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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mar. Sci.</journal-id>
<journal-title>Frontiers in Marine Science</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mar. Sci.</abbrev-journal-title>
<issn pub-type="epub">2296-7745</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fmars.2023.1300005</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Marine Science</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Cyclic resistance evaluation of marine clay based on CPTu data: a case study of Shaba Wind Farm</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Wu</surname>
<given-names>Qi</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/2063144"/>
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<role content-type="https://credit.niso.org/contributor-roles/resources/"/>
<role content-type="https://credit.niso.org/contributor-roles/validation/"/>
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<role content-type="https://credit.niso.org/contributor-roles/writing-original-draft/"/>
<role content-type="https://credit.niso.org/contributor-roles/writing-review-editing/"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Zhu</surname>
<given-names>En-ci</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/2523292"/>
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<role content-type="https://credit.niso.org/contributor-roles/writing-review-editing/"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Xiao</surname>
<given-names>Xing</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="author-notes" rid="fn001">
<sup>*</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/2240880"/>
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</contrib>
<contrib contrib-type="author">
<name>
<surname>Li</surname>
<given-names>Yuan-xi</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<role content-type="https://credit.niso.org/contributor-roles/conceptualization/"/>
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</contrib>
<contrib contrib-type="author">
<name>
<surname>Chen</surname>
<given-names>Guo-xing</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<role content-type="https://credit.niso.org/contributor-roles/conceptualization/"/>
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<aff id="aff1">
<sup>1</sup>
<institution>Institute of Geotechnical Engineering, Nanjing Tech University</institution>, <addr-line>Nanjing, Jiangsu</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>China Energy Engineering Group Guangdong Electric Power Design Institute Co., Ltd.</institution>, <addr-line>Guangzhou, Guangdong</addr-line>, <country>China</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>Edited by: Xingsen Guo, University College London, United Kingdom</p>
</fn>
<fn fn-type="edited-by">
<p>Reviewed by: Xiaotong Yang, Tsinghua University, China</p>
<p>Xianwei Zhang, Chinese Academy of Sciences (CAS), China</p>
<p>Zhongkun Ouyang, Tsinghua University, China</p>
<p>Xiaotong Yang, Tsinghua University, China in collaboration with reviewer ZO</p>
</fn>
<fn fn-type="corresp" id="fn001">
<p>*Correspondence: Xing Xiao, <email xlink:href="mailto:xx_0524@126.com">xx_0524@126.com</email>
</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>04</day>
<month>01</month>
<year>2024</year>
</pub-date>
<pub-date pub-type="collection">
<year>2023</year>
</pub-date>
<volume>10</volume>
<elocation-id>1300005</elocation-id>
<history>
<date date-type="received">
<day>23</day>
<month>09</month>
<year>2023</year>
</date>
<date date-type="accepted">
<day>05</day>
<month>12</month>
<year>2023</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2024 Wu, Zhu, Xiao, Li and Chen</copyright-statement>
<copyright-year>2024</copyright-year>
<copyright-holder>Wu, Zhu, Xiao, Li and Chen</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>The offshore wind farm industry has recently experienced significant global growth. This study presents a thorough site investigation and analysis of the cyclic resistance of marine clay for offshore foundation design, using the Shaba wind farm in southern China as a case study. <italic>In-situ</italic> cone penetrometer (CPTu) tests and borehole sampling are conducted to explore the geotechnical characteristics of the soils. However, the soil conditions are characterized by multiple layers and complex sedimentary components. The classification and mechanical properties, such as water content and cyclic resistances, are compared through CPTu interpretation and laboratory tests. The findings indicated that a single physical indicator cannot determine cyclic resistance. In addition, the well-established method in existing literature proved unsuitable for marine clay. Consequently, multiple regression analysis shows that a linear relationship exist between cyclic resistance and depth-corrected CPTu index [<italic>EXP</italic>(<italic>q</italic>
<sub>E</sub>/<italic>f</italic>
<sub>s</sub>)<sup>0.3</sup>/<italic>H</italic>], hence a new evaluation method is developed to predict the cyclic resistance of marine clay based on CPTu data. This research aims to provide more reliable guidance for geotechnical investigations, supporting the rapid expansion of offshore wind farms.</p>
</abstract>
<kwd-group>
<kwd>site investigation</kwd>
<kwd>CPTU</kwd>
<kwd>cyclic resistance</kwd>
<kwd>marine clay</kwd>
<kwd>offshore wind farms</kwd>
</kwd-group>
<counts>
<fig-count count="10"/>
<table-count count="6"/>
<equation-count count="4"/>
<ref-count count="37"/>
<page-count count="12"/>
<word-count count="4741"/>
</counts>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-in-acceptance</meta-name>
<meta-value>Ocean Observation</meta-value>
</custom-meta>
</custom-meta-wrap>
</article-meta>
</front>
<body>
<sec id="s1" sec-type="intro">
<label>1</label>
<title>Introduction</title>
<p>Wind energy, a sustainable and environmentally friendly energy source, offers an innovative path for global efforts in addressing energy shortages. The installed capacity of offshore wind turbines has shown consistent annual growth. These turbines are typically anchored to the seabed, often involving marine clay layers. Foundation costs, comprising approximately 25%&#x2013;35% of total costs (<xref ref-type="bibr" rid="B8">Bhattacharya, 2014</xref>), necessitate various marine clay parameters for the geotechnical design of diverse foundation solutions. Under complex marine environmental loads, such as wind, waves, storms, and earthquakes, marine clay demonstrates notable stiffness degradation characteristics (<xref ref-type="bibr" rid="B36">Yang et&#xa0;al., 2018</xref>; <xref ref-type="bibr" rid="B28">Pan et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B35">Xiao et&#xa0;al., 2023</xref>) and can even lose strength entirely. Thus, understanding the cyclic resistance of marine clay is crucial for foundation design. However, its precise determination and rational design pose significant challenges in engineering construction (<xref ref-type="bibr" rid="B23">Lunne et&#xa0;al., 2006</xref>; <xref ref-type="bibr" rid="B7">Berre et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B15">Gao et&#xa0;al., 2024</xref>).</p>
<p>The predominant method to determine marine clay&#x2019;s cyclic resistance involves laboratory cyclic tests, including cyclic triaxial tests, cyclic torsional shear tests, and cyclic direct simple shear tests. These tests demand high-quality soil samples and skilled testers. Nevertheless, soil sample disturbance during drilling and transport can compromise the accuracy of these tests in representing marine clay&#x2019;s <italic>in-situ</italic> cyclic resistance. In addition, the requirement for a large volume of soil samples substantially increases the cost. Consequently, the engineering community urgently seeks effective methods to ascertain marine clay&#x2019;s cyclic resistance with fewer tests.</p>
<p>Comprehensive <italic>in-situ</italic> and laboratory tests are indispensable in acquiring site geotechnical properties and soil parameters. Cone penetrometer (CPTu) tests are preferred for <italic>in-situ</italic> testing due to their high accuracy, convenience, and speed (<xref ref-type="bibr" rid="B10">Cai et&#xa0;al., 2012</xref>; <xref ref-type="bibr" rid="B9">Cai et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B13">Duan et&#xa0;al., 2017</xref>; <xref ref-type="bibr" rid="B26">Meng and Pei, 2023</xref>). CPTu data comprehensively represent soil strength and deformation capacity under static and dynamic loading. Over the past decades, CPTu-based undrained shear strength evaluation methods for soils have been extensively developed (<xref ref-type="bibr" rid="B31">Sandven, 1990</xref>; <xref ref-type="bibr" rid="B14">Eslami, 1997</xref>). Subsequently, researchers began developing cyclic strength evaluation methods based on <italic>in-situ</italic> and laboratory tests (<xref ref-type="bibr" rid="B27">Olsen, 1994</xref>; <xref ref-type="bibr" rid="B30">Robertson and Wride, 1998</xref>; <xref ref-type="bibr" rid="B29">Robertson, 2009</xref>). <xref ref-type="bibr" rid="B20">Juang et&#xa0;al. (2008)</xref> developed a deterministic CPTu-based cyclic resistance evaluation method applicable to various soil types. <xref ref-type="bibr" rid="B19">Juang et&#xa0;al. (2012)</xref> and <xref ref-type="bibr" rid="B21">Ku and Juang (2012)</xref> refined this model. Notably, these models were formulated using CPTu data for terrestrial soils. However, marine clays, influenced by factors like high salt content, low-temperature seawater environments, unique cementitious materials, and complex hydrodynamics, develop flocculated structures distinct from terrestrial soils. Thus, terrestrial clay cyclic resistance models are not directly transferable to marine clays. Limited research focuses on evaluating marine clay cyclic resistance. <xref ref-type="bibr" rid="B16">He et&#xa0;al. (2021)</xref> and <xref ref-type="bibr" rid="B33">Wang et&#xa0;al. (2022)</xref> explored the cyclic behavior of marine soils using CPTu tests, but they did not develop predictive models. Therefore, creating and refining a cyclic resistance evaluation method for marine clay based on <italic>in-situ</italic> and laboratory tests is essential.</p>
<p>This study conducts a case study involving CPTu tests at the Shaba offshore wind farm in southern China to establish a cost-effective method to evaluate marine clay cyclic resistance. Soil stratigraphy is delineated, highlighting the soil&#x2019;s multilayered and complex sedimentation. In addition, consolidated undrained cyclic triaxial tests on marine clay are conducted to assess cyclic resistance, a vital parameter for foundation design. The well-established CPTu-based cyclic resistance evaluation methods in existing literature are not fully applicable to marine clays. Ultimately, this research develops a CPTu-based cyclic resistance evaluation method for marine clay at the Shaba offshore wind farm. The study&#x2019;s findings will offer assistance and guidance for constructing offshore wind farms in China.</p>
</sec>
<sec id="s2">
<label>2</label>
<title>Site description</title>
<p>The Yangjiang Shaba Offshore Wind Farm is situated in the southern sea area of Shaba Town, Yangxi County, Yangjiang City, Guangdong Province, as illustrated in <xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1</bold>
</xref>. This wind farm lies approximately 20 kilometers offshore. The area&#x2019;s sea is expansive, lacks islands, and features relatively flat terrain. Water depths vary from 23 to 27 meters, with an average tidal range of around 2.73 meters. Summer months bring significant typhoon impacts, leading to maximum wave heights near 8 meters.</p>
<fig id="f1" position="float">
<label>Figure&#xa0;1</label>
<caption>
<p>Site location (Base map data <sup>&#xa9;</sup> 2023 Google).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1300005-g001.tif"/>
</fig>
<p>The site is positioned at the Rudong River&#x2019;s mouth, where the sedimentary environment is notably complex, shaped by the combined influences of river flow and ocean waves. Sediments primarily comprise marine, alluvial marine, and residual deposits, characterized by a swift sedimentation rate. Soil stratification will be elaborated upon based on CPTu and borehole sampling results. In addition, the sea area at this location is spacious, devoid of surrounding islands. The seafloor topography is predominantly gentle, showing a trend of higher elevation in the northwest and lower in the southeast. No potential submarine geological hazards, such as underwater landslides, have been identified.</p>
</sec>
<sec id="s3">
<label>3</label>
<title>CPTu tests and soil characteristic</title>
<sec id="s3_1">
<label>3.1</label>
<title>CPTu test results</title>
<p>This project entailed offshore field investigations, encompassing 4 CPTu tests (CPTu1, CPTu2, CPTu3, and CPTu4) and four borehole samplings (Y1, Y2, Y3, and Y4), with each borehole sampling site situated about 1 meter from its corresponding CPTu test hole. The CPTu tests utilized the ROSON seabed digital CPT penetration equipment by Van Den Berg, Netherlands. This device operates at a penetration speed of 20 mm/s, boasts a maximum thrust of 50 kN, and can penetrate up to 40 meters deep. It can perform continuous CPTu tests in seabeds with water depths reaching 1500 meters. Borehole sampling employed hydrostatic pressure-driven methodology. Standard Shelby tube samplers were used for soft clay, while thick-walled tube samplers were applied for silty mud and sandy soil. The depths of CPTu1, CPTu2, Y1, and Y2 are 14 meters; CPTu3 and Y3 are 24 meters deep; and CPTu4 and Y4 are 28 meters.</p>
<p>
<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2</bold>
</xref> displays the CPTu test results for the four boreholes. Notable fluctuations in <italic>q</italic>
<sub>c</sub> (cone resistance), <italic>f</italic>
<sub>s</sub> (sleeve friction), and <italic>u</italic>
<sub>2</sub> (pore water pressure) are evident with depth in each borehole, signifying multiple soil layers. Utilizing the CPTu data and laboratory test outcomes, the stratigraphic details of soil layers were determined following the ASTM D2487 (<xref ref-type="bibr" rid="B3">ASTM, 2017</xref>) standard. A simplified diagram representing this information accompanies the CPTu test results. <xref ref-type="bibr" rid="B34">Wu et&#xa0;al. (2023)</xref> comprehensively described soil stratification methods. The geological strata mainly consist of marine-terrestrial transitional sedimentary layers. The upper part includes Holocene marine deposits, encompassing sludge and medium sand mixed sludge. The lower part comprises the Holocene sea-land transitional sedimentary layer and the late Pleistocene sea-land alternating sedimentary layer, containing clay, silt, fine sand, medium sand, and coarse sand. This study focuses on clay; hence, emphasis is placed on CPTu data pertinent to clay layers. Compared to cohesionless soil and rock layers, the <italic>q</italic>
<sub>c</sub> and <italic>f</italic>
<sub>s</sub> values for clay layers are relatively low and show little depth dependence, while the <italic>u</italic>
<sub>2</sub> values are higher and typically increase with depth. In addition, an inverse relationship exists between <italic>u</italic>
<sub>2</sub> and <italic>q</italic>
<sub>c</sub>, indicating that higher <italic>u</italic>
<sub>2</sub> values correspond to lower <italic>q</italic>
<sub>c</sub> values. This aligns with the principles of effective stress.</p>
<fig id="f2" position="float">
<label>Figure&#xa0;2</label>
<caption>
<p>CPTu results and soil layer classifications. (<bold>A&#x2013;D</bold> are four different boreholes).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1300005-g002.tif"/>
</fig>
</sec>
<sec id="s3_2">
<label>3.2</label>
<title>Index properties of marine clay</title>
<p>The natural water content (<italic>w</italic>
<sub>0</sub>), density (<italic>&#x3c1;</italic>), plasticity index (<italic>I</italic>
<sub>p</sub>), and initial void ratio (<italic>e</italic>
<sub>0</sub>) of the clay samples (D1~D12, as shown in <xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2</bold>
</xref>) in the stratum were determined in accordance with ASTM D2216 (<xref ref-type="bibr" rid="B2">ASTM, 2019</xref>), D1556/D1556M (<xref ref-type="bibr" rid="B1">ASTM, 2015</xref>), and D4318 (<xref ref-type="bibr" rid="B4">ASTM, 2017</xref>), respectively. The results are depicted in <xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref>. The properties of the clay layers in the four boreholes exhibit considerable uniformity. The natural water content remains relatively consistent within each borehole, while <italic>I</italic>
<sub>p</sub> and <italic>&#x3c1;</italic> gradually increment with depth. Concurrently, <italic>e</italic>
<sub>0</sub> exhibits a steady decrease with increasing depth. The red points in <xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref> symbolize the samples utilized for conducting undrained cyclic triaxial tests. <xref ref-type="table" rid="T1">
<bold>Table&#xa0;1</bold>
</xref> summarizes their fundamental physical properties, whereas <xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4</bold>
</xref> depicts their positions on the plasticity chart. These clays are categorized as CH and CL based on ASTM D2487 (<xref ref-type="bibr" rid="B3">ASTM, 2017</xref>).</p>
<fig id="f3" position="float">
<label>Figure&#xa0;3</label>
<caption>
<p>Index properties of marine clay versus depth. (<bold>A&#x2013;D</bold> are four different boreholes).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1300005-g003.tif"/>
</fig>
<table-wrap id="T1" position="float">
<label>Table&#xa0;1</label>
<caption>
<p>Basic physic properties and scheme of undisturbed marine clay.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" rowspan="2" align="center">Test number</th>
<th valign="middle" colspan="9" align="center">Physical properties</th>
<th valign="middle" colspan="3" align="center">Test scheme</th>
</tr>
<tr>
<th valign="middle" align="center">
<italic>H</italic>/m</th>
<th valign="middle" align="center">
<italic>&#x3c1;</italic>
</th>
<th valign="middle" align="center">
<italic>w</italic>/%</th>
<th valign="middle" align="center">
<italic>w</italic>
<sub>L</sub>/%</th>
<th valign="middle" align="center">
<italic>I</italic>
<sub>p</sub>
</th>
<th valign="middle" align="center">
<italic>e</italic>
<sub>0</sub>
</th>
<th valign="middle" align="center">
<italic>e</italic>
<sub>c</sub>
</th>
<th valign="middle" align="center">&#x394;<italic>e</italic>/<italic>e</italic>
<sub>0</sub>
</th>
<th valign="middle" align="center">Soil code</th>
<th valign="middle" align="center">
<italic>&#x3c3;</italic>&#x2019;<sub>c0</sub>/kPa</th>
<th valign="middle" align="center">
<italic>CSR</italic>
</th>
<th valign="middle" align="center">
<italic>N</italic>
<sub>f</sub>
</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="center">D1-1</td>
<td valign="top" rowspan="3" align="center">3.2-3.6</td>
<td valign="top" rowspan="3" align="center">2.42</td>
<td valign="top" rowspan="3" align="center">49.25</td>
<td valign="top" rowspan="3" align="center">52.32</td>
<td valign="top" rowspan="3" align="center">32.3</td>
<td valign="top" rowspan="3" align="center">0.960</td>
<td valign="top" align="center">0.916</td>
<td valign="top" align="center">0.046</td>
<td valign="top" rowspan="3" align="center">CH</td>
<td valign="top" rowspan="3" align="center">50</td>
<td valign="middle" align="center">0.12</td>
<td valign="middle" align="center">341</td>
</tr>
<tr>
<td valign="middle" align="center">D1-2</td>
<td valign="top" align="center">0.911</td>
<td valign="top" align="center">0.051</td>
<td valign="middle" align="center">0.14</td>
<td valign="middle" align="center">102</td>
</tr>
<tr>
<td valign="middle" align="center">D1-3</td>
<td valign="top" align="center">0.923</td>
<td valign="top" align="center">0.039</td>
<td valign="middle" align="center">0.15</td>
<td valign="middle" align="center">40</td>
</tr>
<tr>
<td valign="middle" align="center">D2-1</td>
<td valign="top" rowspan="3" align="center">7.2-7.6</td>
<td valign="top" rowspan="3" align="center">1.91</td>
<td valign="top" rowspan="3" align="center">27.67</td>
<td valign="top" rowspan="3" align="center">42.15</td>
<td valign="top" rowspan="3" align="center">18.5</td>
<td valign="top" rowspan="3" align="center">0.707</td>
<td valign="top" align="center">0.679</td>
<td valign="top" align="center">0.039</td>
<td valign="top" rowspan="3" align="center">CL</td>
<td valign="top" rowspan="3" align="center">50</td>
<td valign="middle" align="center">0.15</td>
<td valign="middle" align="center">114</td>
</tr>
<tr>
<td valign="middle" align="center">D2-2</td>
<td valign="top" align="center">0.685</td>
<td valign="top" align="center">0.031</td>
<td valign="middle" align="center">0.16</td>
<td valign="middle" align="center">43</td>
</tr>
<tr>
<td valign="middle" align="center">D2-3</td>
<td valign="top" align="center">0.688</td>
<td valign="top" align="center">0.027</td>
<td valign="middle" align="center">0.18</td>
<td valign="middle" align="center">26</td>
</tr>
<tr>
<td valign="middle" align="center">D3-1</td>
<td valign="top" rowspan="3" align="center">7.5-7.9</td>
<td valign="top" rowspan="3" align="center">1.95</td>
<td valign="top" rowspan="3" align="center">22.10</td>
<td valign="top" rowspan="3" align="center">26.80</td>
<td valign="top" rowspan="3" align="center">11.1</td>
<td valign="top" rowspan="3" align="center">0.671</td>
<td valign="top" align="center">0.650</td>
<td valign="top" align="center">0.031</td>
<td valign="top" rowspan="3" align="center">CL</td>
<td valign="top" rowspan="3" align="center">50</td>
<td valign="middle" align="center">0.3</td>
<td valign="middle" align="center">237</td>
</tr>
<tr>
<td valign="middle" align="center">D3-2</td>
<td valign="top" align="center">0.630</td>
<td valign="top" align="center">0.061</td>
<td valign="middle" align="center">0.32</td>
<td valign="middle" align="center">21</td>
</tr>
<tr>
<td valign="middle" align="center">D3-3</td>
<td valign="top" align="center">0.638</td>
<td valign="top" align="center">0.049</td>
<td valign="middle" align="center">0.33</td>
<td valign="middle" align="center">6</td>
</tr>
<tr>
<td valign="middle" align="center">D4-1</td>
<td valign="top" rowspan="3" align="center">8.3-8.7</td>
<td valign="top" rowspan="3" align="center">2.20</td>
<td valign="top" rowspan="3" align="center">30.15</td>
<td valign="top" rowspan="3" align="center">39.80</td>
<td valign="top" rowspan="3" align="center">19.8</td>
<td valign="top" rowspan="3" align="center">0.838</td>
<td valign="top" align="center">0.813</td>
<td valign="top" align="center">0.030</td>
<td valign="top" rowspan="3" align="center">CL</td>
<td valign="top" rowspan="3" align="center">55</td>
<td valign="middle" align="center">0.35</td>
<td valign="middle" align="center">423</td>
</tr>
<tr>
<td valign="middle" align="center">D4-2</td>
<td valign="top" align="center">0.800</td>
<td valign="top" align="center">0.046</td>
<td valign="middle" align="center">0.36</td>
<td valign="middle" align="center">10</td>
</tr>
<tr>
<td valign="middle" align="center">D4-3</td>
<td valign="top" align="center">0.788</td>
<td valign="top" align="center">0.060</td>
<td valign="middle" align="center">0.38</td>
<td valign="middle" align="center">3</td>
</tr>
<tr>
<td valign="middle" align="center">D5-1</td>
<td valign="top" rowspan="3" align="center">9.7-10.1</td>
<td valign="top" rowspan="3" align="center">1.89</td>
<td valign="top" rowspan="3" align="center">36.00</td>
<td valign="top" rowspan="3" align="center">66.65</td>
<td valign="top" rowspan="3" align="center">50.73</td>
<td valign="top" rowspan="3" align="center">0.614</td>
<td valign="top" align="center">0.589</td>
<td valign="top" align="center">0.041</td>
<td valign="top" rowspan="3" align="center">CH</td>
<td valign="top" rowspan="3" align="center">65</td>
<td valign="middle" align="center">0.16</td>
<td valign="middle" align="center">585</td>
</tr>
<tr>
<td valign="middle" align="center">D5-2</td>
<td valign="top" align="center">0.578</td>
<td valign="top" align="center">0.059</td>
<td valign="middle" align="center">0.18</td>
<td valign="middle" align="center">151</td>
</tr>
<tr>
<td valign="middle" align="center">D5-3</td>
<td valign="top" align="center">0.594</td>
<td valign="top" align="center">0.033</td>
<td valign="middle" align="center">0.19</td>
<td valign="middle" align="center">82</td>
</tr>
<tr>
<td valign="middle" align="center">D6-1</td>
<td valign="top" rowspan="3" align="center">11.6-12.0</td>
<td valign="top" rowspan="3" align="center">1.95</td>
<td valign="top" rowspan="3" align="center">29.85</td>
<td valign="top" rowspan="3" align="center">48.51</td>
<td valign="top" rowspan="3" align="center">25.1</td>
<td valign="top" rowspan="3" align="center">1.116</td>
<td valign="top" align="center">1.085</td>
<td valign="top" align="center">0.028</td>
<td valign="top" rowspan="3" align="center">CL</td>
<td valign="top" rowspan="3" align="center">80</td>
<td valign="middle" align="center">0.13</td>
<td valign="middle" align="center">1219</td>
</tr>
<tr>
<td valign="middle" align="center">D6-2</td>
<td valign="top" align="center">1.075</td>
<td valign="top" align="center">0.037</td>
<td valign="middle" align="center">0.15</td>
<td valign="middle" align="center">473</td>
</tr>
<tr>
<td valign="middle" align="center">D6-3</td>
<td valign="top" align="center">1.074</td>
<td valign="top" align="center">0.038</td>
<td valign="middle" align="center">0.17</td>
<td valign="middle" align="center">5</td>
</tr>
<tr>
<td valign="middle" align="center">D7-1</td>
<td valign="top" rowspan="3" align="center">12.0-12.4</td>
<td valign="top" rowspan="3" align="center">1.87</td>
<td valign="top" rowspan="3" align="center">44.85</td>
<td valign="top" rowspan="3" align="center">51.55</td>
<td valign="top" rowspan="3" align="center">29.9</td>
<td valign="top" rowspan="3" align="center">1.119</td>
<td valign="top" align="center">1.068</td>
<td valign="top" align="center">0.046</td>
<td valign="top" rowspan="3" align="center">CH</td>
<td valign="top" rowspan="3" align="center">80</td>
<td valign="middle" align="center">0.13</td>
<td valign="middle" align="center">587</td>
</tr>
<tr>
<td valign="middle" align="center">D7-2</td>
<td valign="top" align="center">1.062</td>
<td valign="top" align="center">0.051</td>
<td valign="middle" align="center">0.15</td>
<td valign="middle" align="center">87</td>
</tr>
<tr>
<td valign="middle" align="center">D7-3</td>
<td valign="top" align="center">1.074</td>
<td valign="top" align="center">0.040</td>
<td valign="middle" align="center">0.16</td>
<td valign="middle" align="center">8</td>
</tr>
<tr>
<td valign="middle" align="center">D8-1</td>
<td valign="top" rowspan="3" align="center">15.6~16.0</td>
<td valign="top" rowspan="3" align="center">1.74</td>
<td valign="top" rowspan="3" align="center">33.60</td>
<td valign="top" rowspan="3" align="center">53.64</td>
<td valign="top" rowspan="3" align="center">30.1</td>
<td valign="top" rowspan="3" align="center">0.908</td>
<td valign="top" align="center">0.876</td>
<td valign="top" align="center">0.035</td>
<td valign="top" rowspan="3" align="center">CL</td>
<td valign="top" rowspan="3" align="center">105</td>
<td valign="middle" align="center">0.14</td>
<td valign="middle" align="center">486</td>
</tr>
<tr>
<td valign="middle" align="center">D8-2</td>
<td valign="top" align="center">0.875</td>
<td valign="top" align="center">0.036</td>
<td valign="middle" align="center">0.16</td>
<td valign="middle" align="center">18</td>
</tr>
<tr>
<td valign="middle" align="center">D8-3</td>
<td valign="top" align="center">0.867</td>
<td valign="top" align="center">0.045</td>
<td valign="middle" align="center">0.17</td>
<td valign="middle" align="center">4</td>
</tr>
<tr>
<td valign="middle" align="center">D9-1</td>
<td valign="top" rowspan="3" align="center">16.0-16.4</td>
<td valign="top" rowspan="3" align="center">1.71</td>
<td valign="top" rowspan="3" align="center">23.54</td>
<td valign="top" rowspan="3" align="center">47.99</td>
<td valign="top" rowspan="3" align="center">22.4</td>
<td valign="top" rowspan="3" align="center">0.836</td>
<td valign="top" align="center">0.803</td>
<td valign="top" align="center">0.039</td>
<td valign="top" rowspan="3" align="center">CL</td>
<td valign="top" rowspan="3" align="center">105</td>
<td valign="middle" align="center">0.13</td>
<td valign="middle" align="center">440</td>
</tr>
<tr>
<td valign="middle" align="center">D9-2</td>
<td valign="top" align="center">0.796</td>
<td valign="top" align="center">0.048</td>
<td valign="middle" align="center">0.14</td>
<td valign="middle" align="center">215</td>
</tr>
<tr>
<td valign="middle" align="center">D9-3</td>
<td valign="top" align="center">0.798</td>
<td valign="top" align="center">0.045</td>
<td valign="middle" align="center">0.16</td>
<td valign="middle" align="center">30</td>
</tr>
<tr>
<td valign="middle" align="center">D10-1</td>
<td valign="top" rowspan="3" align="center">16.4-16.8</td>
<td valign="top" rowspan="3" align="center">1.80</td>
<td valign="top" rowspan="3" align="center">30.74</td>
<td valign="top" rowspan="3" align="center">43.35</td>
<td valign="top" rowspan="3" align="center">20.5</td>
<td valign="top" rowspan="3" align="center">0.981</td>
<td valign="top" align="center">0.920</td>
<td valign="top" align="center">0.062</td>
<td valign="top" rowspan="3" align="center">CL</td>
<td valign="top" rowspan="3" align="center">110</td>
<td valign="middle" align="center">0.12</td>
<td valign="middle" align="center">530</td>
</tr>
<tr>
<td valign="middle" align="center">D10-2</td>
<td valign="top" align="center">0.929</td>
<td valign="top" align="center">0.053</td>
<td valign="middle" align="center">0.15</td>
<td valign="middle" align="center">90</td>
</tr>
<tr>
<td valign="middle" align="center">D10-3</td>
<td valign="top" align="center">0.933</td>
<td valign="top" align="center">0.049</td>
<td valign="middle" align="center">0.17</td>
<td valign="middle" align="center">80</td>
</tr>
<tr>
<td valign="middle" align="center">D11-1</td>
<td valign="top" rowspan="3" align="center">17.2-17.6</td>
<td valign="top" rowspan="3" align="center">2.01</td>
<td valign="top" rowspan="3" align="center">40.00</td>
<td valign="top" rowspan="3" align="center">46.58</td>
<td valign="top" rowspan="3" align="center">22.4</td>
<td valign="top" rowspan="3" align="center">0.984</td>
<td valign="top" align="center">0.945</td>
<td valign="top" align="center">0.039</td>
<td valign="top" rowspan="3" align="center">CH</td>
<td valign="top" rowspan="3" align="center">115</td>
<td valign="middle" align="center">0.08</td>
<td valign="middle" align="center">223</td>
</tr>
<tr>
<td valign="middle" align="center">D11-2</td>
<td valign="top" align="center">0.934</td>
<td valign="top" align="center">0.050</td>
<td valign="middle" align="center">0.11</td>
<td valign="middle" align="center">26</td>
</tr>
<tr>
<td valign="middle" align="center">D11-3</td>
<td valign="top" align="center">0.929</td>
<td valign="top" align="center">0.056</td>
<td valign="middle" align="center">0.13</td>
<td valign="middle" align="center">21</td>
</tr>
<tr>
<td valign="middle" align="center">D12-1</td>
<td valign="top" rowspan="3" align="center">18.8-19.2</td>
<td valign="top" rowspan="3" align="center">1.94</td>
<td valign="top" rowspan="3" align="center">28.10</td>
<td valign="top" rowspan="3" align="center">52.36</td>
<td valign="top" rowspan="3" align="center">29.2</td>
<td valign="top" rowspan="3" align="center">0.788</td>
<td valign="top" align="center">0.754</td>
<td valign="top" align="center">0.043</td>
<td valign="top" rowspan="3" align="center">CH</td>
<td valign="top" rowspan="3" align="center">125</td>
<td valign="middle" align="center">0.19</td>
<td valign="middle" align="center">213</td>
</tr>
<tr>
<td valign="middle" align="center">D12-2</td>
<td valign="top" align="center">0.735</td>
<td valign="middle" align="center">0.067</td>
<td valign="middle" align="center">0.23</td>
<td valign="middle" align="center">40</td>
</tr>
<tr>
<td valign="middle" align="center">D12-3</td>
<td valign="top" align="center">0.736</td>
<td valign="middle" align="center">0.066</td>
<td valign="middle" align="center">0.29</td>
<td valign="middle" align="center">20</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>H is the depth below the seabed, &#x3c1; is the natural density, w is the natural water content, w<sub>L</sub> is the liquid limit, I<sub>p</sub> is the plasticity index, e<sub>0</sub> is the initial void ratio, e<sub>c</sub> is the void ratio after consolidation, and N<sub>f</sub> is the number of cycles to failure.</p>
</fn>
</table-wrap-foot>
</table-wrap>
<fig id="f4" position="float">
<label>Figure&#xa0;4</label>
<caption>
<p>Soil classification lines.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1300005-g004.tif"/>
</fig>
</sec>
</sec>
<sec id="s4">
<label>4</label>
<title>Consolidated undrained triaxial test</title>
<sec id="s4_1">
<label>4.1</label>
<title>Test program</title>
<p>The undrained cyclic triaxial tests were conducted using a dynamic triaxial system provided by GDS Instruments Ltd., UK. <xref ref-type="bibr" rid="B12">Chen et&#xa0;al. (2020)</xref> and <xref ref-type="bibr" rid="B25">Ma et&#xa0;al. (2023)</xref> offer more comprehensive details. <xref ref-type="table" rid="T2">
<bold>Table&#xa0;2</bold>
</xref> lists the primary technical specifications of the controller parameters, sensor range, accuracy, deviation, and other pertinent details. The following must be considered to conduct undisturbed marine clay cyclic triaxial tests following ASTM D5311 (<xref ref-type="bibr" rid="B6">ASTM, 2013</xref>): (1) Mold undisturbed marine clay samples into solid cylindrical specimens measuring 50 mm in diameter and 100 mm in height. (2) Situate the prepared specimens in a saturation vessel within a vacuum saturation chamber, initiating specimen saturation via the vacuum method (<xref ref-type="bibr" rid="B22">Lu et&#xa0;al., 2021</xref>). (3) Once vacuum saturation concludes, position the sample atop the pedestal in the dynamic triaxial system. (4) Implement backpressure saturation; after each stage, determine the <italic>B</italic> value, continuing until <italic>B</italic> exceeds 0.95, signifying complete saturation. (5) Apply uniform consolidation to the fully saturated specimen, selecting the confining pressure based on <italic>in-situ</italic> effective stresses. Based on ASTM D4767 (<xref ref-type="bibr" rid="B5">ASTM, 2020</xref>), consolidation is deemed complete when the average strain rate of the specimen falls below 1 &#xd7; 10<sup>&#x2212;3</sup>%/min. Assessing sample quality or disturbance degree prior to laboratory testing is crucial. <xref ref-type="bibr" rid="B24">Lunne et&#xa0;al. (1997)</xref> index, assessing sample quality based on void ratio alterations due to loading relative to <italic>in-situ</italic> effective stresses, was employed in this study, as indicated in <xref ref-type="table" rid="T1">
<bold>Table&#xa0;1</bold>
</xref>. The findings categorize all examined samples as either &#x201c;very good to excellent&#x201d; or &#x201c;good to fair,&#x201d; with evaluation criteria detailed in <xref ref-type="table" rid="T3">
<bold>Table&#xa0;3</bold>
</xref>.</p>
<table-wrap id="T2" position="float">
<label>Table&#xa0;2</label>
<caption>
<p>The main technical specifications of the GDS dynamic triaxial test apparatus.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" align="center">Sensor</th>
<th valign="middle" align="center">Range</th>
<th valign="middle" align="center">Deviation</th>
<th valign="middle" align="center">Accuracy</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="center">Axial Force</td>
<td valign="middle" align="center">5 kN</td>
<td valign="middle" align="center">0.1% FS</td>
<td valign="middle" align="center">0.2 N</td>
</tr>
<tr>
<td valign="middle" align="center">Axial Displacement</td>
<td valign="middle" align="center">&#xb1; 50 mm</td>
<td valign="middle" align="center">0.15% FS</td>
<td valign="middle" align="center">0.2 &#x3bc;m</td>
</tr>
<tr>
<td valign="middle" align="center">Axial Loading Frequency</td>
<td valign="middle" align="center">&#x2264; 2 Hz</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">&#x2013;</td>
</tr>
<tr>
<td valign="middle" align="center">Confining Pressure/Back Pressure</td>
<td valign="middle" align="center">2 MPa</td>
<td valign="middle" align="center">0.15% FS</td>
<td valign="middle" align="center">1 kPa</td>
</tr>
<tr>
<td valign="middle" align="center">Confining Pressure/Back Pressure Volume</td>
<td valign="middle" align="center">200 mm<sup>3</sup>
</td>
<td valign="middle" align="center">0.25% FS</td>
<td valign="middle" align="center">0.001 mm<sup>3</sup>
</td>
</tr>
<tr>
<td valign="middle" align="center">Pore Water Pressure</td>
<td valign="middle" align="center">2 MPa</td>
<td valign="middle" align="center">0.15% FS</td>
<td valign="middle" align="center">1 kPa</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>FS (Full Scale) = Maximum Range.</p>
</fn>
</table-wrap-foot>
</table-wrap>
<table-wrap id="T3" position="float">
<label>Table&#xa0;3</label>
<caption>
<p>Criteria for evaluation of soil sample quality (<xref ref-type="bibr" rid="B24">Lunne et&#xa0;al., 1997</xref>).</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" rowspan="2" align="center">OCR</th>
<th valign="middle" colspan="4" align="center">&#x394;e/e<sub>0</sub>
</th>
</tr>
<tr>
<th valign="middle" align="center">Very good to excellent</th>
<th valign="middle" align="center">Good to fair</th>
<th valign="middle" align="center">Poor</th>
<th valign="middle" align="center">Very poor</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="center">1-2</td>
<td valign="middle" align="center">&lt;0.04</td>
<td valign="middle" align="center">0.04-0.07</td>
<td valign="middle" align="center">0.07-0.14</td>
<td valign="middle" align="center">&gt;0.14</td>
</tr>
<tr>
<td valign="middle" align="center">2-4</td>
<td valign="middle" align="center">&lt;0.03</td>
<td valign="middle" align="center">0.03-0.05</td>
<td valign="middle" align="center">0.05-0.10</td>
<td valign="middle" align="center">&gt;0.10</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>&#x394;e is the change in void ratio reconsolidated to in-situ stress, and e<sub>0</sub> is the initial void ratio.</p>
</fn>
</table-wrap-foot>
</table-wrap>
<p>Post-consolidation, sinusoidal wave loading at a frequency of 0.1 Hz is applied to the specimen. The specific test plan is listed in <xref ref-type="table" rid="T1">
<bold>Table&#xa0;1</bold>
</xref>. Several tests involving three distinct cyclic stress ratio (<italic>CSR</italic>) levels are conducted on specimens sharing the same identification. As shown in <xref ref-type="disp-formula" rid="eq1">Equation (1)</xref>, the <italic>CSR</italic> is defined as follows:</p>
<disp-formula id="eq1">
<label>(1)</label>
<mml:math display="block" id="M1">
<mml:mrow>
<mml:mi>C</mml:mi>
<mml:mi>S</mml:mi>
<mml:mi>R</mml:mi>
<mml:mo>=</mml:mo>
<mml:msub>
<mml:mi>&#x3c3;</mml:mi>
<mml:mi>d</mml:mi>
</mml:msub>
<mml:mo stretchy="false">/</mml:mo>
<mml:mn>2</mml:mn>
<mml:msubsup>
<mml:mi>&#x3c3;</mml:mi>
<mml:mrow>
<mml:mi>c</mml:mi>
<mml:mn>0</mml:mn>
</mml:mrow>
<mml:mo>'</mml:mo>
</mml:msubsup>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>&#x3c3;</italic>
<sub>d</sub> is the dynamic Stress Amplitude, <italic>&#x3c3;</italic>
<sup>&#x2032;</sup>
<sub>c0</sub> is the initial effective consolidation stress.</p>
</sec>
<sec id="s4_2">
<label>4.2</label>
<title>Representative cyclic responses</title>
<p>
<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5</bold>
</xref> displays typical results for the excess pore water pressure ratio <italic>r</italic>
<sub>u</sub>, axial strain (<italic>&#x3f5;</italic>) curves, cyclic axial stress, deviator stress-axial strain curve, and effective stress path for D11-2. In these results, the excess pore water pressure ratio (<italic>r</italic>
<sub>u</sub>) is the ratio of excess pore pressure to initial confining stress. The double amplitude axial strain (<italic>&#x3f5;</italic>
<sub>DA</sub>) is the difference between the maximum and minimum axial strains in each cycle. <italic>N</italic>
<sub>f</sub> is the number of cycles needed for the specimen to meet the failure criterion, with this criterion being <italic>&#x3f5;</italic>
<sub>DA</sub> reaching 15% in this test. <xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5A</bold>
</xref> indicates that the development of &#x3f5; exhibits progressive characteristics during the cyclic loading process. Initially, <italic>&#x3f5;</italic> increases slowly in a linear manner. As the number of cyclic loading cycles <italic>N</italic> increases, <italic>&#x3f5;</italic> grows rapidly, reaching the failure criterion after a relatively small number of cycles. <xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5B</bold>
</xref> shows that under cyclic loading, the rise in excess water pore pressure in the clay specimen is gradual, and it is challenging for <italic>r</italic>
<sub>u</sub> to increase to 1.0. At failure, <italic>r</italic>
<sub>u</sub> is only 0.48, attributed to the lower permeability of marine clay and the ongoing disruption of its cohesive structure due to cyclic loading. <xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5C</bold>
</xref> shows the relationship between the number of cycles and the axial stress. <xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5D</bold>
</xref> demonstrates that as <italic>N</italic> increases, the inclination of the hysteresis loop gradually diminishes, indicating a progressive decrease in the specimen&#x2019;s stiffness and strength. The shape evolves from &#x201c;elliptical&#x201d; to &#x201c;Z&#x201d; type. Concurrently, the vertical effective stress decreases, reflecting the development of pore water pressure during the cyclic process. The effective stress path shifts to the left with increasing cycle numbers, as shown in <xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5E</bold>
</xref>.</p>
<fig id="f5" position="float">
<label>Figure&#xa0;5</label>
<caption>
<p>Undrained cyclic triaxial typical test results (<bold>A&#x2013;E</bold> show five different typical test results).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1300005-g005.tif"/>
</fig>
</sec>
<sec id="s4_3">
<label>4.3</label>
<title>Cyclic resistance in laboratory tests</title>
<p>
<xref ref-type="bibr" rid="B18">Ishihara et&#xa0;al. (1980)</xref> proposed using a power function to describe the relationship between <italic>CSR</italic> and <italic>N</italic>
<sub>f</sub>. The relationship <xref ref-type="disp-formula" rid="eq2">Equation (2)</xref> is as follows:</p>
<disp-formula id="eq2">
<label>(2)</label>
<mml:math display="block" id="M2">
<mml:mrow>
<mml:mi>C</mml:mi>
<mml:mi>S</mml:mi>
<mml:mi>R</mml:mi>
<mml:mo>=</mml:mo>
<mml:mi>a</mml:mi>
<mml:mo>&#xb7;</mml:mo>
<mml:msubsup>
<mml:mi>N</mml:mi>
<mml:mi>f</mml:mi>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>b</mml:mi>
</mml:mrow>
</mml:msubsup>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>a</italic> and <italic>b</italic> are the fitting parameters.</p>
<p>
<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6</bold>
</xref> depicts the relationship curve between the CSR and <italic>N</italic>
<sub>f</sub> of the clay samples from the Shaba wind farm, with a dashed line representing the fitting curve. The results indicated that as <italic>CSR</italic> increases, <italic>N</italic>
<sub>f</sub> decreases, demonstrating that the marine clay is more prone to damage under high cyclic loading conditions. However, the change pattern in cyclic resistance for each specimen remains unclear.</p>
<fig id="f6" position="float">
<label>Figure&#xa0;6</label>
<caption>
<p>Dynamic strength curve of marine clay.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1300005-g006.tif"/>
</fig>
<p>
<italic>N</italic>
<sub>f</sub> directly correlates with the seismic moment. Based on <xref ref-type="bibr" rid="B17">Idriss and Boulanger (2008)</xref>, an <italic>N</italic>
<sub>f</sub> of 15 typically corresponds to a seismic moment of 7.5. Hence, the <italic>CSR</italic> value corresponding to 15 cycles of uniform loading, extracted from the <italic>N</italic>
<sub>f</sub> vs. <italic>CSR</italic> correlation curve, represents its cyclic resistance (<italic>CRR</italic>
<sub>lab</sub>), as displayed in <xref ref-type="table" rid="T4">
<bold>Table&#xa0;4</bold>
</xref>. <xref ref-type="fig" rid="f7">
<bold>Figure&#xa0;7</bold>
</xref> illustrates the correlations between <italic>H</italic>, <italic>&#x3c1;</italic>, <italic>w</italic>, <italic>I</italic>
<sub>p</sub>, and <italic>CRR</italic>
<sub>lab</sub> of the tested sample. It indicates that <italic>CRR</italic>
<sub>lab</sub> does not significantly correlate with <italic>H</italic>, <italic>&#x3c1;</italic>, <italic>w</italic>, and <italic>I</italic>
<sub>p</sub>. Thus, it cannot evaluate <italic>CRR</italic>
<sub>lab</sub> by a single physical index of marine clay.</p>
<table-wrap id="T4" position="float">
<label>Table&#xa0;4</label>
<caption>
<p>Cyclic resistance of marine clay.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" align="center">Test number</th>
<th valign="middle" align="center">D1</th>
<th valign="middle" align="center">D2</th>
<th valign="middle" align="center">D3</th>
<th valign="middle" align="center">D4</th>
<th valign="middle" align="center">D5</th>
<th valign="middle" align="center">D6</th>
<th valign="middle" align="center">D7</th>
<th valign="middle" align="center">D8</th>
<th valign="middle" align="center">D9</th>
<th valign="middle" align="center">D10</th>
<th valign="middle" align="center">D11</th>
<th valign="middle" align="center">D12</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="left">
<italic>CRR</italic>
<sub>lab</sub>
</td>
<td valign="middle" align="left">0.161</td>
<td valign="middle" align="left">0.185</td>
<td valign="middle" align="left">0.322</td>
<td valign="middle" align="left">0.366</td>
<td valign="middle" align="left">0.204</td>
<td valign="middle" align="left">0.164</td>
<td valign="middle" align="left">0.157</td>
<td valign="middle" align="left">0.161</td>
<td valign="middle" align="left">0.166</td>
<td valign="middle" align="left">0.177</td>
<td valign="middle" align="left">0.120</td>
<td valign="middle" align="left">0.267</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="f7" position="float">
<label>Figure&#xa0;7</label>
<caption>
<p>Correlation between <italic>H</italic>, <italic>&#x3c1;</italic>, <italic>w</italic>, <italic>I</italic>
<sub>p</sub>, and <italic>CRR</italic>
<sub>lab</sub>. (<bold>A&#x2013;D</bold> are four different factors).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1300005-g007.tif"/>
</fig>
</sec>
</sec>
<sec id="s5">
<label>5</label>
<title>CPTu-based evaluation method for cyclic resistance of marine clay</title>
<p>Considering cone resistance as an indicator of the failure strength of soils <italic>in situ</italic> (<xref ref-type="bibr" rid="B37">Yu, 2006</xref>) and sleeve friction <italic>f</italic>
<sub>s</sub> as a measure of soil strength post-failure, <xref ref-type="bibr" rid="B30">Robertson and Wride (1998)</xref> proposed a complex cyclic resistance evaluation method. This approach considers <italic>in-situ</italic> vertical stress, soil behavior type index <italic>I</italic>
<sub>c</sub>, and modified cone resistance <italic>q</italic>
<sub>t1N</sub>. <xref ref-type="bibr" rid="B20">Juang et&#xa0;al. (2008)</xref> simplified the parameters and developed a method using the soil behavior type index <italic>I</italic>
<sub>c,BJ</sub> and modified cone resistance <italic>q</italic>
<sub>t1N</sub>. Compared to Robertson and Wride&#x2019;s model, Juang et&#xa0;al.&#x2019;s approach accounts for the influence of excess pore water pressure, offering insights into soil consolidation and permeability properties (<xref ref-type="bibr" rid="B11">Chai et&#xa0;al., 2011</xref>). In contrast, Olsen&#x2019;s method (<xref ref-type="bibr" rid="B27">Olsen, 1994</xref>) does not consider soil type and excess pore water pressure. These three models, based on CPTu tests on terrestrial soils, are summarized in <xref ref-type="table" rid="T5">
<bold>Table&#xa0;5</bold>
</xref>. <xref ref-type="fig" rid="f8">
<bold>Figure&#xa0;8</bold>
</xref> presents the field cyclic resistance ratio (<italic>CRR</italic>
<sub>field</sub>) calculated using these three models for four borehole locations. It reveals generally consistent trends in results calculated by each model with depth, albeit with notable differences in numerical values. At borehole locations CPTu 1, CPTu 3, and CPTu 4, Olsen&#x2019;s model yields the highest <italic>CRR</italic>
<sub>field,</sub> followed by the Robertson model, with Juang&#x2019;s model providing the lowest values. In contrast, at borehole locations CPTu 2, Olsen&#x2019;s model results in the lowest CRRfield, Juang&#x2019;s model is intermediate, and the Robertson model calculates the highest values.</p>
<table-wrap id="T5" position="float">
<label>Table&#xa0;5</label>
<caption>
<p>CRR<sub>field</sub> calculation model based on CPTu.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" align="center">Reference</th>
<th valign="middle" align="center">Empirical formula</th>
<th valign="middle" align="center">Note</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" rowspan="8" align="center">
<xref ref-type="bibr" rid="B30">Robertson and Wride (1998)</xref>
</td>
<td valign="middle" align="left">
<inline-formula>
<mml:math display="inline" id="im1">
<mml:mrow>
<mml:mtable>
<mml:mtr>
<mml:mtd>
<mml:mrow>
<mml:mi>C</mml:mi>
<mml:mi>R</mml:mi>
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mrow>
<mml:mi>f</mml:mi>
<mml:mi>i</mml:mi>
<mml:mi>e</mml:mi>
<mml:mi>l</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mn>93</mml:mn>
<mml:msup>
<mml:mrow>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mn>1</mml:mn>
<mml:mi>N</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>c</mml:mi>
<mml:mi>s</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mn>1000</mml:mn>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mn>3</mml:mn>
</mml:msup>
<mml:mo>+</mml:mo>
<mml:mn>0.08</mml:mn>
<mml:mo>,</mml:mo>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mn>50</mml:mn>
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<mml:msub>
<mml:mi>q</mml:mi>
<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mn>1</mml:mn>
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<mml:mo>,</mml:mo>
<mml:mi>c</mml:mi>
<mml:mi>s</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&lt;</mml:mo>
<mml:mn>160</mml:mn>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd>
<mml:mrow>
<mml:mi>C</mml:mi>
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<mml:msub>
<mml:mi>R</mml:mi>
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<mml:mi>i</mml:mi>
<mml:mi>e</mml:mi>
<mml:mi>l</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mn>0.833</mml:mn>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mn>1</mml:mn>
<mml:mi>N</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>c</mml:mi>
<mml:mi>s</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mn>1000</mml:mn>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mo>+</mml:mo>
<mml:mn>0.05</mml:mn>
<mml:mo>,</mml:mo>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mn>1</mml:mn>
<mml:mi>N</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>c</mml:mi>
<mml:mi>s</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&lt;</mml:mo>
<mml:mn>50</mml:mn>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:mrow>
</mml:math>
</inline-formula>
</td>
<td valign="top" rowspan="8" align="left">
<italic>&#x3c3;</italic>
<sub>vo</sub> = <italic>in-situ</italic> total vertical stress.<break/>
<italic>&#x3c3;</italic>&#x2019;<sub>vo</sub> = <italic>in-situ</italic> effective vertical stress.<break/>
<italic>n</italic> = stress exponent.<break/>
<italic>p</italic>
<sub>a</sub> = atmospheric pressure.<break/>
<italic>q</italic>
<sub>t1N</sub> = modified cone resistance<break/>
<italic>q</italic>
<sub>t</sub> = total cone resistance<break/>
<italic>Q</italic>
<sub>tn</sub>, <italic>q</italic>
<sub>t1N,cs</sub>, <italic>F</italic>
<sub>r</sub> = cone parameters.<break/>
<italic>f</italic>
<sub>s</sub> = sleeve friction.<break/>
<italic>I</italic>
<sub>c</sub> = soil behavior type index.<break/>
<italic>K</italic>
<sub>c</sub> is a function of <italic>I</italic>
<sub>c</sub>.</td>
</tr>
<tr>
<td valign="middle" align="left">
<inline-formula>
<mml:math display="inline" id="im2">
<mml:mrow>
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mn>1</mml:mn>
<mml:mi>N</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>c</mml:mi>
<mml:mi>s</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mn>1</mml:mn>
<mml:mi>N</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>
</td>
</tr>
<tr>
<td valign="middle" align="center">
<inline-formula>
<mml:math display="inline" id="im3">
<mml:mrow>
<mml:mtable>
<mml:mtr>
<mml:mtd>
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mn>1.0</mml:mn>
<mml:mo>,</mml:mo>
<mml:msub>
<mml:mi>I</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
<mml:mo>&#x2264;</mml:mo>
<mml:mn>1.64</mml:mn>
</mml:mrow>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd>
<mml:mrow>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>0.403</mml:mn>
<mml:msubsup>
<mml:mi>I</mml:mi>
<mml:mi>c</mml:mi>
<mml:mn>2</mml:mn>
</mml:msubsup>
<mml:mo>+</mml:mo>
<mml:mn>5.58</mml:mn>
<mml:msubsup>
<mml:mi>I</mml:mi>
<mml:mi>c</mml:mi>
<mml:mn>3</mml:mn>
</mml:msubsup>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>21.63</mml:mn>
<mml:msubsup>
<mml:mi>I</mml:mi>
<mml:mi>c</mml:mi>
<mml:mn>2</mml:mn>
</mml:msubsup>
<mml:mo>+</mml:mo>
<mml:mn>33.75</mml:mn>
<mml:msub>
<mml:mi>I</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>17.88</mml:mn>
</mml:mrow>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:mrow>
</mml:math>
</inline-formula>
</td>
</tr>
<tr>
<td valign="middle" align="center">
<inline-formula>
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<mml:mrow>
<mml:msub>
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<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mn>1</mml:mn>
<mml:mi>N</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mfrac>
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<mml:mrow>
<mml:mi>v</mml:mi>
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<mml:mrow>
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</inline-formula>
</td>
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<tr>
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<inline-formula>
<mml:math display="inline" id="im5">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>=</mml:mo>
<mml:mn>0.381</mml:mn>
<mml:msub>
<mml:mi>I</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
<mml:mo>+</mml:mo>
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<mml:mn>1.0</mml:mn>
</mml:mrow>
</mml:math>
</inline-formula>
</td>
</tr>
<tr>
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<tr>
<td valign="middle" align="left">
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</inline-formula>
</td>
</tr>
<tr>
<td valign="middle" rowspan="5" align="center">
<xref ref-type="bibr" rid="B20">Juang et&#xa0;al. (2008)</xref>
</td>
<td valign="middle" align="center">
<inline-formula>
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</td>
<td valign="top" rowspan="5" align="left">A&#x3001;B&#x3001;C = fitting parameter.<break/>
<italic>I</italic>
<sub>c,BJ</sub> = soil behaviour type index.<break/>
<italic>q</italic>
<sub>c</sub> = modified cone resistance.<break/>
<italic>Q</italic>
<sub>t</sub>, <italic>q</italic>
<sub>c1</sub>, <italic>F</italic>
<sub>r</sub> = cone parameters.<break/>
<italic>B<sub>q</sub>
</italic> = excess pore pressure ratio.</td>
</tr>
<tr>
<td valign="middle" align="center">
<inline-formula>
<mml:math display="inline" id="im10">
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<mml:mn>100</mml:mn>
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<mml:mo>&#x2212;</mml:mo>
<mml:mn>14.7</mml:mn>
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</mml:math>
</inline-formula>
</td>
</tr>
<tr>
<td valign="middle" align="center">
<inline-formula>
<mml:math display="inline" id="im11">
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<mml:mi>B</mml:mi>
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</inline-formula>
</td>
</tr>
<tr>
<td valign="middle" align="center">
<inline-formula>
<mml:math display="inline" id="im12">
<mml:mrow>
<mml:mi>C</mml:mi>
<mml:mo>=</mml:mo>
<mml:mn>0.059</mml:mn>
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</inline-formula>
</td>
</tr>
<tr>
<td valign="middle" align="center">
<inline-formula>
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<mml:msub>
<mml:mi>I</mml:mi>
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</inline-formula> <inline-formula>
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</mml:math>
</inline-formula>
</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">
<xref ref-type="bibr" rid="B27">Olsen (1994)</xref>
</td>
<td valign="middle" align="center">
<inline-formula>
<mml:math display="inline" id="im15">
<mml:mrow>
<mml:mi>C</mml:mi>
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<mml:msub>
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<mml:mi>q</mml:mi>
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</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>0.025</mml:mn>
<mml:mo>+</mml:mo>
<mml:mn>0.17</mml:mn>
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mi>f</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
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<mml:mi>R</mml:mi>
<mml:mi>f</mml:mi>
<mml:mn>2</mml:mn>
</mml:msubsup>
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<mml:mn>0.0016</mml:mn>
<mml:msubsup>
<mml:mi>R</mml:mi>
<mml:mi>f</mml:mi>
<mml:mn>3</mml:mn>
</mml:msubsup>
</mml:mrow>
</mml:math>
</inline-formula>
</td>
<td valign="top" rowspan="2" align="left">
<italic>R</italic>
<sub>f</sub> = friction ratio.<break/>
<italic>q</italic>
<sub>c</sub> = modified cone resistance.</td>
</tr>
<tr>
<td valign="middle" align="left">
<inline-formula>
<mml:math display="inline" id="im16">
<mml:mrow>
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mrow>
<mml:mi>c</mml:mi>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:msup>
<mml:mrow>
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</mml:mrow>
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</mml:mrow>
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</mml:mrow>
</mml:mrow>
<mml:mrow>
<mml:mn>0.7</mml:mn>
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</mml:msup>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
</inline-formula>
</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="f8" position="float">
<label>Figure&#xa0;8</label>
<caption>
<p>
<italic>CRR</italic>
<sub>field</sub> calculation curve based on CPTu data.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1300005-g008.tif"/>
</fig>
<p>The laboratory test conditions are a simplified representation of field conditions. Differences often arise when applying results from laboratory cyclic triaxial tests to field situations. <xref ref-type="bibr" rid="B32">Seed (1979)</xref> proposed a conversion factor, <italic>C</italic>
<sub>r</sub>, to modify <italic>CRR</italic>
<sub>lab</sub>, yielding <italic>CRR</italic>
<sub>field,</sub> as demonstrated in the subsequent <xref ref-type="disp-formula" rid="eq3">Equation (3)</xref>:</p>
<disp-formula id="eq3">
<label>(3)</label>
<mml:math display="block" id="M3">
<mml:mrow>
<mml:mi>C</mml:mi>
<mml:mi>R</mml:mi>
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mrow>
<mml:mi>f</mml:mi>
<mml:mi>i</mml:mi>
<mml:mi>e</mml:mi>
<mml:mi>l</mml:mi>
<mml:mi>d</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>l</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>b</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mn>0.9</mml:mn>
<mml:mo>&#xb7;</mml:mo>
<mml:msub>
<mml:mi>C</mml:mi>
<mml:mi>r</mml:mi>
</mml:msub>
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<mml:mi>C</mml:mi>
<mml:mi>R</mml:mi>
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mrow>
<mml:mi>l</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>b</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where 0.9 is the correction factor for converting the laboratory cyclic resistance ratio under unidirectional loading to the cyclic resistance ratio under multiple-direction loading conditions in the field, <italic>C</italic>
<sub>r</sub> is taken as 0.7.</p>
<p>Comparisons of <italic>CRR</italic>
<sub>field</sub>, as calculated by various models at respective depths, with <italic>CRR</italic>
<sub>field-lab</sub> determined by the test results are depicted in <xref ref-type="fig" rid="f9">
<bold>Figure&#xa0;9</bold>
</xref>. This figure reveals that Robertson&#x2019;s and Juang&#x2019;s approaches exhibit comparable effectiveness, with most errors remaining under 30% relative to <italic>CRR</italic>
<sub>field-lab</sub>. However, Olsen&#x2019;s method, which does not account for soil type and excess pore water pressure, shows the least accuracy, with errors surpassing 60%.</p>
<fig id="f9" position="float">
<label>Figure&#xa0;9</label>
<caption>
<p>Comparison of CPTu-based <italic>CRR</italic>
<sub>field</sub> calculation results with indoor results <italic>CRR</italic>
<sub>lab</sub>. (<bold>A&#x2013;C</bold> are three different methods).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1300005-g009.tif"/>
</fig>
<p>Accordingly, while <italic>CRR</italic>
<sub>field</sub> models derived from CPTu data show some applicability, the overall errors are significant. In addition, these models lack a clear functional relationship, potentially limiting their utility in practical engineering projects. As detailed in Section 3, the geotechnical properties of soil layers vary considerably at different depths. Incorporating soil characteristics indicated by <italic>q</italic>
<sub>t</sub>, <italic>u</italic>
<sub>2</sub>, and <italic>f</italic>s, and amalgamating laboratory test outcomes with CPTu data, a discernible functional relationship emerges among the effective cone tip resistance <italic>q</italic>
<sub>E</sub> (= <italic>q</italic>
<sub>t</sub> &#x2212; <italic>u</italic>
<sub>2</sub>), <italic>f</italic>
<sub>s</sub>, and <italic>CRR</italic>
<sub>field-lab</sub>. Thus, an empirical model to predict CRRfield-lab for marine clay was formulated, using <italic>q</italic>
<sub>E</sub>, <italic>f</italic>
<sub>s</sub>, and <italic>H</italic> as independent variables, with <italic>CRR</italic>
<sub>field-lab</sub> as the dependent variable, as delineated in <xref ref-type="disp-formula" rid="eq4">Equation 4</xref>. Notably, <italic>H</italic> accounts for the <italic>in-situ</italic> stress of soils. Through multiple regression analysis, a new <italic>CRR</italic>
<sub>field-lab</sub> evaluation method based on depth-corrected CPTu index [<italic>EXP</italic>(<italic>q</italic>
<sub>E</sub>/<italic>f</italic>
<sub>s</sub>)<sup>0.3</sup>/<italic>H</italic>] was developed, as <xref ref-type="disp-formula" rid="eq4">Equation (4)</xref> shown, and its application to assess <italic>CRR</italic>
<sub>field-lab</sub> for marine clay in the Yangjiang Wind Farm offshore area has demonstrated a robust fit, as illustrated in <xref ref-type="fig" rid="f10">
<bold>Figure&#xa0;10</bold>
</xref>.</p>
<fig id="f10" position="float">
<label>Figure&#xa0;10</label>
<caption>
<p>Dynamic strength evaluation method of marine clay based on CPTu data.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1300005-g010.tif"/>
</fig>
<disp-formula id="eq4">
<label>(4)</label>
<mml:math display="block" id="M4">
<mml:mrow>
<mml:mi>C</mml:mi>
<mml:mi>R</mml:mi>
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mrow>
<mml:mi>f</mml:mi>
<mml:mi>i</mml:mi>
<mml:mi>e</mml:mi>
<mml:mi>l</mml:mi>
<mml:mi>d</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>l</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>b</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mn>0.018</mml:mn>
<mml:mo>+</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mn>0.103</mml:mn>
<mml:msup>
<mml:mi>e</mml:mi>
<mml:mrow>
<mml:msup>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mi>E</mml:mi>
</mml:msub>
<mml:mo stretchy="false">/</mml:mo>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mi>s</mml:mi>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mrow>
<mml:mn>0.3</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:msup>
</mml:mrow>
<mml:mi>H</mml:mi>
</mml:mfrac>
</mml:mrow>
</mml:math>
</disp-formula>
<p>Noted that the CPTu-based <italic>CRR</italic>
<sub>field-lab</sub> prediction model proposed in this study can effectively predict the cyclic resistance of marine clay, which makes up for the difficulty of sampling and high testing costs in offshore engineering. Also, compared with the above three well-developed prediction models (<xref ref-type="bibr" rid="B27">Olsen, 1994</xref>; <xref ref-type="bibr" rid="B30">Robertson and Wride, 1998</xref>; <xref ref-type="bibr" rid="B20">Juang et&#xa0;al., 2008</xref>), the <italic>CRR</italic>
<sub>field-lab</sub> prediction model contains just only fewer basial physical parameters, i.e., if the depth <italic>H</italic> and CPTu data of marine clay are determined, then the <italic>CRR</italic>
<sub>field-lab</sub> can be evaluated quickly and efficiently, which provides a significant advantage in the evaluation of liquefaction triggering of marine soils in practice.</p>
</sec>
<sec id="s6" sec-type="conclusions">
<label>6</label>
<title>Conclusion</title>
<p>This study presents the site investigation and cyclic resistance of marine clay, utilizing CPTu tests and advanced laboratory tests, taking the Shaba wind farm in southern China as a case study. An evaluation method for the cyclic resistance of marine clay, grounded in CPTu data, is introduced. The key conclusions are as follows:</p>
<list list-type="simple">
<list-item>
<p>1. The interpretation of CPTU data and index parameter tests depict the site conditions as having a multilayered and intricate sedimentary structure. The initial void ratio of clay layers shows a gradual increase with depth.</p>
</list-item>
<list-item>
<p>2. Under cyclic loading, the marine clay&#x2019;s hysteresis loop dip angle in the Yangjiang Sea region diminishes progressively, gradually reducing soil stiffness and strength. Concurrently, the maximum strain typically occurs post-peak stress, highlighting the delayed response between stress and strain in marine clay. In addition, the hysteresis curve&#x2019;s expansion toward the stretching direction suggests an elevated risk of tensile failure in the sample.</p>
</list-item>
<list-item>
<p>3. The <italic>CRR</italic>
<sub>lab</sub>, derived from consolidated undrained cyclic triaxial tests, was converted to an <italic>in-situ CRR</italic>
<sub>field-lab</sub>. Notable discrepancies were observed between the calculated results of the existing prediction methods based on CPTu data and the actual <italic>CRR</italic>
<sub>field-lab</sub>. Utilizing the CPTu data <italic>q</italic>
<sub>E</sub>, <italic>f</italic>
<sub>s</sub>, and depth <italic>H</italic>, a linear relationship existed between cyclic resistance and depth-corrected CPTu index [<italic>EXP</italic>(<italic>q</italic>
<sub>E</sub>/<italic>f</italic>
<sub>s</sub>)<sup>0.3</sup>/<italic>H</italic>]. Then an alternative evaluation method to determine the <italic>CRR</italic>
<sub>field-lab</sub> of marine clay was proposed. This method yielded prediction results that align well with engineering practice requirements.</p>
</list-item>
</list>
</sec>
<sec id="s7" sec-type="data-availability">
<title>Data availability statement</title>
<p>The raw data supporting the conclusions of this article will be made available by the authors, without undue reservation.</p>
</sec>
<sec id="s8" sec-type="author-contributions">
<title>Author contributions</title>
<p>QW: Conceptualization, Data curation, Project administration, Resources, Validation, Visualization, Writing &#x2013; original draft, Writing &#x2013; review &amp; editing. EZ: Data curation, Investigation, Methodology, Validation, Writing &#x2013; original draft, Writing &#x2013; review &amp; editing. XX: Data curation, Investigation, Methodology, Validation, Visualization, Writing &#x2013; review &amp; editing. YL: Conceptualization, Methodology, Resources, Supervision, Validation, Visualization, Writing &#x2013; review &amp; editing. GC: Conceptualization, Data curation, Funding acquisition, Supervision, Validation, Visualization, Writing &#x2013; review &amp; editing.</p>
</sec>
</body>
<back>
<sec id="s9" sec-type="funding-information">
<title>Funding</title>
<p>The author(s) declare that no financial support was received for the research, authorship, and/or publication of this article.</p>
</sec>
<sec id="s10" sec-type="COI-statement">
<title>Conflict of interest</title>
<p>Author YX-L was employed by China Energy Engineering Group Guangdong Electric Power Design Institute Co., Ltd.</p>
<p>The remaining authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec id="s11" sec-type="disclaimer">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
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<glossary>
<title>Glossary</title>
<table-wrap position="anchor">
<table frame="hsides">
<tbody>
<tr>
<td valign="middle" align="center">
<italic>q</italic>
<sub>c</sub>
</td>
<td valign="middle" align="left">cone resistance</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>f</italic>
<sub>s</sub>
</td>
<td valign="middle" align="left">sleeve friction</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>u</italic>
<sub>2</sub>
</td>
<td valign="middle" align="left">pore water pressure</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>w</italic>
<sub>0</sub>
</td>
<td valign="middle" align="left">natural water content</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>&#x3c1;</italic>
</td>
<td valign="middle" align="left">natural density</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>I</italic>
<sub>p</sub>
</td>
<td valign="middle" align="left">plasticity index</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>e</italic>
<sub>0</sub>
</td>
<td valign="middle" align="left">initial void ratio</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>w</italic>
<sub>L</sub>
</td>
<td valign="middle" align="left">liquid limit</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>e</italic>
<sub>c</sub>
</td>
<td valign="middle" align="left">void ratio after consolidation</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>N</italic>
<sub>f</sub>
</td>
<td valign="middle" align="left">number of cycles to failure</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>r</italic>
<sub>u</sub>
</td>
<td valign="middle" align="left">excess pore water pressure ratio</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>&#x3f5;</italic>
<sub>DA</sub>
</td>
<td valign="middle" align="left">double amplitude axial strain</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>CRR</italic>
<sub>lab</sub>
</td>
<td valign="middle" align="left">laboratory cyclic resistance</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>CRR</italic>
<sub>field</sub>
</td>
<td valign="middle" align="left">field cyclic resistance</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>CRR</italic>
<sub>field-lab</sub>
</td>
<td valign="middle" align="left">
<italic>CRR</italic>
<sub>lab</sub> based on field correction</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>q</italic>
<sub>E</sub>
</td>
<td valign="middle" align="left">effective cone tip resistance</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>C</italic>
<sub>r</sub>
</td>
<td valign="middle" align="left">correction factor</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>N</italic>
</td>
<td valign="middle" align="left">number of cyclic loading cycles</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>&#x3c3;</italic>&#x2019;<sub>c0</sub>
</td>
<td valign="middle" align="left">initial effective confining pressure</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>&#x3f5;</italic>
</td>
<td valign="middle" align="left">axial strain</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>&#x394;e</italic>
</td>
<td valign="middle" align="left">change of void ratio before and after consolidation</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>a</italic>, <italic>b</italic>
</td>
<td valign="middle" align="left">fitting parameters</td>
</tr>
<tr>
<td valign="middle" align="center">
<italic>CSR</italic>
</td>
<td valign="middle" align="left">cyclic stress ratio</td>
</tr>
</tbody>
</table>
</table-wrap>
</glossary>
</back>
</article>