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<front>
<journal-meta>
<journal-id journal-id-type="pmc">SDHM</journal-id>
<journal-id journal-id-type="nlm-ta">SDHM</journal-id>
<journal-id journal-id-type="publisher-id">SDHM</journal-id>
<journal-title-group>
<journal-title>Structural Durability &#x0026; Health Monitoring</journal-title>
</journal-title-group>
<issn pub-type="epub">1930-2991</issn>
<issn pub-type="ppub">1930-2983</issn>
<publisher>
<publisher-name>Tech Science Press</publisher-name>
<publisher-loc>USA</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">63813</article-id>
<article-id pub-id-type="doi">10.32604/sdhm.2025.063813</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Article</subject>
</subj-group>
</article-categories>
<title-group>
<article-title>Calibration and Reliability Analysis of Eccentric Compressive Concrete Column with High Strength Rebars</article-title>
<alt-title alt-title-type="left-running-head">Calibration and Reliability Analysis of Eccentric Compressive Concrete Column with High Strength Rebars</alt-title>
<alt-title alt-title-type="right-running-head">Calibration and Reliability Analysis of Eccentric Compressive Concrete Column with High Strength Rebars</alt-title>
</title-group>
<contrib-group>
<contrib id="author-1" contrib-type="author">
<name name-style="western"><surname>Qin</surname><given-names>Baojun</given-names></name><xref ref-type="aff" rid="aff-1">1</xref><xref ref-type="aff" rid="aff-2">2</xref></contrib>
<contrib id="author-2" contrib-type="author">
<name name-style="western"><surname>Jiang</surname><given-names>Hong</given-names></name><xref ref-type="aff" rid="aff-1">1</xref><xref ref-type="aff" rid="aff-2">2</xref><xref ref-type="aff" rid="aff-3">3</xref></contrib>
<contrib id="author-3" contrib-type="author">
<name name-style="western"><surname>Zhang</surname><given-names>Wei</given-names></name><xref ref-type="aff" rid="aff-4">4</xref></contrib>
<contrib id="author-4" contrib-type="author" corresp="yes">
<name name-style="western"><surname>Liu</surname><given-names>Xiang</given-names></name><xref ref-type="aff" rid="aff-4">4</xref><email>liuxiang@fjut.edu.cn</email></contrib>
<aff id="aff-1"><label>1</label><institution>China Communications Construction Co., Ltd.</institution>, <addr-line>Beijing, 100088</addr-line>, <country>China</country></aff>
<aff id="aff-2"><label>2</label><institution>China Communications Construction Corporation Rail Transit Branch</institution>, <addr-line>Beijing, 102200</addr-line>, <country>China</country></aff>
<aff id="aff-3"><label>3</label><institution>China Communications (Tianjin) Rail Transit Investment and Construction Co., Ltd.</institution>, <addr-line>Tianjin, 300222</addr-line>, <country>China</country></aff>
<aff id="aff-4"><label>4</label><institution>School of Civil Engineering, Fujian University of Technology</institution>, <addr-line>Fuzhou, 350118</addr-line>, <country>China</country></aff>
</contrib-group>
<author-notes>
<corresp id="cor1"><label>&#x002A;</label>Corresponding Author: Xiang Liu. Email: <email>liuxiang@fjut.edu.cn</email></corresp>
</author-notes>
<pub-date date-type="collection" publication-format="electronic">
<year>2025</year>
</pub-date>
<pub-date date-type="pub" publication-format="electronic">
<day>05</day><month>09</month><year>2025</year>
</pub-date>
<volume>19</volume>
<issue>5</issue>
<fpage>1203</fpage>
<lpage>1220</lpage>
<history>
<date date-type="received">
<day>24</day>
<month>1</month>
<year>2025</year>
</date>
<date date-type="accepted">
<day>23</day>
<month>4</month>
<year>2025</year>
</date>
</history>
<permissions>
<copyright-statement>&#x00A9; 2025 The Authors.</copyright-statement>
<copyright-year>2025</copyright-year>
<copyright-holder>Published by Tech Science Press.</copyright-holder>
<license xlink:href="https://creativecommons.org/licenses/by/4.0/">
<license-p>This work is licensed under a <ext-link ext-link-type="uri" xlink:type="simple" xlink:href="https://creativecommons.org/licenses/by/4.0/">Creative Commons Attribution 4.0 International License</ext-link>, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.</license-p>
</license>
</permissions>
<self-uri content-type="pdf" xlink:href="_SDHM_63813.pdf"></self-uri>
<abstract>
<p>The utilization of high-strength steel bars (HSSB) within concrete structures demonstrates significant advantages in material conservation and mechanical performance enhancement. Nevertheless, existing design codes exhibit limitations in addressing the distinct statistical characteristics of HSSB, particularly regarding strength design parameters. For instance, GB50010-2010 fails to specify design strength values for reinforcement exceeding 600 MPa, creating technical barriers for advancing HSSB implementation. This study systematically investigates the reliability of eccentric compression concrete columns reinforced with 600 MPa-grade HSSB through high-order moment method analysis. Material partial factors were calibrated against target reliability indices prescribed by GB50068-2018, incorporating critical variables including live-to-dead load ratios, design methodologies, and service conditions. The findings show that the value of <italic>k</italic> significantly affects the calibration of material partial factors, impacting the reliability of bearing capacity. Considering various <italic>k</italic> values and target reliability indices, it is recommended that the material partial factor be set at 1.15, implying that the design strength for 600 MPa high-strength steel bars should be considered as 522 MPa. For safety levels I and II, load adjustment factors of 1.1 and 0.9, respectively, may be applied.</p>
</abstract>
<kwd-group kwd-group-type="author">
<kwd>Reliability</kwd>
<kwd>high-strength steel rebar</kwd>
<kwd>concrete column</kwd>
<kwd>material partial factor</kwd>
<kwd>high-order moment method</kwd>
<kwd>failure probability</kwd>
</kwd-group>
<funding-group>
<award-group id="awg1">
<funding-source>Natural Science Foundation of Fujian Province</funding-source>
<award-id>2022J05184</award-id>
</award-group>
</funding-group>
</article-meta>
</front>
<body>
<sec id="s1">
<label>1</label>
<title>Introduction</title>
<p>Recent advancements in steel manufacturing technology have enabled construction steel to achieve greater strength and ductility, resulting in high-performance materials that also contribute to material conservation in construction. Steel bars with a yield strength over 500 MPa are typically classified as high-strength steel bars (HSSB). The adoption of HSSBs could influence the mechanical properties of concrete member. Under the same reinforcement ratio, the use of HSSBs will cause a decrease in ductility, but it can reduce the reinforcement ratio to achieve the same ductility and reduce the use of materials. The price of HRB400 grade steel bars is about 5500 yuan/ton, and the price of HRB635 is about 7000 yuan/ton. The cost of HRB635 is about 27% higher than HRB400 grade, but its strength has increased by about 59%. By rational design, construction costs can be reduced.</p>
<p>The durability and deformation mode of HSSBs are similar to those of ordinary steel bars [<xref ref-type="bibr" rid="ref-1">1</xref>]. Consequently, researchers have explored the mechanical behavior of concrete elements containing HSSBs. For example, Zhang et al. [<xref ref-type="bibr" rid="ref-2">2</xref>] conducted a study on the seismic performance of concrete beam&#x2014;column joints that were strengthened. Luo and Li [<xref ref-type="bibr" rid="ref-3">3</xref>] examined the nonlinear behavior of concrete continuous beams with HSSBs, including their ductility and stiffness; Li et al. [<xref ref-type="bibr" rid="ref-4">4</xref>] performed eccentric loading tests on 12 circular tubed reinforced concrete columns, analyzing the effects of parameters such as the diameter to thickness ratio and load eccentricity on damage modes, load carrying capacity and ductility; Liao et al. [<xref ref-type="bibr" rid="ref-5">5</xref>] conducted an experimental study on the cyclic behavior of concrete columns with various transverse reinforcement configurations. Three designs of concrete columns with HSSBs, which included traditional closed-loop hoops, butt-welded loop hoops, and single closed-loop hoops with tie rods, were compared. Further studies on concrete members with HSSBs are listed in <xref ref-type="table" rid="table-1">Table 1</xref>. These research results all indicated that HSSBs have higher yield strength and ultimate strength, and their ductility is also better than ordinary steel bars.</p>
<table-wrap id="table-1">
<label>Table 1</label>
<caption>
<title>Some research on RC members with HSSB</title>
</caption>
<table>
<colgroup>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
</colgroup>
<thead>
<tr align="center">
<th align="center">Test</th>
<th align="center">Type of steel rebar</th>
<th align="center">Yield strength of steel rebar</th>
<th align="center">Ultimate strength of steel rebar</th>
<th align="center">Elongation (%)</th>
<th align="center">Citation</th>
</tr>
</thead>
<tbody>
<tr align="center">
<td>Concrete column under eccentric loading</td>
<td>Grade 600</td>
<td>833 MPa</td>
<td>1153 MPa</td>
<td>18</td>
<td>Alavi-Dehkordi and Mostofinejad [<xref ref-type="bibr" rid="ref-6">6</xref>]</td>
</tr>
<tr align="center">
<td>Seismic behavior of concrete beam-column joint</td>
<td>Grade 600</td>
<td>824 MPa</td>
<td>1132 MPa</td>
<td>24</td>
<td>Alavi-Dehkordi et al. [<xref ref-type="bibr" rid="ref-7">7</xref>]</td>
</tr>
<tr align="center">
<td>Seismic behavior of concrete column</td>
<td>ASTM A615 Grade 100</td>
<td>124 and 128 ksi</td>
<td>167.3 and 162 ksi</td>
<td>12.6 and 15.4</td>
<td>Aboukifa and Moustafa [<xref ref-type="bibr" rid="ref-8">8</xref>]</td>
</tr>
<tr align="center">
<td>Seismic behavior of concrete beam-column joint</td>
<td>HRB600</td>
<td>636 and 631 MPa</td>
<td>773 and 813 MPa</td>
<td>Not provide.</td>
<td>Guan et al. [<xref ref-type="bibr" rid="ref-9">9</xref>]</td>
</tr>
<tr align="center">
<td>Concrete column under axial and eccentric loading</td>
<td>ASTM A1035 Grade 100</td>
<td>810 MPa</td>
<td>935</td>
<td>Not provide.</td>
<td>Khalajestani et al. [<xref ref-type="bibr" rid="ref-10">10</xref>]</td>
</tr>
<tr align="center">
<td>The static and blast response of beam</td>
<td>ASTM A1035 Grade 690 MPa</td>
<td>855 MPa</td>
<td>Not provide.</td>
<td>Not provide.</td>
<td>Li and Aoude [<xref ref-type="bibr" rid="ref-11">11</xref>]</td>
</tr>
<tr align="center">
<td>Seismic behavior of concrete beam-column joint</td>
<td>HRB600</td>
<td>615 and 620 MPa</td>
<td>785 and 784 MPa</td>
<td>15 and 16</td>
<td>Zhang et al. [<xref ref-type="bibr" rid="ref-2">2</xref>]</td>
</tr>
<tr align="center">
<td rowspan="2">Cyclic behavior of concrete column</td>
<td>SD685</td>
<td>698 MPa</td>
<td>920 MPa</td>
<td>Not provide.</td>
<td rowspan="2">Liao et al. [<xref ref-type="bibr" rid="ref-5">5</xref>]</td>
</tr>
<tr align="center">
<td>SD785</td>
<td>886</td>
<td>1095</td>
<td>Not provide.</td>
</tr>
<tr align="center">
<td>Bending performance of concrete beams</td>
<td>HRB500</td>
<td>540 MPa</td>
<td>675 MPa</td>
<td>Not provide.</td>
<td>Zhang et al. [<xref ref-type="bibr" rid="ref-12">12</xref>]</td>
</tr>
<tr align="center">
<td>Concrete column under eccentric loading</td>
<td>HRB600</td>
<td>701 MPa</td>
<td>876 MPa</td>
<td>20.37</td>
<td>Du et al. [<xref ref-type="bibr" rid="ref-13">13</xref>]</td>
</tr>
<tr align="center">
<td>Concrete column under eccentric loading</td>
<td>HRB600</td>
<td>727, 737, 693 and 713 MPa</td>
<td>915, 932, 883 and 901 MPa</td>
<td>20.0, 19.5, 21.7, 21.8</td>
<td>Shao [<xref ref-type="bibr" rid="ref-14">14</xref>]</td>
</tr>
<tr align="center">
<td rowspan="2">Cyclic behavior of flexural members</td>
<td>HRB400</td>
<td>477 MPa</td>
<td>731 MPa</td>
<td>19</td>
<td rowspan="2">Hung and Chueh [<xref ref-type="bibr" rid="ref-15">15</xref>]</td>
</tr>
<tr align="center">
<td>HRB600</td>
<td>703 MPa</td>
<td>907 MPa</td>
<td>15</td>
</tr>
<tr align="center">
<td>Cooling rates on thermos mechanically process</td>
<td>BST 500S</td>
<td>696 MPa</td>
<td>756 MPa</td>
<td>14 and 17.72</td>
<td>Zaky et al. [<xref ref-type="bibr" rid="ref-16">16</xref>]</td>
</tr>
<tr align="center">
<td>The fracture behaviour of concrete prisms</td>
<td>Fe550</td>
<td>574 MPa</td>
<td>667 MPa</td>
<td>Not provide.</td>
<td>Krishnaa et al. [<xref ref-type="bibr" rid="ref-17">17</xref>]</td>
</tr>
<tr align="center">
<td>Anchorage performance strength rebars</td>
<td>HRB600</td>
<td>737.36, 693.88 and 713.51 MPa</td>
<td>931.93, 883.04 and 901.5 MPa</td>
<td>19.5, 21.73 and 21.86</td>
<td>Xu et al. [<xref ref-type="bibr" rid="ref-18">18</xref>]</td>
</tr>
<tr align="center">
<td>Seismic behavior of concrete columns</td>
<td>USD 685</td>
<td>961 MPa</td>
<td>1037 MPa</td>
<td>25.7</td>
<td>Wang et al. [<xref ref-type="bibr" rid="ref-19">19</xref>]</td>
</tr>
<tr align="center">
<td>Seismic behavior of shear walls</td>
<td>HRB600</td>
<td>612 MPa</td>
<td>837 MPa</td>
<td>13.8</td>
<td>Zhang et al. [<xref ref-type="bibr" rid="ref-20">20</xref>]</td>
</tr>
<tr align="center">
<td>Fatigue performance of steel rebars</td>
<td>HRB500</td>
<td>598</td>
<td>727</td>
<td>19</td>
<td>Sheng et al. [<xref ref-type="bibr" rid="ref-21">21</xref>]</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>When it comes to the widespread application of new construction materials in building and bridge structures, appropriate technical specifications or guidelines are essential. Regrettably, the current standards for HSSBs are lacking; they either do not exist or rely on existing guidelines, such as guideline GB50010-2010 [<xref ref-type="bibr" rid="ref-22">22</xref>], which does not specify a strength design value for steel bars with strengths above 600 MPa.</p>
<p>The construction process of structures inherently involves variability in material characteristics and component dimensions. Similarly, the live and dead loads that a structure bears during its operation are subject to randomness, affecting the reliability of structural safety. Consequently, modern design methods for buildings and highway bridges adopt the limit state design approach, anchored in reliability as the fundamental principle.</p>
<p>In reliability analysis, the simplest method entails the utilization of Monte Carlo simulation (MCS) to perform reliability assessments. Nevertheless, this method requires a considerably large quantity of samples, resulting in low analysis efficiency. Consequently, numerous researchers have explored various methods to improve reliability analysis efficiency. For example, Chen and Yang [<xref ref-type="bibr" rid="ref-23">23</xref>], as well as Li et al. [<xref ref-type="bibr" rid="ref-24">24</xref>,<xref ref-type="bibr" rid="ref-25">25</xref>], introduced a direct probability integration approach grounded in probability conservation for calculating structural reliability, and this method is characterized by its convenience, efficiency, and accuracy. Tong et al. [<xref ref-type="bibr" rid="ref-26">26</xref>] developed a fourth-order L-moments, and this method is easy to used and has applications in engineering reliability evaluation. Zhang et al. [<xref ref-type="bibr" rid="ref-27">27</xref>,<xref ref-type="bibr" rid="ref-28">28</xref>] developed an efficient outcrossing (GLO) method based on Gauss-Legendre quadrature. The main innovations of this method are twofold: first, it evaluates the cumulative failure probability using weighted sums of outcross rates over a limited number of moments- three to five- thus avoiding the time-consuming numerical integrations that require discretization over a large number of moments. Second, it offers an efficient algorithm to calculate the outcross rate, building on the recently developed system reliability method that draws from the well-established first order reliability method (FORM). Wang et al. [<xref ref-type="bibr" rid="ref-29">29</xref>] introduced a stochastic model that integrates the physical and mechanical models, accounting for the degradation effects of crack development and corrosion progression to estimate the failure probability of reinforced concrete structures over time. Tran et al. [<xref ref-type="bibr" rid="ref-30">30</xref>] developed an effective reliability analysis program and suggested a structural resistance factor for designing a steel-concrete composite frame system consisting of steel tube concrete columns and composite beams.</p>
<p>Nowadays, the limit state function method is the most commonly used design method in building and bridge construction [<xref ref-type="bibr" rid="ref-31">31</xref>,<xref ref-type="bibr" rid="ref-32">32</xref>]. To assess the reliability of structural design, the partial safety factor format (PSFF) and resistance reduction factor format (RRFF) are predominantly utilized. For instance, Zhang et al. [<xref ref-type="bibr" rid="ref-33">33</xref>] analyzed the flexural strength reliability of steel-fiber reinforced plastics beams and proposed material partial factors for FRP bars in such beams. Similarly, Zhang et al. [<xref ref-type="bibr" rid="ref-12">12</xref>] investigated the flexural performance of a concrete beam incorporating HSSBs and, based on reliability theory, the bearing capacity reduction factor for the beam was proposed.</p>
<p>Concrete columns have traditionally been designed as principal components, with eccentric compression being one of the main force modes for columns. Columns require higher reliability compared to beams, slabs, and other components. Therefore, the reliability of the reinforced concrete (RC) column with HSSB under eccentric compression was analyzed to propose the material partial factor for HSSB, offering a theoretical foundation for for the promotion of HSSB.</p>
</sec>
<sec id="s2">
<label>2</label>
<title>Resistance Model for Ultimate Force of HSSBCC under Eccentric Compression</title>
<p>Currently, the bearing capacity design of reinforced concrete columns is <bold>mainly applies</bold> the limit state method, and guidelines provide specific provisions for the eccentric bearing capacity design of RC columns. The failure mode of a RC column under eccentric loading with HSSB is similar to that of with ordinary steel rebars, as shown in <xref ref-type="fig" rid="fig-1">Fig. 1</xref>, therefore the calculation method recommended in GB50010-2010 [<xref ref-type="bibr" rid="ref-22">22</xref>] is employed.</p>
<fig id="fig-1">
<label>Figure 1</label>
<caption>
<title>Typical failure modes of RC column with HSSB under eccentric compression</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_63813-fig-1.tif"/>
</fig>
<p>When the length of the member is relatively long, and the second-order effect is significant due to a larger axial compression ratio in the eccentric compression member, it is essential to consider the <italic>P</italic>-<italic>&#x03B4;</italic> effect in the section design. The design value for the bending moment of the eccentric compression concrete column, considering the <italic>P</italic>-<italic>&#x03B4;</italic> effect, can be expressed as follows [<xref ref-type="bibr" rid="ref-22">22</xref>]:
<disp-formula id="eqn-1"><label>(1)</label><mml:math id="mml-eqn-1" display="block"><mml:mi>M</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mrow><mml:mtext>m</mml:mtext></mml:mrow></mml:mrow></mml:msub><mml:msub><mml:mi>&#x03B7;</mml:mi><mml:mrow><mml:mrow><mml:mtext>ns</mml:mtext></mml:mrow></mml:mrow></mml:msub><mml:msub><mml:mi>M</mml:mi><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:math></disp-formula>where <italic>C</italic><sub><italic>m</italic></sub> is the eccentricity adjustment coefficient.</p>
<p>There are two failure mode of large eccentric compression failure or small eccentric compression failure, depending on the design scheme and loading conditions. The calculation formula for large eccentric compression failure is as follows:
<disp-formula id="eqn-2"><label>(2)</label><mml:math id="mml-eqn-2" display="block"><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>&#x03B1;</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi>f</mml:mi><mml:mrow><mml:mrow><mml:mtext>c</mml:mtext></mml:mrow></mml:mrow></mml:msub><mml:mi>b</mml:mi><mml:mi>x</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi>f</mml:mi><mml:mrow><mml:mi>y</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi>A</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:msubsup><mml:mi>f</mml:mi><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:msubsup><mml:mi>A</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math></disp-formula>
<disp-formula id="eqn-3"><label>(3)</label><mml:math id="mml-eqn-3" display="block"><mml:mi>N</mml:mi><mml:mi>e</mml:mi><mml:mo>&#x2264;</mml:mo><mml:msub><mml:mi>&#x03B1;</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi>f</mml:mi><mml:mrow><mml:mrow><mml:mtext>c</mml:mtext></mml:mrow></mml:mrow></mml:msub><mml:mi>b</mml:mi><mml:mi>x</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>h</mml:mi><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:mfrac><mml:mi>x</mml:mi><mml:mn>2</mml:mn></mml:mfrac><mml:mo>)</mml:mo></mml:mrow><mml:mo>+</mml:mo><mml:mrow><mml:msubsup><mml:mi>f</mml:mi><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:msubsup><mml:mi>A</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>h</mml:mi><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:msubsup><mml:mi>a</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>where <italic>&#x03B1;</italic>1 represents the coefficient, <italic>f</italic><sub>c</sub> denotes the standard value of concrete strength, <italic>b</italic> stands for the width of the section. Additionally, <inline-formula id="ieqn-1"><mml:math id="mml-ieqn-1"><mml:mrow><mml:msubsup><mml:mi>f</mml:mi><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> and <inline-formula id="ieqn-2"><mml:math id="mml-ieqn-2"><mml:mrow><mml:msubsup><mml:mi>A</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> refer to the yield strength and area of the compressive steel bar, respectively. Meanwhile <italic>f</italic><sub><italic>y</italic></sub> and <italic>A</italic><sub><italic>s</italic></sub> respectively represent the yield strength and area of the tensile steel bar. <italic>x</italic> is the height of the compression zone, <italic>e</italic> is the distance between the axial force <italic>N</italic> and the center of the resultant force of the tensile steel bar, which can be expressed as:
<disp-formula id="eqn-4"><label>(4)</label><mml:math id="mml-eqn-4" display="block"><mml:mi>e</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mfrac><mml:mi>h</mml:mi><mml:mn>2</mml:mn></mml:mfrac><mml:mo>&#x2212;</mml:mo><mml:mi>a</mml:mi></mml:math></disp-formula>with
<disp-formula id="eqn-5"><label>(5)</label><mml:math id="mml-eqn-5" display="block"><mml:msub><mml:mi>e</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mrow><mml:mrow><mml:mtext>a</mml:mtext></mml:mrow></mml:mrow></mml:msub></mml:math></disp-formula>where <italic>e</italic><sub>0</sub> is the initial eccentricity.</p>
<p>The calculation formula of small eccentric compression failure is as follows:
<disp-formula id="eqn-6"><label>(6)</label><mml:math id="mml-eqn-6" display="block"><mml:mi>N</mml:mi><mml:mo>&#x2264;</mml:mo><mml:msub><mml:mi>&#x03B1;</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi>f</mml:mi><mml:mrow><mml:mrow><mml:mtext>c</mml:mtext></mml:mrow></mml:mrow></mml:msub><mml:mi>b</mml:mi><mml:mi>x</mml:mi><mml:mo>+</mml:mo><mml:mrow><mml:msubsup><mml:mi>f</mml:mi><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:msubsup><mml:mi>A</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi>A</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:math></disp-formula>
<disp-formula id="eqn-7"><label>(7)</label><mml:math id="mml-eqn-7" display="block"><mml:mi>N</mml:mi><mml:mi>e</mml:mi><mml:mo>&#x2264;</mml:mo><mml:msub><mml:mi>&#x03B1;</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi>f</mml:mi><mml:mrow><mml:mrow><mml:mtext>c</mml:mtext></mml:mrow></mml:mrow></mml:msub><mml:mi>b</mml:mi><mml:mi>x</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>h</mml:mi><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:mfrac><mml:mi>x</mml:mi><mml:mn>2</mml:mn></mml:mfrac><mml:mo>)</mml:mo></mml:mrow><mml:mo>+</mml:mo><mml:mrow><mml:msubsup><mml:mi>f</mml:mi><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:msubsup><mml:mi>A</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>h</mml:mi><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:msubsup><mml:mi>a</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2032;</mml:mi></mml:mrow></mml:msubsup></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>where <italic>&#x03C3;</italic><sub>s</sub> is the stress of the tensile steel bar, which can be determined by the strain <italic>&#x03B5;</italic><sub><italic>s</italic></sub> of the tensile steel bar from the assumption of the plane section, and then determined by <inline-formula id="ieqn-3"><mml:math id="mml-ieqn-3"><mml:msub><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mrow><mml:mtext>s</mml:mtext></mml:mrow></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>&#x03B5;</mml:mi><mml:mrow><mml:mrow><mml:mtext>s</mml:mtext></mml:mrow></mml:mrow></mml:msub><mml:msub><mml:mi>E</mml:mi><mml:mrow><mml:mrow><mml:mtext>s</mml:mtext></mml:mrow></mml:mrow></mml:msub></mml:math></inline-formula>.</p>
</sec>
<sec id="s3">
<label>3</label>
<title>Estimation of the Statistical Parameters of the Resistance Models</title>
<sec id="s3_1">
<label>3.1</label>
<title>Mode Uncertainty</title>
<p>Structural engineering, being a blend of empirical and theoretical approaches, relies on certain fundamental assumptions for calculating the eccentric compressive capacity of RC columns. Coefficients derived from experimental data introduce uncertainties into the calculation mode, making the calculation error a stochastic variable. To ascertain the statistical characteristics of uncertainty and model error in the calculation mode for the eccentric compressive capacity of RCCs with HSSB, 37 datasets were analyzed, as presented in <xref ref-type="table" rid="table-2">Table 2</xref>. The model error <italic>&#x03BC;</italic> can be expressed as [<xref ref-type="bibr" rid="ref-33">33</xref>]:
<disp-formula id="eqn-8"><label>(8)</label><mml:math id="mml-eqn-8" display="block"><mml:mi>&#x03BC;</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:msub><mml:mi>N</mml:mi><mml:mrow><mml:mi>t</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi>N</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mi>r</mml:mi><mml:mi>e</mml:mi></mml:mrow></mml:msub></mml:mfrac></mml:math></disp-formula>where <italic>N</italic><sub><italic>test</italic></sub> and <italic>N</italic><sub><italic>pre</italic></sub> denote the test value and theoretical value of concrete column under eccentric compression.</p>
<table-wrap id="table-2">
<label>Table 2</label>
<caption>
<title>Uncertainty of calculation model</title>
</caption>
<table>
<colgroup>
<col/>
<col/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col/>
</colgroup>
<thead>
<tr align="center">
<th>No.</th>
<th>Specimen</th>
<th align="center">Width (mm)</th>
<th align="center">Height (mm)</th>
<th align="center">a<sub>s</sub> (mm)</th>
<th align="center"><italic>n</italic></th>
<th align="center"><italic>d</italic> (mm)</th>
<th align="center"><italic>f</italic><sub><italic>y</italic></sub> (MPa)</th>
<th align="center"><italic>f</italic><sub><italic>c</italic></sub> (MPa)</th>
<th align="center">e0 (mm)</th>
<th align="center"><italic>N</italic><sub><bold><italic>test</italic></bold></sub> (kN)</th>
<th align="center"><italic>N</italic><sub><bold><italic>pre</italic></bold></sub> (kN)</th>
<th><italic><bold>&#x03BC;</bold></italic></th>
<th>Reference</th>
</tr>
</thead>
<tbody>
<tr align="center">
<td>1</td>
<td>EC1-1</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>16</td>
<td>633</td>
<td>32.67</td>
<td>270</td>
<td>1779</td>
<td>1156</td>
<td>0.65</td>
<td rowspan="9">Wang et al. [<xref ref-type="bibr" rid="ref-34">34</xref>]</td>
</tr>
<tr align="center">
<td>2</td>
<td>EC1-2</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>22</td>
<td>633</td>
<td>32.67</td>
<td>270</td>
<td>2192</td>
<td>1705</td>
<td>0.78</td>
</tr>
<tr align="center">
<td>3</td>
<td>EC1-3</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>25</td>
<td>633</td>
<td>32.67</td>
<td>270</td>
<td>2279</td>
<td>1963</td>
<td>0.86</td>
</tr>
<tr align="center">
<td>4</td>
<td>EC3-1</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>16</td>
<td>633</td>
<td>32.67</td>
<td>220</td>
<td>2404</td>
<td>1599</td>
<td>0.67</td>
</tr>
<tr align="center">
<td>5</td>
<td>EC3-2</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>16</td>
<td>633</td>
<td>32.67</td>
<td>320</td>
<td>1289</td>
<td>856</td>
<td>0.66</td>
</tr>
<tr align="center">
<td>6</td>
<td>EC4-1</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>16</td>
<td>633</td>
<td>32.67</td>
<td>270</td>
<td>1719</td>
<td>1156</td>
<td>0.67</td>
</tr>
<tr align="center">
<td>7</td>
<td>EC5-1</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>16</td>
<td>633</td>
<td>27.76</td>
<td>270</td>
<td>1524</td>
<td>1087</td>
<td>0.71</td>
</tr>
<tr align="center">
<td>8</td>
<td>EC5-2</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>22</td>
<td>633</td>
<td>27.76</td>
<td>270</td>
<td>1992</td>
<td>1595</td>
<td>0.80</td>
</tr>
<tr align="center">
<td>9</td>
<td>EC6-1</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>16</td>
<td>633</td>
<td>20.9</td>
<td>270</td>
<td>1364</td>
<td>973</td>
<td>0.71</td>
</tr>
<tr align="center">
<td>10</td>
<td>HRCC-1</td>
<td>300</td>
<td>400</td>
<td>42</td>
<td>2</td>
<td>25</td>
<td>540</td>
<td>36.1</td>
<td>250</td>
<td>1369</td>
<td>1292</td>
<td>0.94</td>
<td rowspan="6">Zhang et al. [<xref ref-type="bibr" rid="ref-35">35</xref>]</td>
</tr>
<tr align="center">
<td>11</td>
<td>HRCC-2</td>
<td>300</td>
<td>400</td>
<td>42</td>
<td>3</td>
<td>25</td>
<td>540</td>
<td>36.1</td>
<td>250</td>
<td>1418</td>
<td>1694</td>
<td>1.19</td>
</tr>
<tr align="center">
<td>12</td>
<td>HRCC-3</td>
<td>300</td>
<td>400</td>
<td>42</td>
<td>2</td>
<td>25</td>
<td>540</td>
<td>48.1</td>
<td>250</td>
<td>1304</td>
<td>1409</td>
<td>1.08</td>
</tr>
<tr align="center">
<td>13</td>
<td>HRCC-4</td>
<td>300</td>
<td>400</td>
<td>42</td>
<td>3</td>
<td>25</td>
<td>540</td>
<td>48.1</td>
<td>300</td>
<td>1316</td>
<td>1469</td>
<td>1.12</td>
</tr>
<tr align="center">
<td>14</td>
<td>HRCC-5</td>
<td>300</td>
<td>400</td>
<td>42</td>
<td>2</td>
<td>25</td>
<td>540</td>
<td>36.1</td>
<td>300</td>
<td>1073</td>
<td>1006</td>
<td>0.94</td>
</tr>
<tr align="center">
<td>15</td>
<td>HRCC-6</td>
<td>300</td>
<td>400</td>
<td>42</td>
<td>3</td>
<td>25</td>
<td>540</td>
<td>36.1</td>
<td>300</td>
<td>1411</td>
<td>1370</td>
<td>0.97</td>
</tr>
<tr align="center">
<td>16</td>
<td>PZ1</td>
<td>200</td>
<td>350</td>
<td>30</td>
<td>2</td>
<td>18</td>
<td>700.79</td>
<td>33.1</td>
<td>100</td>
<td>1791</td>
<td>1470</td>
<td>0.82</td>
<td rowspan="9">Du et al. [<xref ref-type="bibr" rid="ref-13">13</xref>]</td>
</tr>
<tr align="center">
<td>17</td>
<td>PZ2</td>
<td>200</td>
<td>350</td>
<td>30</td>
<td>2</td>
<td>18</td>
<td>700.79</td>
<td>33.1</td>
<td>210</td>
<td>1023</td>
<td>852</td>
<td>0.83</td>
</tr>
<tr align="center">
<td>18</td>
<td>PZ3</td>
<td>200</td>
<td>350</td>
<td>30</td>
<td>2</td>
<td>18</td>
<td>700.79</td>
<td>33.1</td>
<td>230</td>
<td>877</td>
<td>774</td>
<td>0.88</td>
</tr>
<tr align="center">
<td>19</td>
<td>PZ4</td>
<td>200</td>
<td>350</td>
<td>30</td>
<td>2</td>
<td>20</td>
<td>700.79</td>
<td>33.1</td>
<td>130</td>
<td>1521</td>
<td>1354</td>
<td>0.89</td>
</tr>
<tr align="center">
<td>20</td>
<td>PZ5</td>
<td>200</td>
<td>350</td>
<td>30</td>
<td>2</td>
<td>20</td>
<td>700.79</td>
<td>33.1</td>
<td>230</td>
<td>866</td>
<td>878</td>
<td>1.01</td>
</tr>
<tr align="center">
<td>21</td>
<td>PZ6</td>
<td>200</td>
<td>350</td>
<td>30</td>
<td>2</td>
<td>20</td>
<td>700.79</td>
<td>33.1</td>
<td>250</td>
<td>690</td>
<td>815</td>
<td>1.18</td>
</tr>
<tr align="center">
<td>22</td>
<td>PZ7</td>
<td>200</td>
<td>350</td>
<td>30</td>
<td>2</td>
<td>22</td>
<td>700.79</td>
<td>33.1</td>
<td>130</td>
<td>1560</td>
<td>1467</td>
<td>0.94</td>
</tr>
<tr align="center">
<td>23</td>
<td>PZ8</td>
<td>200</td>
<td>350</td>
<td>30</td>
<td>2</td>
<td>22</td>
<td>700.79</td>
<td>33.1</td>
<td>250</td>
<td>833</td>
<td>908</td>
<td>1.09</td>
</tr>
<tr align="center">
<td>24</td>
<td>PZ9</td>
<td>200</td>
<td>350</td>
<td>30</td>
<td>2</td>
<td>22</td>
<td>700.79</td>
<td>33.1</td>
<td>260</td>
<td>834</td>
<td>878</td>
<td>1.05</td>
</tr>
<tr align="center">
<td>25</td>
<td>HHRC-R4-Eh01</td>
<td>250</td>
<td>350</td>
<td>25</td>
<td>3</td>
<td>14/16</td>
<td>727.2</td>
<td>35.33</td>
<td>87.5</td>
<td>2498</td>
<td>1975</td>
<td>0.79</td>
<td rowspan="13">Shao [<xref ref-type="bibr" rid="ref-14">14</xref>]</td>
</tr>
<tr align="center">
<td>26</td>
<td>HHRC-S4-E02</td>
<td>300</td>
<td>300</td>
<td>25</td>
<td>3</td>
<td>14/16</td>
<td>727.2</td>
<td>35.33</td>
<td>75</td>
<td>2401</td>
<td>1956</td>
<td>0.81</td>
</tr>
<tr align="center">
<td>27</td>
<td>HHRC-R4-Eh11</td>
<td>250</td>
<td>350</td>
<td>25</td>
<td>3</td>
<td>14/16</td>
<td>727.2</td>
<td>35.33</td>
<td>0</td>
<td>3632</td>
<td>3397</td>
<td>0.94</td>
</tr>
<tr align="center">
<td>28</td>
<td>HHRC-R4-Eh12</td>
<td>250</td>
<td>350</td>
<td>25</td>
<td>3</td>
<td>14/16</td>
<td>727.2</td>
<td>35.33</td>
<td>43.75</td>
<td>2903</td>
<td>2597</td>
<td>0.89</td>
</tr>
<tr align="center">
<td>29</td>
<td>HHRC-R4-Eh13</td>
<td>250</td>
<td>350</td>
<td>25</td>
<td>3</td>
<td>14/16</td>
<td>727.2</td>
<td>35.33</td>
<td>131.25</td>
<td>1885</td>
<td>1522</td>
<td>0.81</td>
</tr>
<tr align="center">
<td>30</td>
<td>HHRC-R4-Eh14</td>
<td>250</td>
<td>350</td>
<td>25</td>
<td>3</td>
<td>14/16</td>
<td>727.2</td>
<td>35.33</td>
<td>175</td>
<td>1559</td>
<td>1203</td>
<td>0.77</td>
</tr>
<tr align="center">
<td>31</td>
<td>HHRC-R4-Eh15</td>
<td>250</td>
<td>350</td>
<td>25</td>
<td>3</td>
<td>14/16</td>
<td>727.2</td>
<td>35.33</td>
<td>262.5</td>
<td>938.4</td>
<td>742</td>
<td>0.79</td>
</tr>
<tr align="center">
<td>32</td>
<td>HHRC-S4-E11</td>
<td>300</td>
<td>300</td>
<td>25</td>
<td>3</td>
<td>14/16</td>
<td>727.2</td>
<td>35.33</td>
<td>0</td>
<td>3795</td>
<td>3401</td>
<td>0.90</td>
</tr>
<tr align="center">
<td>33</td>
<td>HHRC-S4-E12</td>
<td>300</td>
<td>300</td>
<td>25</td>
<td>3</td>
<td>14/16</td>
<td>727.2</td>
<td>35.33</td>
<td>112.5</td>
<td>2042</td>
<td>1501</td>
<td>0.73</td>
</tr>
<tr align="center">
<td>34</td>
<td>HHRC-S4-E13</td>
<td>300</td>
<td>300</td>
<td>25</td>
<td>3</td>
<td>14/16</td>
<td>727.2</td>
<td>35.33</td>
<td>150</td>
<td>1608</td>
<td>1183</td>
<td>0.74</td>
</tr>
<tr align="center">
<td>35</td>
<td>HHRC-R4-Eh21</td>
<td>250</td>
<td>350</td>
<td>25</td>
<td>2</td>
<td>14</td>
<td>727.2</td>
<td>35.33</td>
<td>87.5</td>
<td>2126</td>
<td>1737</td>
<td>0.82</td>
</tr>
<tr align="center">
<td>36</td>
<td>HHRC-R4-Eh22</td>
<td>250</td>
<td>350</td>
<td>25</td>
<td>4</td>
<td>14/16</td>
<td>727.2</td>
<td>35.33</td>
<td>87.5</td>
<td>2672</td>
<td>2185</td>
<td>0.82</td>
</tr>
<tr align="center">
<td>37</td>
<td>HHRC-R4-Eh41</td>
<td>210</td>
<td>420</td>
<td>25</td>
<td>3</td>
<td>14/16</td>
<td>727.2</td>
<td>35.33</td>
<td>105</td>
<td>2568</td>
<td>2045</td>
<td>0.80</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The comparison between the experimental results and the theoretical estimations is illustrated in <xref ref-type="fig" rid="fig-2">Fig. 2</xref>. Most of the results obtained by the bearing capacity calculation formulas (predicted values) are larger than the real values (test values). Among the 37 samples, only 7 samples had predicted values that were lower than the measured values. This indicates that the prediction model shows a trend of producing unsafe estimates.</p>
<fig id="fig-2">
<label>Figure 2</label>
<caption>
<title>Comparison between predicted model calculation results and experimental results [<xref ref-type="bibr" rid="ref-4">4</xref>,<xref ref-type="bibr" rid="ref-14">14</xref>,<xref ref-type="bibr" rid="ref-18">18</xref>,<xref ref-type="bibr" rid="ref-34">34</xref>]</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_63813-fig-2.tif"/>
</fig>
<p><xref ref-type="fig" rid="fig-3">Fig. 3</xref> displays the probability density function (PDF) of the model error <italic>&#x03BC;</italic>, which follows a distribution with a mean value of 1.18, a standard deviation of 0.19, and a coefficient of variation of 0.16. Compared to bending components, the model for the compressive capacity of RC concrete shows more variability when using HSSB [<xref ref-type="bibr" rid="ref-12">12</xref>].</p>
<fig id="fig-3">
<label>Figure 3</label>
<caption>
<title>PDF of model error</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_63813-fig-3.tif"/>
</fig>
</sec>
<sec id="s3_2">
<label>3.2</label>
<title>Parameter Uncertainty</title>
<p>In the limit state design approach for reinforced concrete elements, the randomness primarily arises from two aspects: structural parameters and load variables. In the estimation of the eccentric compressive bearing capacity of RC columns, variables such as cross-sectional size, concrete strength, reinforcement strength, reinforcement area, eccentricity, and slenderness ratio have most influence on the bearing capacity. Thus, cross-sectional size, concrete strength, reinforcement strength, and reinforcement area are treated as random variables. For load parameters, including dead and live loads, both are also regarded as random variables. Based on the compiled data in <xref ref-type="table" rid="table-2">Table 2</xref>, the yield strength bias of HSSB is 1.17, with a coefficient of variation of 0.096. The statistical details for each random variable are provided in <xref ref-type="table" rid="table-3">Table 3</xref>.</p>
<table-wrap id="table-3">
<label>Table 3</label>
<caption>
<title>Statistical characteristics of random variables</title>
</caption>
<table>
<colgroup>
<col/>
<col/>
<col/>
<col/>
<col/>
</colgroup>
<thead>
<tr align="center">
<th>Random variable</th>
<th>Bias</th>
<th>COV</th>
<th>Distribution</th>
<th>Reference</th>
</tr>
</thead>
<tbody>
<tr align="center">
<td>Section width/section height</td>
<td>1.00</td>
<td>0.02</td>
<td>Normal</td>
<td>Lu et al. [<xref ref-type="bibr" rid="ref-36">36</xref>]</td>
</tr>
<tr align="center">
<td>Strength of concrete</td>
<td>1.15</td>
<td>0.15</td>
<td>Lognormal</td>
<td>Ribeiro and Diniz [<xref ref-type="bibr" rid="ref-37">37</xref>]</td>
</tr>
<tr align="center">
<td>Area of reinforcement</td>
<td>1.00</td>
<td>0.03</td>
<td>Normal</td>
<td>Lu et al. [<xref ref-type="bibr" rid="ref-36">36</xref>]</td>
</tr>
<tr align="center">
<td>Dead load</td>
<td>1.06</td>
<td>0.075</td>
<td>Normal</td>
<td>GB50068-2018 [<xref ref-type="bibr" rid="ref-38">38</xref>]</td>
</tr>
<tr align="center">
<td>Live load (house)</td>
<td>0.644</td>
<td>0.233</td>
<td>Extreme type I</td>
<td>GB50068-2018 [<xref ref-type="bibr" rid="ref-38">38</xref>]</td>
</tr>
<tr align="center">
<td>Dead load (office)</td>
<td>0.524</td>
<td>0.288</td>
<td>Extreme type I</td>
<td>GB50068-2018 [<xref ref-type="bibr" rid="ref-38">38</xref>]</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</sec>
<sec id="s4">
<label>4</label>
<title>Reliability Theory</title>
<sec id="s4_1">
<label>4.1</label>
<title>Statistical Moment Calculation</title>
<p>Suppose p(x) denotes the probability density function of a continuous random variable <italic>Y</italic> &#x003D; <italic>G</italic>(<bold>X</bold>). As defined in [<xref ref-type="bibr" rid="ref-39">39</xref>], its mean value <italic>M</italic><sub>1</sub> and <italic>k</italic>-th central moments <italic>M</italic><sub><italic>k</italic></sub> are expressed as follows:
<disp-formula id="eqn-9"><label>(9)</label><mml:math id="mml-eqn-9" display="block"><mml:msub><mml:mi>M</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mi>G</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext mathvariant="bold">X</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:msubsup><mml:mo>&#x222B;</mml:mo><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi mathvariant="normal">&#x221E;</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x221E;</mml:mi></mml:mrow></mml:msubsup><mml:mi>G</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext mathvariant="bold">X</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mi>p</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext mathvariant="bold">X</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mi>d</mml:mi><mml:mrow><mml:mtext mathvariant="bold">X</mml:mtext></mml:mrow></mml:math></disp-formula>
<disp-formula id="eqn-10"><label>(10)</label><mml:math id="mml-eqn-10" display="block"><mml:msub><mml:mi>M</mml:mi><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msubsup><mml:mo>&#x222B;</mml:mo><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi mathvariant="normal">&#x221E;</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x221E;</mml:mi></mml:mrow></mml:msubsup><mml:msup><mml:mrow><mml:mo>[</mml:mo><mml:mi>G</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext mathvariant="bold">X</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi>&#x03BC;</mml:mi><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:msup><mml:mi>p</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext mathvariant="bold">X</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mi>d</mml:mi><mml:mrow><mml:mtext mathvariant="bold">X</mml:mtext></mml:mrow><mml:mrow><mml:mtext>&#xA0;for</mml:mtext></mml:mrow><mml:mrow><mml:mtext>k</mml:mtext></mml:mrow><mml:mo>&#x2265;</mml:mo><mml:mn>2</mml:mn></mml:math></disp-formula></p>
<p>As the random variable <italic>Y</italic> includes multiple variables, the statistical moments of <italic>G</italic>(<bold>X</bold>) cannot be acquired directly. In such instances, dimensionality reduction is performed as described in Rahman and Xu [<xref ref-type="bibr" rid="ref-40">40</xref>]. When a function contains <italic>n</italic> random variables, it can be resolved into <italic>s</italic>-dimensional random variable functions <italic>G</italic><sup><italic>s</italic></sup>(<italic>X</italic>), as shown below:
<disp-formula id="eqn-11"><label>(11)</label><mml:math id="mml-eqn-11" display="block"><mml:mi>G</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext mathvariant="bold">X</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2245;</mml:mo><mml:msup><mml:mi>G</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext mathvariant="bold">X</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>0</mml:mn></mml:mrow><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:munderover><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msup><mml:msubsup><mml:mi>C</mml:mi><mml:mrow><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mi>s</mml:mi><mml:mo>+</mml:mo><mml:mi>i</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msubsup><mml:munder><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>&#x003C;</mml:mo><mml:mo>&#x22EF;</mml:mo><mml:mo>&#x003C;</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mrow><mml:mi>s</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:munder><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>s</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:math></disp-formula>where <italic>s</italic> &#x003C; <italic>n</italic>, and <inline-formula id="ieqn-4"><mml:math id="mml-ieqn-4"><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>s</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>G</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mo>&#x22EF;</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mo>&#x22EF;</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mrow><mml:mi>c</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mrow><mml:mi>c</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mrow><mml:mi>c</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mo>&#x22EF;</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>; c is a reference point, and it equals to <inline-formula id="ieqn-5"><mml:math id="mml-ieqn-5"><mml:mrow><mml:mo>[</mml:mo><mml:mtable columnalign="left left left left" rowspacing="4pt" columnspacing="1em"><mml:mtr><mml:mtd><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo></mml:mtd><mml:mtd><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo></mml:mtd><mml:mtd><mml:mo>&#x22EF;</mml:mo></mml:mtd><mml:mtd><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>.</p>
<p>When s &#x003D; 2, the multivariate function problem is transformed into a problem of combining multiple univariate functions, and then <xref ref-type="disp-formula" rid="eqn-14">Eq. (14)</xref> transform to the following formula:
<disp-formula id="eqn-12"><label>(12)</label><mml:math id="mml-eqn-12" display="block"><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext mathvariant="bold">X</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2245;</mml:mo><mml:msup><mml:mi>g</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext mathvariant="bold">X</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:munderover><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>c</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>with
<disp-formula id="eqn-13"><label>(13)</label><mml:math id="mml-eqn-13" display="block"><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mrow><mml:mtext mathvariant="bold">X</mml:mtext></mml:mrow><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mo>&#x22EF;</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mo>&#x22EF;</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula></p>
<p>This indicates that except the <italic>i</italic>-th variable, all other variables maintain their corresponding values at the reference point.</p>
<p>Through the substituting <xref ref-type="disp-formula" rid="eqn-15">Eq. (15)</xref> into <xref ref-type="disp-formula" rid="eqn-12">Eqs. (12)</xref> and <xref ref-type="disp-formula" rid="eqn-13">(13)</xref>, the statistical moment of the dimensionality reduced random variable <italic>Y</italic> can be obtained as follows:
<disp-formula id="eqn-14"><label>(14)</label><mml:math id="mml-eqn-14" display="block"><mml:mi>&#x03BC;</mml:mi><mml:mo>=</mml:mo><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:munderover><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>c</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>&#x2245;</mml:mo><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:munderover><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>c</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>
<disp-formula id="eqn-15"><label>(15)</label><mml:math id="mml-eqn-15" display="block"><mml:mtable columnalign="right left right left right left right left right left right left" rowspacing="3pt" columnspacing="0em 2em 0em 2em 0em 2em 0em 2em 0em 2em 0em" displaystyle="true"><mml:mtr><mml:mtd><mml:msub><mml:mi>M</mml:mi><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2245;</mml:mo><mml:mtext>&#x00A0;</mml:mtext></mml:mtd><mml:mtd><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:munderover><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:mi>&#x03BC;</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:msup><mml:mrow><mml:mo>[</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>c</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi>&#x03BC;</mml:mi><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mo>=</mml:mo></mml:mtd><mml:mtd><mml:mi></mml:mi><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:munderover><mml:mi>E</mml:mi><mml:mrow><mml:mo>{</mml:mo><mml:msup><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi>&#x03BC;</mml:mi><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mo>}</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:msup><mml:mrow><mml:mo>[</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>c</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi>&#x03BC;</mml:mi><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mn>2</mml:mn><mml:mo>,</mml:mo><mml:mn>3</mml:mn><mml:mo>,</mml:mo><mml:mn>4</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p>
<p>When the random variables in <italic>G</italic>(<italic>X</italic>) follow a normal distribution, <inline-formula id="ieqn-6"><mml:math id="mml-ieqn-6"><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula id="ieqn-7"><mml:math id="mml-ieqn-7"><mml:mi>E</mml:mi><mml:mrow><mml:mo>{</mml:mo><mml:msup><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi>&#x03BC;</mml:mi><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mo>}</mml:mo></mml:mrow></mml:math></inline-formula> can be evaluated through Gaussian-Hermite integration and expressed as:
<disp-formula id="eqn-16"><label>(16)</label><mml:math id="mml-eqn-16" display="block"><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>l</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>r</mml:mi></mml:mrow></mml:munderover><mml:mfrac><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mrow><mml:mtext>GH</mml:mtext></mml:mrow><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:msqrt><mml:mi>&#x03C0;</mml:mi></mml:msqrt></mml:mfrac><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mrow><mml:mtext>GH</mml:mtext></mml:mrow><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>
<disp-formula id="eqn-17"><label>(17)</label><mml:math id="mml-eqn-17" display="block"><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi>&#x03BC;</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>l</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>r</mml:mi></mml:mrow></mml:munderover><mml:mfrac><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mrow><mml:mtext>GH</mml:mtext></mml:mrow><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:msqrt><mml:mi>&#x03C0;</mml:mi></mml:msqrt></mml:mfrac><mml:msup><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mrow><mml:mtext>GH</mml:mtext></mml:mrow><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mi>&#x03BC;</mml:mi><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup></mml:math></disp-formula>where <italic>r</italic> represents the number of integration point; <italic>x</italic><sub><italic>GH</italic>,<italic>l</italic></sub> and <italic>w</italic><sub><italic>GH</italic>,<italic>l</italic></sub> denote the integration point and the weight of Gaussian-Hermite, respectively, with detailed values available in references.</p>
<p>For s &#x003D; 2, the multivariate function problem reduces to combining univariate functions, and then <xref ref-type="disp-formula" rid="eqn-14">Eq. (14)</xref> transform to the following formula [<xref ref-type="bibr" rid="ref-39">39</xref>]:
<disp-formula id="eqn-18"><label>(18)</label><mml:math id="mml-eqn-18" display="block"><mml:msub><mml:mi>M</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>&#x2248;</mml:mo><mml:munder><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>l</mml:mi><mml:mo>&#x003C;</mml:mo><mml:mi>m</mml:mi></mml:mrow></mml:munder><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>m</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>2</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:munderover><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>+</mml:mo><mml:mfrac><mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mn>2</mml:mn></mml:mfrac><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula><disp-formula id="eqn-19"><label>(19)</label><mml:math id="mml-eqn-19" display="block"><mml:mtable columnalign="right left right left right left right left right left right left" rowspacing="3pt" columnspacing="0em 2em 0em 2em 0em 2em 0em 2em 0em 2em 0em" displaystyle="true"><mml:mtr><mml:mtd><mml:msub><mml:mi>M</mml:mi><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msub></mml:mtd><mml:mtd><mml:mtext>&#x00A0;</mml:mtext><mml:mo>&#x2248;</mml:mo><mml:munder><mml:mo movablelimits="false">&#x2211;</mml:mo><mml:mrow><mml:mi>l</mml:mi><mml:mo>&#x003C;</mml:mo><mml:mi>m</mml:mi></mml:mrow></mml:munder><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>m</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03BC;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>2</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:munderover><mml:mo movablelimits="false">&#x2211;</mml:mo><mml:mrow><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:munderover><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03BC;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd /><mml:mtd><mml:mi></mml:mi><mml:mo>+</mml:mo><mml:mfrac><mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mn>2</mml:mn></mml:mfrac><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03BC;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mn>2</mml:mn><mml:mo>,</mml:mo><mml:mn>3</mml:mn><mml:mo>,</mml:mo><mml:mn>4</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<disp-formula id="eqn-20"><label>(20)</label><mml:math id="mml-eqn-20" display="block"><mml:mrow><mml:mo>{</mml:mo><mml:mtable columnalign="left" rowspacing="4pt" columnspacing="1em"><mml:mtr><mml:mtd><mml:msub><mml:mi>&#x03BC;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>M</mml:mi><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:msub><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msqrt><mml:msub><mml:mi>M</mml:mi><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:msqrt></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:msub><mml:mi>&#x03B1;</mml:mi><mml:mrow><mml:mn>3</mml:mn><mml:mi>G</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>M</mml:mi><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:msup><mml:mrow><mml:msub><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msup></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:msub><mml:mi>&#x03B1;</mml:mi><mml:mrow><mml:mn>4</mml:mn><mml:mi>G</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>M</mml:mi><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:msup><mml:mrow><mml:msub><mml:mi>&#x03C3;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msup></mml:mtd></mml:mtr></mml:mtable><mml:mo fence="true" stretchy="true" symmetric="true"></mml:mo></mml:mrow></mml:math></disp-formula>where <italic>M</italic><sub><italic>z</italic></sub> denotes the <italic>z</italic>-th central moment; <italic>&#x03B1;</italic><sub>3</sub> and <italic>&#x03B1;</italic><sub>4</sub> respectively stand for the skewness coefficient and the kurtosis coefficien; <italic>g</italic>(<italic>u</italic><sub><italic>c</italic></sub>) denotes the response value under the condition that all random parameters take values corresponding to the reference point; <italic>g</italic>(<italic>X</italic><sub><italic>k</italic></sub>, <italic>u</italic><sub><italic>c</italic></sub>) denotes response value when <italic>k</italic>-th parameter is considered as random variable while the others are set to their reference values; <italic>g</italic>(<italic>X</italic><sub><italic>l</italic></sub>, <italic>X</italic><sub><italic>m</italic></sub>, <italic>u</italic><sub><italic>c</italic></sub>) denotes response value when <italic>l</italic>-th and <italic>m</italic>-th parameters are considered as random variable while the others are corresponding to the reference point. <inline-formula id="ieqn-8"><mml:math id="mml-ieqn-8"><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03BC;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula id="ieqn-9"><mml:math id="mml-ieqn-9"><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>m</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03BC;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> can be calculated based on Gaussian Hermite integration, and they can be formulated in the following functions:
<disp-formula id="eqn-21"><label>(21)</label><mml:math id="mml-eqn-21" display="block"><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03BC;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>h</mml:mi></mml:mrow></mml:munderover><mml:mfrac><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi>G</mml:mi><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:msqrt><mml:mi>&#x03C0;</mml:mi></mml:msqrt></mml:mfrac><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03BC;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup></mml:math></disp-formula>
<disp-formula id="eqn-22"><label>(22)</label><mml:math id="mml-eqn-22" display="block"><mml:mi>E</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>m</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03BC;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>h</mml:mi></mml:mrow></mml:munderover><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>h</mml:mi></mml:mrow></mml:munderover><mml:mfrac><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi>G</mml:mi><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi>G</mml:mi><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mi>&#x03C0;</mml:mi></mml:mfrac><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi>l</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi>m</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03BC;</mml:mi><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msup></mml:math></disp-formula></p>
</sec>
<sec id="s4_2">
<label>4.2</label>
<title>Calculation of Reliability Index</title>
<p>The failure probability <italic>P</italic><sub><italic>f</italic></sub> can be expressed as a function of the fourth order moment reliability index <italic>&#x03B2;</italic><sub>4M</sub> function based on the center moment of the first four moments of the limit state function, and it can be written as [<xref ref-type="bibr" rid="ref-39">39</xref>]:
<disp-formula id="eqn-23"><label>(23)</label><mml:math id="mml-eqn-23" display="block"><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mrow><mml:mtext>f</mml:mtext></mml:mrow></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mrow><mml:mi mathvariant="normal">&#x03A6;</mml:mi></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03B2;</mml:mi><mml:mrow><mml:mn>4</mml:mn><mml:mrow><mml:mtext>M</mml:mtext></mml:mrow></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>where &#x03A6;(&#x00B7;) represents the cumulative distribution function for the standard normal distribution, and the detail calculation formula of <italic>&#x03B2;</italic><sub>4M</sub> can be found in Zhao and Lu [<xref ref-type="bibr" rid="ref-39">39</xref>], and this method can also be termed high order moment method (HOMM).</p>
</sec>
<sec id="s4_3">
<label>4.3</label>
<title>LimitStateFunction</title>
<p>Before analyzing the reliability of the structure, a limit state function is neccessary to be established, and its fundamental expression is presented below:
<disp-formula id="eqn-24"><label>(24)</label><mml:math id="mml-eqn-24" display="block"><mml:mi>Z</mml:mi><mml:mo>=</mml:mo><mml:mi>&#x03BC;</mml:mi><mml:mi>R</mml:mi><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mrow><mml:mi>G</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>G</mml:mi><mml:mi>k</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mrow><mml:mi>Q</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>Q</mml:mi><mml:mi>k</mml:mi></mml:mrow></mml:msub></mml:math></disp-formula>where <italic>R</italic> is resistance, and it can satisfy <xref ref-type="disp-formula" rid="eqn-1">Eqs. (1)</xref>&#x2013;<xref ref-type="disp-formula" rid="eqn-10">(10)</xref>; <italic>&#x03B3;</italic><sub><italic>G</italic></sub> and <italic>&#x03B3;</italic><sub><italic>Q</italic></sub> represents the partial factor of dead load and live load, respectively; <italic>S</italic><sub><italic>Gk</italic></sub> and <italic>S</italic><sub><italic>Qk</italic></sub> respectively represents the standard values of dead load and live load, and they can be given as follows:
<disp-formula id="eqn-25"><label>(25)</label><mml:math id="mml-eqn-25" display="block"><mml:mrow><mml:mo>{</mml:mo><mml:mtable columnalign="left" rowspacing="4pt" columnspacing="1em"><mml:mtr><mml:mtd><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>G</mml:mi><mml:mi>k</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>d</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mrow><mml:mi>G</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mi>k</mml:mi><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mrow><mml:mi>Q</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>Q</mml:mi><mml:mi>k</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mi>k</mml:mi><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>d</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mrow><mml:mi>G</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mi>k</mml:mi><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mrow><mml:mi>Q</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr></mml:mtable><mml:mo fence="true" stretchy="true" symmetric="true"></mml:mo></mml:mrow></mml:math></disp-formula>where <italic>S</italic><sub><italic>d</italic></sub> is the standard value of load, and <italic>k</italic> denotes the ratio of live load to dead load.</p>
</sec>
</sec>
<sec id="s5">
<label>5</label>
<title>Analysis of Reliability and Partial Factor</title>
<p>According to <xref ref-type="disp-formula" rid="eqn-1">Eqs. (1)</xref> to <xref ref-type="disp-formula" rid="eqn-7">(7)</xref>, the prediction value of the bearing capacity of eccentrically compressed RC columns with HSSBs can be determined, and the moment values of limit state function can be calculated by <xref ref-type="disp-formula" rid="eqn-14">Eqs. (14)</xref> to <xref ref-type="disp-formula" rid="eqn-22">(22)</xref> and <xref ref-type="disp-formula" rid="eqn-24">Eqs. (24)</xref> and <xref ref-type="disp-formula" rid="eqn-25">(25)</xref>. Then the reliability index and failure probability can be obtained by <xref ref-type="disp-formula" rid="eqn-23">Eq. (23)</xref>.</p>
<sec id="s5_1">
<label>5.1</label>
<title>Reliability Analysis</title>
<p>The precision of the methods used for reliability calculations plays a significant role in the dependability of reliability analysis. Considering six cross-sections as examples, presented in <xref ref-type="table" rid="table-4">Table 4</xref>, the reliability of RC cross-sections under eccentric loads was calculated using the HOMM, and these results are compared with those obtained from the Monte Carlo simulation (MCS) method. While MCS is a straightforward and precise method for reliability calculations, it necessitates a significant sample size for accurate outcomes. Moreover, this section will explore the material partial factors for HSSB, the value of <italic>k</italic>, and how varying load conditions (house load or office) affect the reliability indexes.</p>
<table-wrap id="table-4">
<label>Table 4</label>
<caption>
<title>Case of reliability analysis</title>
</caption>
<table>
<colgroup>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
</colgroup>
<thead>
<tr align="center">
<th align="center">No.</th>
<th align="center">Specimen</th>
<th align="center">Width (mm)</th>
<th align="center">Height (mm)</th>
<th align="center"><italic>a</italic><sub><bold><italic>s</italic></bold></sub> (mm)</th>
<th align="center"><italic>n</italic></th>
<th align="center"><italic>d</italic> (mm)</th>
<th align="center"><italic>f</italic><sub><bold><italic>c</italic></bold></sub> (MPa)</th>
<th align="center">e<sub><bold>0</bold></sub> (mm)</th>
</tr>
</thead>
<tbody>
<tr align="center">
<td>1</td>
<td>EC1-1</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>16</td>
<td>32.67</td>
<td>270</td>
</tr>
<tr align="center">
<td>2</td>
<td>EC1-2</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>22</td>
<td>32.67</td>
<td>270</td>
</tr>
<tr align="center">
<td>3</td>
<td>EC1-3</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>25</td>
<td>32.67</td>
<td>270</td>
</tr>
<tr align="center">
<td>4</td>
<td>EC3-1</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>16</td>
<td>32.67</td>
<td>220</td>
</tr>
<tr align="center">
<td>5</td>
<td>EC3-2</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>16</td>
<td>32.67</td>
<td>320</td>
</tr>
<tr align="center">
<td>6</td>
<td>EC4-1</td>
<td>300</td>
<td>500</td>
<td>25</td>
<td>2</td>
<td>16</td>
<td>32.67</td>
<td>270</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The reliability indices computed by HOMM and MCS are displayed in <xref ref-type="fig" rid="fig-4">Fig. 4</xref>. It is evident that the reliability indices from HOMM are in agreement with those from MCS, affirming the method&#x2019;s accuracy. Furthermore, it is observed that for different design sections, the reliability index exhibits a linear increase with the rise in material partial factors, and this is because the increase in partial factor leads to a greater actual bearing capacity, which is consistent with the results in the literatures [<xref ref-type="bibr" rid="ref-41">41</xref>,<xref ref-type="bibr" rid="ref-42">42</xref>].</p>
<fig id="fig-4">
<label>Figure 4</label>
<caption>
<title>Calculation result from HOMM and MCS</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_63813-fig-4.tif"/>
</fig>
<p><xref ref-type="fig" rid="fig-5">Fig. 5</xref> illustrates the reliability indices for varying <italic>k</italic> values and material partial factors, considering both house load and office loads. In different scenarios, the reliability index similarly shows a linear upward trend with the increase in material partial factors. Additionally, the reliability index increases with higher <italic>k</italic> values, indicating that the distribution ratio of lateral to live load in the design significantly influences reliability.</p>
<fig id="fig-5">
<label>Figure 5</label>
<caption>
<title>Reliability indexes under various <italic>k</italic> values</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_63813-fig-5.tif"/>
</fig>
</sec>
<sec id="s5_2">
<label>5.2</label>
<title>Calibration of Material Partial Factor</title>
<p>Structural safety and economy are often seen as conflicting factors in design. A high reliability index may lead to an excessive structural surplus, indicating a compromise in economic efficiency. Conversely, a low reliability index may risk structural safety. Design guidelines often differentiate target reliability indices based on the importance level of the results, as specified in GB5068-2018 [<xref ref-type="bibr" rid="ref-38">38</xref>], which is detailed in <xref ref-type="table" rid="table-5">Table 5</xref>.</p>
<table-wrap id="table-5">
<label>Table 5</label>
<caption>
<title>Target reliability index</title>
</caption>
<table>
<colgroup>
<col/>
<col/>
<col/>
<col/>
</colgroup>
<thead>
<tr align="center">
<th></th>
<th>Level I</th>
<th>Level II</th>
<th>Level III</th>
</tr>
</thead>
<tbody>
<tr align="center">
<td>Brittle comment</td>
<td>4.2</td>
<td>3.7</td>
<td>3.2</td>
</tr>
<tr align="center">
<td>Ductile comment</td>
<td>3.7</td>
<td>3.2</td>
<td>2.7</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>To determine the optimal material partial factors, multiple eccentrically loaded RC rectangular sections were designed, with parameters listed in <xref ref-type="table" rid="table-6">Table 6</xref>. These parameters encompass five section widths, seven section heights, four concrete strength classes, ten eccentricities, and eight reinforcement ratios, yielding a total of 5 &#x00D7; 7 &#x00D7; 4 &#x00D7; 10 &#x00D7; 8 &#x003D; 11,200 cases. For each set of parameters under identical conditions, a reliability index is calculated, resulting in 11,200 reliability indices. To calibrate the material partial factors, the following index can be utilized [<xref ref-type="bibr" rid="ref-33">33</xref>]:
<disp-formula id="eqn-26"><label>(26)</label><mml:math id="mml-eqn-26" display="block"><mml:mi>H</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:mi>n</mml:mi></mml:mfrac><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:munderover><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>&#x03B2;</mml:mi><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>&#x03B2;</mml:mi><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>where <italic>&#x03B2;</italic><sub><italic>i</italic></sub> and <italic>&#x03B2;</italic><sub><italic>T</italic></sub> represents the calculated reliability index and the target reliability index, respectively, and the value of <italic>&#x03B2;</italic><sub><italic>T</italic></sub> can be found in <xref ref-type="table" rid="table-5">Table 5</xref>; <italic>n</italic> represents the number of calculated cases. As the calibration value decreases, the reliability index associated with the material partial factor progressively converges toward the target reliability index, and its value is more reasonable.</p>
<table-wrap id="table-6">
<label>Table 6</label>
<caption>
<title>Design parameters</title>
</caption>
<table>
<colgroup>
<col/>
<col/>
<col/>
<col/>
</colgroup>
<thead>
<tr align="center">
<th>Parameter</th>
<th>Unit</th>
<th>Range</th>
<th>Interval</th>
</tr>
</thead>
<tbody>
<tr align="center">
<td>Width <italic>b</italic></td>
<td>mm</td>
<td>300 to 500</td>
<td>50</td>
</tr>
<tr align="center">
<td>Height <italic>h</italic></td>
<td>mm</td>
<td>300 to 600</td>
<td>50</td>
</tr>
<tr align="center">
<td>Concrete strength <italic>fc</italic></td>
<td>MPa</td>
<td>16.7, 20.1, 23.4, 26.8</td>
<td>&#x2013;</td>
</tr>
<tr align="center">
<td>Type of reinforcement</td>
<td>&#x2013;</td>
<td>&#x2013;</td>
<td>&#x2013;</td>
</tr>
<tr align="center">
<td>Eccentricity <italic>e</italic><sub>0</sub></td>
<td>mm</td>
<td>50 to 500</td>
<td>50</td>
</tr>
<tr align="center">
<td>Reinforcement ratio <italic>&#x03C1;</italic><sub><italic>s</italic></sub></td>
<td>%</td>
<td>0.5 to 2.0</td>
<td>0.2</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>Separate assessments for house and office loading conditions were conducted to ascertain the optimal material partial factor, with these factors ranging from 1.0 to 1.35 at increments of 0.05. The considered <italic>k</italic> values were 0.5, 1.0, 1.5, 2.0, and 2.5. The calibration results are presented in <xref ref-type="fig" rid="fig-6">Figs. 6</xref> and <xref ref-type="fig" rid="fig-7">7</xref>.</p>
<fig id="fig-6">
<label>Figure 6</label>
<caption>
<title>Calibration for partial factor of office condition</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_63813-fig-6.tif"/>
</fig><fig id="fig-7">
<label>Figure 7</label>
<caption>
<title>Calibration for partial factor of house condition</title>
</caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_63813-fig-7.tif"/>
</fig>
<p>According to <xref ref-type="fig" rid="fig-6">Fig. 6</xref>, the value of <italic>k</italic> significantly influences the calibration of reliability indices. At <italic>k</italic> &#x003D; 0.5, the calibration values for target reliabilities of 3.2 and 3.7 decrease with increasing material partial factors, while for a target reliability of 2.7, the calibration values initially decrease and then increase, with the lowest value occurring at approximately 1.15. At <italic>k</italic> &#x003D; 1.0, the calibration values for target reliabilities of 3.2 and 3.7 decrease with increasing material partial factors, whereas for a target reliability of 2.7, they increase with increasing material partial factors. At <italic>k</italic> &#x003D; 1.5, the calibration value for a target reliability of 3.2 initially declines and then rises with a rise in the material partial factor, reaching its minimum at around 1.18. For a target reliability of 2.7, the calibration value increases, while for a target reliability of 3.7, it decreases with increasing material partial factor. At <italic>k</italic> &#x003D; 2.0 and 2.5, the calibration values of the reliability indices are similar to those observed at <italic>k</italic> &#x003D; 1.5.</p>

<p><xref ref-type="fig" rid="fig-7">Fig. 7</xref> shows the situation for house loading. Similarly, the value of <italic>k</italic> has a significant impact on the calibration of reliability indices. At <italic>k</italic> &#x003D; 0.5, the calibration values of different target reliabilities increase with the material partial factor. At <italic>k</italic> &#x003D; 1.0, the calibration values for target reliabilities of 3.2 and 3.7 decrease with increasing material partial factors, while those for a target reliability of 2.7 initially decrease and then increase, with the lowest value occurring at approximately 1.15. At <italic>k</italic> &#x003D; 1.5, the calibration value for a target reliability of 3.2 shows a similar pattern of initial decrease and subsequent increase, with the lowest value at around 1.18. For a target reliability of 2.7, the calibration value increases, while for a target reliability of 3.7, it decreases with increasing material partial factors. At <italic>k</italic> &#x003D; 2.0 and 2.5, the calibration values follow the pattern observed at <italic>k</italic> &#x003D; 1.5.</p>
<p>Based on the calculations, it is recommended to set the material partial factor at 1.15 for a target reliability index of 3.2. For cases with reliability indices of 2.7 and 3.7, it is advisable to refer to the specifications and apply load effect amplification factors of 0.9 and 1.1, respectively. According to the material partial factor, the strength design value of corresponding high-strength reinforcement can be obtained as shown in <xref ref-type="table" rid="table-7">Table 7</xref>.</p>
<table-wrap id="table-7">
<label>Table 7</label>
<caption>
<title>Design strength of steel rebar</title>
</caption>
<table>
<colgroup>
<col/>
<col/>
<col/>
<col/>
</colgroup>
<thead>
<tr align="center">
<th>Grade</th>
<th>Standard strength (MPa)</th>
<th>Design strength (MPa)</th>
<th>Note</th>
</tr>
</thead>
<tbody>
<tr align="center">
<td>HRB335</td>
<td>335</td>
<td>300</td>
<td>GB50010-2010</td>
</tr>
<tr align="center">
<td>HRB400</td>
<td>400</td>
<td>360</td>
<td>GB50010-2010</td>
</tr>
<tr align="center">
<td>HRB500</td>
<td>500</td>
<td>435</td>
<td>GB50010-2010 and proposed</td>
</tr>
<tr align="center">
<td>HRB600</td>
<td>600</td>
<td>520</td>
<td>Proposed</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</sec>
<sec id="s6">
<label>6</label>
<title>Discussions</title>
<p>(1) HOMM has high accuracy and computational efficiency in calculating reliability indexes, and it is easy to use, and it can be widely applied in reliability analysis of other types of concrete structures.</p>
<p>(2) The material partial factor of HRB335 and HRB400 in the code GB50010-2010 is about 1.11, and their strength design values are 300 and 360 MPa, respectively; Regarding axial compressive strength, the compressive strength design value for HRB500 and HRBF500 reinforcement is 400 MPa, with a partial factor of 1.25. Conversely, other cases have a design strength of 435 MPa and a partial factor of 1.15. These results are in line with those presented in this paper, though the 1.25 partial factor is viewed as quite conservative. For reinforcement with standard tensile strength of 600 MPa, the recommended strength design value is 520 MPa, as shown in <xref ref-type="table" rid="table-7">Table 7</xref>.</p>

<p>(3) It is important to mention that the proposed partial factors for HSSB were derived from the bearing capacity of eccentrically compressed RC columns. Additional investigations are required to verify whether member under other states are also applicable.</p>
<p>(4) The coefficient of variation of high-performance steel bars is inconsistent with that of ordinary steel bars, resulting in inconsistent partial factor. This research provides some reference for the calibration strategy of partial factor for other high-performance materials.</p>
</sec>
<sec id="s7">
<label>7</label>
<title>Conclusions</title>
<p>To enhance the application of HSSB concrete, this study addressed the uncertainty in the approach used to determine the load-bearing capacity of RC columns with HSSB under eccentric compression. The uncertainties of other parameters were also collected. A limit state function was formulated, taking into account various ratios of dead load to live load. The HOMM was employed to evaluate the reliability of the bearing capacity of reinforced concrete columns under eccentric compression, and its accuracy was validated. Extensive case studies were conducted to determine the calibration values for material partial factors under different dead-to-live load ratios and usage conditions, leading to the identification of optimal factors. The main conclusions are as follows:</p>
<p>(1) For RC columns with HSSB under eccentric compression, the calculation method&#x2019;s uncertainty is represented by a normal distribution, with parameters including a mean of 1.18, a standard deviation of 0.19, and a coefficient of variation of 0.16.</p>
<p>(2) The HOMM has proven to be both efficient and accurate in calculating the reliability of the bearing capacity for eccentrically compressed RC columns with HSSB when compared to MCS.</p>
<p>(3) The reliability of the bearing capacity of reinforced concrete columns is greatly affected by the ratio of dead load to live load. As this ratio rises, the reliability index typically becomes higher. Additionally, an increase in the material partial factor leads to a linear increase in the reliability index.</p>
<p>(4) Based on the computational results, it is advised that the material partial factor be set according to a target reliability index of 3.2, which is recommended to be 1.15. For cases with reliability indices of 2.7 and 3.7, it is appropriate to consult the specifications and apply load effect amplification factors of 0.9 and 1.1, respectively.</p>
</sec>
</body>
<back>
<ack>
<p>Not applicable.</p>
</ack>
<sec>
<title>Funding Statement</title>
<p>The work described in this paper is supported by grants from the Natural Science Foundation of Fujian Province (Grant No. 2022J05184).</p>
</sec>
<sec>
<title>Author Contributions</title>
<p>Baojun Qin: Performed the review, wrote the manuscript. Hong Jiang: Detailed check of the text and references, editorial contribution. Wei Zhang: Detailed check of the text and references, editorial contribution. Xiang Liu: Planned and organized the paper, performed the review, wrote the manuscript, performed editorial tasks, organized the tasks, served as a corresponding author. All authors reviewed the results and approved the final version of the manuscript.</p>
</sec>
<sec sec-type="data-availability">
<title>Availability of Data and Materials</title>
<p>Available upon request.</p>
</sec>
<sec>
<title>Ethics Approval</title>
<p>Not applicable.</p>
</sec>
<sec sec-type="COI-statement">
<title>Conflicts of Interest</title>
<p>The authors declare no conflicts of interest to report regarding the present study.</p>
</sec>
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