created by JATS Editor</meta-name><meta-value><ext-link ext-link-type="uri" xlink:href="https://jatseditor.com" xlink:title="JATS Editor">JATS Editor</ext-link></meta-value></custom-meta><custom-meta><meta-name>issue-created-year</meta-name><meta-value>2025</meta-value></custom-meta></custom-meta-group></article-meta></front><body><sec><title>1. Introduction.</title><p>The inclusion of additive manufacturing (AM) offers a transformative shift in the construction and structural engineering industries, presenting significant potential for innovation, optimization, and sustainability. AM allows the production of complex geometries directly from digital models <xref ref-type="bibr" rid="BIBR-1">(Bos et al., 2016)</xref>, significantly expanding the design space available to engineers and architects. In particular, Wire and Arc Additive Manufacturing (WAAM) has gained traction as a viable method for large-scale structural fabrication due to its high deposition rate, geometric flexibility, and cost-effectiveness <xref ref-type="bibr" rid="BIBR-2">(Shukla et al., 2020)</xref>. The integration between AM and topology optimization made a generation of optimized structures with efficient material distribution possible with the aid of finite element applications <xref ref-type="bibr" rid="BIBR-3">(Craveiro et al., 2017)</xref>. The use of AM in construction enables the production of unique components that are difficult to fabricate using traditional techniques <xref ref-type="bibr" rid="BIBR-4">(Labonnote et al., 2016)</xref>. Recent high-profile applications—such as the Gaudí-inspired pavilion in Barcelona, Spain, and the 3D-printed office buildings in Dubai—demonstrate the architectural and structural capabilities of AM in producing complex forms that would be challenging, if not impossible, to achieve through conventional manufacturing methods <xref ref-type="bibr" rid="BIBR-5">(Lange et al., 2021)</xref>.</p><p>This advancement aligns naturally with the field of topology optimization, a computational design approach that strategically redistributes material within a given domain to achieve maximum structural performance with minimum material use. Topology optimization, particularly using methods like Solid Isotropic Material with Penalization (SIMP), has proven effective in generating lightweight and structurally efficient components, often with non-intuitive geometries that require AM for physical realization (<xref ref-type="bibr" rid="BIBR-6">(Bendsøe &amp; Sigmund, 2013)</xref>; <xref ref-type="bibr" rid="BIBR-7">(Galjaard et al., 2014)</xref>). Previous studies have extended this methodology to various structural elements, including perforated beams <xref ref-type="bibr" rid="BIBR-8">(Tsavdaridis et al., 2015)</xref>, trusses, and custom joints, with demonstrated benefits in both mechanical performance and material sustainability. The integration of AM with topology optimization not only enables highly efficient load paths but also supports sustainability goals by reducing material waste and embodied carbon in construction <xref ref-type="bibr" rid="BIBR-3">(Craveiro et al., 2017)</xref> <xref ref-type="bibr" rid="BIBR-9">(Wu et al., 2016)</xref>.</p><p>In the context of seismic design, the application of topology optimization remains relatively underexplored but increasingly important. One of the most promising structural systems in seismic regions is the Eccentrically Braced Frame (EBF), which combines the ductility of moment-resisting frames with the stiffness and strength of concentrically braced frames. Central to the performance of EBFs is the shear link, a designated yielding component that dissipates energy during seismic events and protects the main structural members from inelastic deformation <xref ref-type="bibr" rid="BIBR-10">(Della Corte et al., 2013)</xref><xref ref-type="bibr" rid="BIBR-11">(Bruneau et al., 2011)</xref>. Conventional shear links are typically fabricated from rolled steel profiles such as HEB sections, chosen for their availability and standardized behavior. However, these standard profiles do not necessarily represent the most material-efficient or performance-optimized solutions, particularly in complex or high-seismic applications.</p><p>Recent research efforts have begun exploring the potential of topology-optimized shear links to improve the performance of EBFs. Notably, <xref ref-type="bibr" rid="BIBR-12">(Ramonell &amp; Chacón, 2021)</xref> employed ABAQUS-based finite element modeling to design and assess topology-optimized horizontal links, reporting improvements in both yielding and ultimate strength compared to standard HEB sections. Similarly, <xref ref-type="bibr" rid="BIBR-13">(Saleh et al., 2024-08)</xref> extended this work to vertical shear links and cyclic loading conditions, further demonstrating the viability of optimization for enhancing seismic performance. These studies collectively highlight the potential of combining AM and topology optimization to create next-generation structural components that are both efficient and resilient.</p><p>However, the majority of existing research has focused on single-story frames, which do not fully capture the structural complexity or interaction effects present in multi-story buildings. As seismic demands and inter-story drift accumulate over height, the behavior of optimized shear links may differ significantly, necessitating further investigation into their scalability and effectiveness in multi-story contexts. This study aims to extend the current state of knowledge by applying topology optimization to horizontal shear links in multi-story EBFs and evaluating their performance under both monotonic (pushover) and cyclic loading conditions. Finite element models developed in Abaqus are used to simulate realistic boundary conditions and loading protocols, with performance metrics including base shear capacity, effective stiffness, energy dissipation, and buckling behavior. Comparisons between conventional HEB sections and their topology-optimized counterparts are made across one-, two-, and three-story frame configurations. This research also seeks to reduce structural material usage through computational topology optimization, thereby achieving volume-efficient structural components with improved seismic performance. This volume reduction directly translates into a lower demand for steel, which contributes to minimizing resource consumption and embodied carbon emissions-two core themes in environmental sustainability. As the steel industry is a major contributor to global CO₂ emissions, designing structural elements that require less material promotes more sustainable construction practices. In doing so, this research seeks to not only demonstrate the potential benefits of topology-optimized shear links in seismic design but also identify the limitations and considerations that must be addressed for their broader implementation.</p></sec><sec><title>2. Numerical Modeling</title><p>Finite Element Models (FEM) within Abaqus were deployed to conduct pushover analyses on horizontal links in eccentric braced frames. The specifications of the link sections, including dimensions and material properties, were directly sourced from <xref ref-type="bibr" rid="BIBR-12">(Ramonell &amp; Chacón, 2021)</xref>, facilitating a rigorous validation of the resultant data. The sections utilized in this study are detailed in <xref ref-type="table" rid="table-1">Table 1</xref>, with the material of choice being European steel grade S275. The material's plastic behavior is characterized by a nonlinear profile, delineated through two critical points: an initial yield point at zero strain and an ultimate strength of 430 MPa at a maximum strain of 0.2. The geometry and dimensions of the eccentric braced frame under investigation are illustrated in <xref ref-type="fig" rid="figure-1">Figure 1</xref>. For this analysis, the entire frame is modeled using wire elements, whereas the link component is designated as a solid element to facilitate focused study.</p><fig id="figure-1" ignoredToc=""><label>Figure 1</label><caption><p>Eccentric braced frame dimensions (source: <xref ref-type="bibr" rid="BIBR-12">(Ramonell &amp; Chacón, 2021)</xref>)</p></caption><graphic xlink:href="https://press.ierek.com/index.php/ESSD/article/download/1211/1387/6936" mimetype="image" mime-subtype="png"><alt-text>Image</alt-text></graphic></fig><table-wrap id="table-1" ignoredToc=""><label>Table 1</label><caption><p>Eccentric braced frame sections (source: <xref ref-type="bibr" rid="BIBR-12">(Ramonell &amp; Chacón, 2021)</xref>).</p></caption><table frame="box" rules="all"><thead><tr><th colspan="1" rowspan="1" style="" align="center" valign="middle">Model</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Link section</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Beam section</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Diagonal section</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Column section</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Link length (e) (m)</th></tr></thead><tbody><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">HEB140</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">HEB140</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">HEB200</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">HEB180</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.75</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">HEB160</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">HEB160</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">HEB200</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">HEB200</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.83</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">HEB180</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">HEB180</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">HEB200</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">HEB200</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.93</td></tr></tbody></table></table-wrap><sec><title>2.1. Mesh Convergence</title><p>To ensure the utmost accuracy of results for each link, the frame underwent meshing with a specified size of 10 mm, employing a linear beam in spatial configuration with two nodes (B31), aligning with the default setting for wire elements. The selection of a 10 mm mesh was substantiated through an analysis of the forces at a displacement of 56 mm across varying mesh sizes. It was observed that results stabilized at a mesh size of 10 mm, with the discrepancy between mesh sizes of 10 mm and 100 mm being a negligible 0.00155233%. This analysis conclusively validates the suitability of a 10 mm mesh for all three models, affirming its non-impact on the integrity of the results.</p><p>For all link analyses, the mesh was standardized using the hexahedral linear element with reduced integration from the Abaqus library (C3D8R). Initial trials with various mesh sizes for the HEB140 link yielded unstable results, underscoring the necessity of a comprehensive mesh convergence study. Such an investigation is paramount to ascertain the optimal mesh size that ensures stability and accuracy across all link models. The findings from the mesh convergence analysis indicated that a mesh size of 9 mm was most conducive to convergence for both HEB140 and HEB160 links. Conversely, for the HEB180 link, stability was achieved with a mesh size of 10 mm or larger.</p></sec><sec><title>2.2. Boundary Conditions</title><p>To preclude any out-of-plane movements within the eccentric braced frame, the columns and beams were externally constrained by restricting the U3 displacement, effectively immobilizing them in the out-of-plane direction. Furthermore, the frame's base points were configured as pinned, ensuring rotational freedom while preventing translational movements. Additionally, to facilitate the pushover analysis, a target displacement of 56 mm was applied at the frame's eave as shown in <xref ref-type="fig" rid="figure-2">Figure 2</xref>. <xref ref-type="bibr" rid="BIBR-12">(Ramonell &amp; Chacón, 2021)</xref> advocate for the implementation of a coupling constraint to preserve the kinematic coupling between the link and the frame as illustrated in  <xref ref-type="fig" rid="figure-3">Figure 3</xref>, thereby enhancing the solution's accuracy with respect to degrees of freedom. This coupling is strategically applied between a designated point on the frame and the corresponding surface of the link.</p><fig id="figure-2" ignoredToc=""><label>Figure 2</label><caption><p>Assigned displacement for pushover analysis (source: by authors)</p></caption><graphic xlink:href="https://press.ierek.com/index.php/ESSD/article/download/1211/1387/6937" mimetype="image" mime-subtype="png"><alt-text>Image</alt-text></graphic></fig><fig id="figure-3" ignoredToc=""><label>Figure 3</label><caption><p>Coupling constraint between the solid element model of the link and the frame elements representing the rest of the EBF model (source: by authors)</p></caption><graphic xlink:href="https://press.ierek.com/index.php/ESSD/article/download/1211/1387/6938" mimetype="image" mime-subtype="png"><alt-text>Image</alt-text></graphic></fig></sec><sec><title>2.3. Topology Optimization Method</title><p>The conventional HEB profile is substituted with a cubic volume, mirroring the dimensions, width, depth, and length of the HEB originally employed, as depicted in <xref ref-type="fig" rid="figure-4">Figure 4</xref>. In the pursuit of mesh convergence, varying mesh sizes were evaluated through topology optimization for the HEB 140 model. A pushover analysis utilizing the cubic link model facilitated the generation of force-displacement curves, alongside correlations between the number of elements and forces at a 56mm displacement. Interestingly, the results indicated uniformity across different mesh sizes, a phenomenon attributable to the geometric simplicity of the cubic shape, rendering mesh size a non-critical factor in this context. Conversely, stress distribution within the optimized shape varied significantly across different meshes. This variability underscores the influence of mesh size on stress distribution outcomes within the topology optimization process. Specifically, for meshes sized 10mm and 15mm, minimal stress was observed in the initial third of the shape. Meanwhile, a 5mm mesh size resulted in stress concentration within the link's central region. This observation highlights how mesh granularity affects stress distribution across the link, corroborating <xref ref-type="bibr" rid="BIBR-12">(Ramonell &amp; Chacón, 2021)</xref> assertion that finer meshes yield more detailed shape resolutions, thereby enhancing the scope for material reduction during topology optimization. Consequently, a 10mm mesh size was selected for all topology-optimized links, aiming to centralize stress distribution within the link to optimize computational efficiency in subsequent topology optimization iterations.</p><p>The optimization process was refined by adjusting the increment settings to medium, initiating with zero percent initial material removal. Central to this methodology is the establishment of two singular term responses derived from the comprehensive response list: </p><p>1) Strain energy encompassing the entire model, and 2) Volume pertaining to the link area targeted for topology optimization. The primary objective function concerning strain energy aims to maximize the design's overall response. Concurrently, a volume design response criterion facilitates the desired material reduction in the link area by approximately 18%, aligning the optimized link volume closely with that of traditional HEB section volumes. This strategy is graphically represented in <xref ref-type="fig" rid="figure-5">Figure 5</xref>.</p><fig id="figure-4" ignoredToc=""><label>Figure 4</label><caption><p>Link used for topology optimization (source: by authors)</p></caption><graphic xlink:href="https://press.ierek.com/index.php/ESSD/article/download/1211/1387/6939" mimetype="image" mime-subtype="png"><alt-text>Image</alt-text></graphic></fig><fig id="figure-5" ignoredToc=""><label>Figure 5</label><caption><p>Topology optimization procedure (source: by authors)</p></caption><graphic xlink:href="https://press.ierek.com/index.php/ESSD/article/download/1211/1387/6940" mimetype="image" mime-subtype="png"><alt-text>Image</alt-text></graphic></fig><p>Following the completion of the topology optimization process, the optimized shape was extracted as an Abaqus input (.inp) file, located within the topology optimization job directory. This crucial step facilitates the integration of the optimized shape into the model, a process visually depicted in <xref ref-type="fig" rid="figure-6">Figure 6</xref>. Subsequently, a crucial modification of the mesh configuration was undertaken, transitioning from triangular (tri) to tetrahedral (tet) elements. This transformation is essential for converting the optimized shape from a shell to a solid element format, thereby enabling the assignment of material properties to the newly optimized shape. The assembly of the model was facilitated by incorporating the obtained part instance into the assembly environment. This instance was automatically positioned at the specific location extracted from the optimization output, streamlining the integration of the topology-optimized component within the overall model framework. Subsequent to the assembly, kinematic coupling was established to maintain the structural integrity and functional interaction between the frame and the optimized link. This was achieved by selecting the entire surface of the optimized shape as the coupling region, effectively linking the control points of the frame to the surface of the optimized link.</p><fig id="figure-6" ignoredToc=""><label>Figure 6</label><caption><p>Sample of the extracted optimized shapes (source: by authors)</p></caption><graphic xlink:href="https://press.ierek.com/index.php/ESSD/article/download/1211/1387/6941" mimetype="image" mime-subtype="png"><alt-text>Image</alt-text></graphic></fig></sec><sec><title>2.4. Multi-story EBF</title><p>To model multi-story Eccentric Braced Frames (EBFs), the initial single-story model underwent duplication one or two times, thereby generating structures with two or three stories, respectively. In ensuring structural integrity and preventing out-of-plane movements, the beams and columns of the newly added frames were rigidly fixed. Additionally, to maintain the structural and functional coherence between the link and the frame across all stories, kinematic coupling was systematically applied. Consistent with the single-story model, a displacement of 56mm was imposed at the top corner of the EBF for each story, ensuring uniformity in the simulation parameters. The methodology for topology optimization was adapted for the multi-story context by introducing a cubic volume in the story designated for optimization, while retaining normal HEB links in the remaining stories. The validation of the optimized link was conducted through a comparative analysis between the results obtained by <xref ref-type="bibr" rid="BIBR-12">(Ramonell &amp; Chacón, 2021)</xref> and those derived from the HEB 160 model. This comparative evaluation is graphically represented in <xref ref-type="fig" rid="figure-7">Figure 7</xref>, demonstrating a congruence between the results. Such identical outcomes affirm the reliability and accuracy of the developed model.</p><fig id="figure-7" ignoredToc=""><label>Figure 7</label><caption><p>Validation for HEB and optimized links: a) force, displacement, b) plastic energy dissipation – displacement (source: by authors)</p></caption><graphic xlink:href="https://press.ierek.com/index.php/ESSD/article/download/1211/1387/6942" mimetype="image" mime-subtype="png"><alt-text>Image</alt-text></graphic></fig></sec></sec><sec><title>3. Pushover Analysis</title><p>The pushover analysis, conducted on each optimized link, was meticulously compared with the performance metrics of the conventional HEB links to evaluate enhancements or modifications in structural behavior. Notably, the analysis revealed that the performance improvements attributed to the optimized links were more pronounced in structures comprising two and three stories than in single-story configurations. This observation is particularly evident in the force-displacement curves, where, for single-story applications, the curves of optimized links closely approximated those of standard HEB sections, indicating a marginal performance differentiation. For the HEB 140 models, the comparative force-displacement curves are illustrated in <xref ref-type="fig" rid="figure-8">Figure 8</xref>. Furthermore, a comprehensive comparison encapsulating the performance outcomes of both optimized and conventional links is presented in  <xref ref-type="table" rid="table-hkds30">Table 2</xref>.</p><fig id="figure-8" ignoredToc=""><label>Figure 8</label><caption><p>HEB140 pushover analysis results: a) force, displacement, b) plastic energy dissipation – displacement (source: by authors)</p></caption><graphic xlink:href="https://press.ierek.com/index.php/ESSD/article/download/1211/1387/6943" mimetype="image" mime-subtype="png"><alt-text>Image</alt-text></graphic></fig><table-wrap id="table-hkds30" ignoredToc=""><label>Table 2</label><caption><p>Pushover analysis results</p></caption><table frame="box" rules="all"><thead><tr><th colspan="1" rowspan="1" style="" align="center" valign="middle">Story</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Effective yielding (<italic>N</italic>)</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">%</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Yielding displacement (mm)</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">%</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Effective stiffness (N/mm)</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">%</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Volume (mm<sup>3</sup>)</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">%</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Max. force (<italic>kN</italic>)</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">%</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Max. energy (<italic>KJ</italic>)</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">%</th></tr></thead><tbody><tr><td colspan="13" rowspan="1" style="" align="center" valign="middle">HEB 140</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">168,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">89.3</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">2</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">100.0</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">84,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">89.3</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">3,225,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">93.2</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">322</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">94.1</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">15,383</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">85.3</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">150,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">2</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">75,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">3,004,780</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">303</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">13,128</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">165,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">145.5</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">6</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">100.0</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">27,500</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">145.5</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">6,450,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">94.0</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">317</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">167.2</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">13,783</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">125.1</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">240,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">6</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">40,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">6,062,480</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">530</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">17,245</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">162,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">144.4</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">8</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">137.5</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">20,250</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">105.1</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">9,675,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">93.6</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">309</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">156.6</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">11,933</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">102.5</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">234,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">11</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">21,273</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">9,053,850</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">484</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">12,235</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="13" rowspan="1" style="" align="center" valign="middle">HEB 160</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">213,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">123.9</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">3</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">100.0</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">71,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">123.9</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">4,506,900</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">100.0</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">409</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">114.2</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">19,587</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">86.7</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">264,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">3</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">88,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">4,505,650</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">467</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">16,991</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">216,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">166.7</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">5</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">160.0</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">43,200</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">104.2</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">9,013,800</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">99.2</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">423</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">179.7</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">17,717</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">142.3</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">360,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">8</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">45,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">8,938,390</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">760</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">25,206</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">210,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">157.1</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">8</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">150.0</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">26,250</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">104.8</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">13,520,700</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">97.8</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">408</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">173.5</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">15,265</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">115.9</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">330,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">12</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">27,500</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">13,223,500</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">708</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">17,687</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="13" rowspan="1" style="" align="center" valign="middle">HEB 180</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">260,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">161.5</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">4</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">150.0</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">65,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">107.7</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">6,138,200</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">99.9</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">495</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">159.4</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">19,626</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">168.2</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">420,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">6</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">70,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">6,129,870</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">789</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">33,013</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">264,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">161.4</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">8</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">137.5</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">33,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">117.4</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">12,276,400</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">99.2</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">497</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">173.0</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">19,553</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">115.0</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">426,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">11</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">38,727</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">12,180,200</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">860</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">22,483</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">258,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">136.8</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">11</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">109.1</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">23,455</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">125.4</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">18,414,600</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">99.5</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">477</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">150.9</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">15,809</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">94.5</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">353,000</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">12</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">29,417</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">18,314,469</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">720</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">14,938</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr></tbody></table></table-wrap></sec><sec><title>4. Applied cyclic loading</title><p>The cyclic loading protocol adheres to the specifications outlined in the <xref ref-type="bibr" rid="BIBR-14">(Steel Construction, 2016)</xref> guidelines, utilizing predefined link rotational angles. These angles are set at 0.0025, 0.005, 0.01, 0.02, 0.03, 0.04, 0.05, 0.06, 0.07, 0.08, and 0.09. The protocol specifies that the first three angles undergo three loading cycles each, while the subsequent angles are subjected to two cycles. This approach ensures that the maximum rotational angle reaches 0.09, accommodating the typical range of shear link rotational angles, noted in the literature as spanning from 0.02 to 0.08. Given the known lengths of the link and the total beam for each model, a ratio—representing the division of the eccentric braced frame's length by the link's length—is calculated. Drift is then determined by dividing the link rotational angle by this ratio. Subsequently, displacement calculations are conducted by multiplying the height of the eccentric braced frame by the derived drift value. Furthermore, within the ABAQUS environment, the material's plastic hardening behavior is adjusted to a kinematic model. For each model, an amplitude is defined to facilitate the execution of the cyclic analysis, ensuring a rigorous and methodologically sound investigation into the structural dynamics of eccentric braced frames under cyclic loading conditions. The cyclic behavior was analyzed by obtaining the base shear for each model. From the base shear, an envelope is made to compare the behavior of the optimized shape and the normal HEB link. The energy dissipation coefficient is calculated using the area under the force-displacement curve and the two triangles OBE and ODF shown in <xref ref-type="fig" rid="figure-amzhs9">Figure 9</xref>. The effective stiffness (ke) is obtained by knowing the maximum and minimum forces and their corresponding displacements (FEMA 356, 2000). A methodological detail is also illustrated in Fig. 9. The viscous damping coefficient (he) is obtained using Eq. 1 as follows:</p><p>                                                                                                         <inline-formula><tex-math id="math-1"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h_e = \frac{1}{2\pi} \cdot \frac{S_{ABC} + S_{ADC}}{S_{BOE} + S_{DOF}} \end{document} ]]></tex-math></inline-formula></p><fig id="figure-amzhs9" ignoredToc=""><label>Figure 9</label><caption><p>a) Energy dissipation calculation method <xref ref-type="bibr" rid="BIBR-14">(Steel Construction, 2016)</xref>. b) Effective stiffness method <xref ref-type="bibr" rid="BIBR-15">(Agency, 2000)</xref></p></caption><graphic xlink:href="https://press.ierek.com/index.php/ESSD/article/download/1211/1387/6944" mimetype="image" mime-subtype="png"><alt-text>Image</alt-text></graphic></fig><p>The results show that while performance metrics such as effective stiffness and base shear capacity improved in optimized links. However, energy dissipation capacity and damping efficiency were reduced. Moreover, The cyclic analysis revealed a notable phenomenon where all optimized links exhibited a buckling effect, predominantly in one direction. This buckling, while not catastrophic, was consistently observed across various frame configurations and indicates a structural vulnerability introduced during the optimization process. The cause can be attributed to the redistribution of material away from regions that contribute to out-of-plane stiffness—a consequence of compliance-based topology optimization that does not inherently account for stability or local buckling resistance. While symmetry is often preserved in standard sections, the freedom allowed in topology optimization to remove material wherever deemed structurally redundant may lead to irregularities that, under dynamic conditions, act as triggers for instability. A sample of the force-displacement results for the HEB 140 links in the 2-storey model, illustrating this behavioral pattern, is graphically represented in <xref ref-type="fig" rid="figure-9">Figure 10</xref>. Additionally,  <xref ref-type="table" rid="table-0tuicu">Table 3</xref> consolidates the comprehensive outcomes derived from the cyclic analysis across all tested models.</p><fig id="figure-9" ignoredToc=""><label>Figure 10</label><caption><p>Cyclic Base shear response for (a) HEB 140 link (b) Opt. HEB 140 link (c) cyclic envelope for 2-storey EBF (source: by authors)</p></caption><graphic xlink:href="https://press.ierek.com/index.php/ESSD/article/download/1211/1387/6945" mimetype="image" mime-subtype="png"><alt-text>Image</alt-text></graphic></fig><table-wrap id="table-0tuicu" ignoredToc=""><label>Table 3</label><caption><p>Cyclic analysis results</p></caption><table frame="box" rules="all"><thead><tr><th colspan="1" rowspan="1" style="" align="center" valign="middle">Story</th><th colspan="1" rowspan="1" style="" align="center" valign="middle"><italic>K</italic><italic><sub>e</sub></italic> (<italic>N/m</italic>)</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">%</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Max. force (<italic>N</italic>)</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">%</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Min. force (<italic>N</italic>)</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">%</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">Energy dissipation</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">%</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">he</th><th colspan="1" rowspan="1" style="" align="center" valign="middle">%</th></tr></thead><tbody><tr><td colspan="11" rowspan="1" style="" align="center" valign="middle">HEB 140</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">10,302</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">101.9</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">307,853</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">96.7</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">358,631</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">114.6</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.855</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">82.2</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.454</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">82.3</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">10,501</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">297,841</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">410,882</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.348</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.374</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">5,110</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">145.8</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">319,126</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">142.7</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">346,766</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">157.3</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">3.01</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">75.3</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.489</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">73.8</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">7,448</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">455,458</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">545,365</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.268</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.361</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">3,351</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">129.6</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">323,685</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">109.6</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">342,450</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">152.6</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.879</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">62.7</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.458</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">62.7</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">4,342</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">354,610</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">522,683</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">1.806</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.287</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="11" rowspan="1" style="" align="center" valign="middle">HEB 160</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">11,695</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">174.9</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">401,947</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">161.1</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">465,769</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">185.7</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.94</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">65.8</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.468</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">65.8</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">20,459</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">647,607</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">864,903</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">1.934</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.308</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">5,927</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">180.3</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">417,403</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">171.6</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">453,089</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">192.1</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.975</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">77.9</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.473</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">78.0</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">10,689</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">716,336</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">870,296</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.319</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.369</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">3,942</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">159.8</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">422,490</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">142.1</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">447,451</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">181.3</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.949</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">73.0</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.469</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">73.0</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">6,299</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">600,161</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">811,064</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.153</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.343</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="11" rowspan="1" style="" align="center" valign="middle">HEB 180</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">12,298</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">169.5</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">482,327</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">163.3</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">555,358</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">174.6</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.926</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">78.7</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.466</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">78.7</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">1 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">20,845</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">787,750</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">969,471</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.302</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.366</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">6,378</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">143.8</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">497,079</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">133.0</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">539,269</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">164.6</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.873</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">71.5</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.457</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">71.5</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">2 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">9,170</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">661,136</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">887,603</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.053</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.327</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3 HEB</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">4,124</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">126.7</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">505,639</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">133.4</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">532,945</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">169.1</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">2.82</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">68.5</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.45</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">68.4</td></tr><tr><td colspan="1" rowspan="1" style="" align="center" valign="middle">3 OPT</td><td colspan="1" rowspan="1" style="" align="center" valign="middle">5,222</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">674,760</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">901,047</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">1.933</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/><td colspan="1" rowspan="1" style="" align="center" valign="middle">0.308</td><td colspan="1" rowspan="1" style="" align="center" valign="middle"/></tr></tbody></table></table-wrap></sec><sec><title>5. Conclusion</title><p>The integration of additive manufacturing and topology optimization opens new avenues for research, design, and construction of complex steel elements. This synergy promotes the creation of novel, complex structural sections and contributes to material conservation and environmental sustainability. Comparative analysis through pushover analysis between conventional HEB links and their optimized counterparts reveals significant findings. The optimized shapes demonstrate an increase in effective yielding force and a substantial enhancement in the base shear ultimate force across all models, with the sole exception of the HEB 140 one-story model, which closely parallels the performance of the standard HEB link. This enhancement translates into an augmented effective stiffness for the optimized configurations. Furthermore, plastic energy dissipation analysis indicates a comparable performance between the optimized and conventional HEB links. Cyclic performance analysis of the optimized shapes underscores a notable increase in the base shear ultimate force, reaffirming the structural benefits of the optimization.</p><p>Despite the improved stiffness and strength observed in the optimized shear links, the study revealed limitations related to directional buckling and reduced energy dissipation capacity under cyclic loading. These issues highlight the need to explore multi-objective topology optimization that incorporates structural stability requirements, fatigue performance criteria, and energy dissipation capacity. Additionally, experimental validation of the optimized geometries, especially under dynamic loading, is recommended to support practical implementation and improve design robustness.</p></sec><sec><title>Ackowledgment</title><p>The abstract of this paper was presented at the Environmental Design, Material Science, and Engineering Technologies (EDMSET) Conference -2nd Edition, which was held on the 22 <sup>nd </sup>-24 <sup>th </sup>of April 2025.</p><sec><title>Ethics Approval</title><p>Not applicable.</p></sec><sec><title>Conflict of Interest</title><p>The authors declare there is no conflict.</p></sec></sec></body><back><ref-list><title>References</title><ref id="BIBR-1"><element-citation publication-type="article-journal"><article-title>Additive manufacturing of concrete in construction: Potentials and challenges of 3D concrete printing</article-title><source>Virtual and Physical Prototyping</source><volume>11</volume><issue>3</issue><person-group 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