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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Earth Sci.</journal-id>
<journal-title>Frontiers in Earth Science</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Earth Sci.</abbrev-journal-title>
<issn pub-type="epub">2296-6463</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">1216614</article-id>
<article-id pub-id-type="doi">10.3389/feart.2023.1216614</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Earth Science</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Impact of anti-sticking coating technology on shear strength at the clay-metal interface in cohesive strata</article-title>
<alt-title alt-title-type="left-running-head">Liu et al.</alt-title>
<alt-title alt-title-type="right-running-head">
<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.3389/feart.2023.1216614">10.3389/feart.2023.1216614</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Liu</surname>
<given-names>Pengfei</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Sun</surname>
<given-names>Shicheng</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/2228816/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Yang</surname>
<given-names>Zhao</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Ji</surname>
<given-names>Fuquan</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Xu</surname>
<given-names>Chao</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Zhu</surname>
<given-names>Hanbiao</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>CCCC Second Harbor Engineering Company Ltd.</institution>, <addr-line>Wuhan</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>CCCC First Harbor Engineering Company Ltd.</institution>, <addr-line>Tianjin</addr-line>, <country>China</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>School of Civil Engineering</institution>, <institution>Central South University</institution>, <addr-line>Changsha</addr-line>, <country>China</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1346061/overview">Xuelong Li</ext-link>, Shandong University of Science and Technology, China</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1756709/overview">Danqing Song</ext-link>, South China University of Technology, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/2310539/overview">Cai Ziyong</ext-link>, Central South University, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1341874/overview">Xiangfeng Guo</ext-link>, National University of Singapore, Singapore</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Zhao Yang, <email>45574335@qq.com</email>
</corresp>
</author-notes>
<pub-date pub-type="epub">
<day>21</day>
<month>08</month>
<year>2023</year>
</pub-date>
<pub-date pub-type="collection">
<year>2023</year>
</pub-date>
<volume>11</volume>
<elocation-id>1216614</elocation-id>
<history>
<date date-type="received">
<day>04</day>
<month>05</month>
<year>2023</year>
</date>
<date date-type="accepted">
<day>07</day>
<month>08</month>
<year>2023</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2023 Liu, Sun, Yang, Ji, Xu and Zhu.</copyright-statement>
<copyright-year>2023</copyright-year>
<copyright-holder>Liu, Sun, Yang, Ji, Xu and Zhu</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 shield machine is clogged frequently when tunneling in cohesive strata. Shield clogging is closely linked to the shear strength exhibited at the clay-metal interface. To investigate the impact of anti-sticking coating technology on the shear strength at the clay-metal interface, a series of direct shear tests were conducted. The obtained test results revealed an initial increase in shear stress at the clay-metal interface as shear displacement increased, eventually reaching a state of stabilization. The shear strength exhibited a gradual increase initially, followed by a significant increase, and eventually reached a plateau with the rise in the consistency index. It was observed that the adhesion between the anti-adhesion coating and clay was relatively weak, but the presence of the anti-adhesion coating effectively reduced the risk of shield clogging.</p>
</abstract>
<kwd-group>
<kwd>shield tunneling</kwd>
<kwd>cohesive strata</kwd>
<kwd>tunnel excavation</kwd>
<kwd>anti-adhesion coating</kwd>
<kwd>shield clogging</kwd>
</kwd-group>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-at-acceptance</meta-name>
<meta-value>Geohazards and Georisks</meta-value>
</custom-meta>
</custom-meta-wrap>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="s1">
<title>1 Introduction</title>
<p>Currently, China has emerged as the leading country worldwide in terms of scale and complexity of tunnel and underground construction (<xref ref-type="bibr" rid="B28">Song et al., 2021</xref>; <xref ref-type="bibr" rid="B39">Xu et al., 2022</xref>). The 21st century has witnessed significant advancements in underground engineering in China (<xref ref-type="bibr" rid="B7">Ding and Xu, 2017</xref>; <xref ref-type="bibr" rid="B21">Liu et al., 2020</xref>; <xref ref-type="bibr" rid="B11">Huang et al., 2022</xref>). Over the past two&#xa0;decades, numerous tunnels have been successfully constructed (<xref ref-type="bibr" rid="B32">Wang et al., 2022a</xref>; <xref ref-type="bibr" rid="B46">Zhou et al., 2022</xref>; <xref ref-type="bibr" rid="B31">Wang et al., 2023a</xref>). The shield tunneling technology, known for its safety and efficiency, has been extensively utilized in the construction of urban subways and municipal tunnels (<xref ref-type="bibr" rid="B14">Langmaack and Lee, 2016</xref>; <xref ref-type="bibr" rid="B40">Xu et al., 2020</xref>; <xref ref-type="bibr" rid="B13">Jia and Gao, 2022</xref>). However, when a shield machine traverses clayey strata, the excavated clayey muck tends to adhere to the cutter head and cutters (<xref ref-type="bibr" rid="B10">Hollmann and Thewes, 2013</xref>; <xref ref-type="bibr" rid="B36">Wang et al., 2023b</xref>; <xref ref-type="bibr" rid="B9">Gao et al., 2023</xref>). The force exerted during shield pushing causes the attached muck to consolidate, resulting in the formation of a layer of hardened muck on the surface of cutter head (<xref ref-type="bibr" rid="B29">Thewes and Hollmann, 2016</xref>; <xref ref-type="bibr" rid="B43">Zeng et al., 2020</xref>; <xref ref-type="bibr" rid="B15">Li et al., 2021</xref>). As the hard muck rubs against the ground, heat is generated at the tunneling face. This heat accelerates the consolidation of muck adhering to the steel instruments. Consequently, the cutter becomes completely engulfed in consolidated muck, rendering it incapable of cutting and leading to a clogging in the shield machine. The shield clogging can have various adverse effects. In milder cases, it can lead to a loss of cutting efficiency of the cutting tools, significantly impacting the tunneling construction efficiency. In more severe instances, it can cause surface subsidence, posing risks to surface structures and personnel safety. For example, a large diameter shield tunneling machine was clogged when it was passing through a railway station in Shenzhen, China. The on-site construction personnel used frequent cabin cleaning to remove the soil adhered on the cutter head, resulting in a significant increase in ground settlement and settlement rate, posing a huge threat to the safety of surface railway station.</p>
<p>Based on current engineering experience, both slurry pressure balance (SPB) and Earth pressure balance (EPB) shields can face clogging issues in clayey strata (<xref ref-type="bibr" rid="B6">Chen et al., 2022</xref>; <xref ref-type="bibr" rid="B17">Li et al., 2022</xref>). To mitigate shield clogging during EPB tunneling, soil conditioning chemicals are frequently injected ahead of the cutter head (<xref ref-type="bibr" rid="B22">Martinelli et al., 2015</xref>; <xref ref-type="bibr" rid="B47">Zumsteg and Langmaack, 2017</xref>; <xref ref-type="bibr" rid="B19">Liu et al., 2018</xref>; <xref ref-type="bibr" rid="B33">Wang et al., 2021</xref>). However, the injection holes for soil conditioning chemicals in the cutter head are sparsely distributed, making it challenging to evenly distribute the injected chemicals across the entire cutter head. Consequently, certain areas may still experience shield clogging. During SPB shield tunneling, the central position of the cutter head is washed with slurry sprayed from the pipeline to prevent muck adhesion (<xref ref-type="bibr" rid="B38">Xiao et al., 2020</xref>). Nevertheless, due to limited flow rates, the cutter head may still encounter clogging issues in cases of high adhesion strata or poorly designed cutter heads (<xref ref-type="bibr" rid="B42">Yang et al., 2023</xref>).</p>
<p>Shield clogging is primarily caused by the strong adhesive strength between metal and clay, also known as the clay-metal interface strength (<xref ref-type="bibr" rid="B27">Sass and Burbaum, 2009</xref>; <xref ref-type="bibr" rid="B34">Wang et al., 2020</xref>; <xref ref-type="bibr" rid="B18">Liu et al., 2022</xref>). The clay-metal interface strength can be divided into the normal direction perpendicular to the contact and the tangential direction along the interface (<xref ref-type="bibr" rid="B48">Zumsteg et al., 2013</xref>; <xref ref-type="bibr" rid="B4">Burbaum and Sass, 2017</xref>; <xref ref-type="bibr" rid="B16">Li et al., 2023</xref>). The cutting tool used in shield tunneling tears through the stratum, with the muck predominantly flowing tangentially along the cutter head. When the tangential strength, referred to as the shear strength of the clay-metal interface, is too high, it causes the flow of muck to halt and results in shield clogging. Therefore, the shear strength of the clay-metal interface is the primary factor contributing to shield clogging (<xref ref-type="bibr" rid="B49">Zumsteg and Puzrin, 2012</xref>; <xref ref-type="bibr" rid="B19">Liu et al., 2018</xref>; <xref ref-type="bibr" rid="B20">Liu et al., 2019</xref>). Several researchers have conducted relevant studies on the shear strength of the clay-metal interface. <xref ref-type="bibr" rid="B49">Zumsteg and Puzrin (2012)</xref> developed a rotating shear device to evaluate the shear strength between metal and clay in the interface. They investigated the impacts of metal surface roughness, water content, and applied pressure on the soil specimen. The findings demonstrated that an increase in surface roughness or normal pressure applied to the soil specimen led to a steady increase in the shear strength of the clay-metal interface. However, the shear strength dramatically decreased as the water content rose. <xref ref-type="bibr" rid="B2">Basmenj et al. (2016)</xref> used a direct shear apparatus and inserted the bottom half of the shear box into a metal block to test the shear strength of the clay-metal interface. They analyzed the variation in shear strength for soil specimens with different clay contents using the consistency index. The results showed that when the consistency index was low, the shear strength of the clay-metal interface remained relatively constant, but it increased rapidly when the consistency index surpassed a certain threshold. <xref ref-type="bibr" rid="B3">Bircha et al. (2016)</xref> investigated the relationship between water content, compactness, and the fluctuation of shear strength between sand, silt, clay, and metal. The study demonstrated that the shear strength of the clay-metal interface initially increased and subsequently decreased as the water content increased. Furthermore, the shear strength of the clay-metal interface decreased with the level of sand and silt compactness. <xref ref-type="bibr" rid="B35">Wang et al. (2022b)</xref> investigated the effects of the consistency index, normal pressure, clay plasticity, contact angle, and metal surface roughness on the shear strength of the clay-metal interface. They found that normal pressure, consistency index, and hydrophilicity of the metal surface significantly influenced the shear strength. In shield tunneling, the normal pressure is related to the tunnel face support pressure. Lower face support pressure reduces the likelihood of shield clogging but may lead to tunnel face collapse (<xref ref-type="bibr" rid="B5">Cao et al., 2020</xref>; <xref ref-type="bibr" rid="B37">Wang et al., 2022c</xref>; <xref ref-type="bibr" rid="B24">Niu et al., 2022</xref>). Therefore, simply decreasing the normal pressure is not a viable solution to avoid shield clogging. The natural water content and Atterberg limits of the soil in the stratum, which are challenging to modify, determine the consistency index. By applying an anti-adhesion substance to cover the cutter head and cutter, it is possible to reduce the hydrophilicity of the metal surface and prevent shield clogging. Preventing the formation of shield clogging can significantly improve shield tunneling construction efficiency and eliminate construction risks in cohesive strata. Coating technology is widely employed in various industries. For instance, in the medical field, anti-adhesion substances are coated on the surface of medical devices to reduce bacterial adhesion (<xref ref-type="bibr" rid="B41">Yang et al., 2022</xref>). In the glass manufacturing industry, anti-adhesion coatings are used to enhance the surface roughness of products by applying them to the mold surface (<xref ref-type="bibr" rid="B45">Zhang et al., 2020</xref>). Similarly, coatings are utilized to prevent corrosion in offshore wind power plants (<xref ref-type="bibr" rid="B8">Eom et al., 2020</xref>). However, there has been limited recent research specifically focusing on the application of anti-adhesion coatings to address shield clogging in tunnel engineering.</p>
<p>To investigate the impact of anti-adhesion coating on preventing shield clogging, this study conducted a comprehensive series of direct shear tests to measure the shear strength of the clay-metal interface under varying water contents. The analysis focused on examining the influence of the consistency index on the shear strength of the clay-metal interface and comparing the shear strength with and without the application of an anti-adhesion coating. The results confirmed the effectiveness of the anti-adhesion coating and provided further insights into its underlying mechanism.</p>
</sec>
<sec id="s2">
<title>2 Testing material and scheme</title>
<sec id="s2-1">
<title>2.1 Testing material</title>
<p>The soil sample used in this study was obtained from a construction site in Wuhan, China. <xref ref-type="table" rid="T1">Table 1</xref> presents the results of an X-ray diffraction (XRD) analysis conducted to identify the soil minerals. The analysis revealed the presence of albite, kaolinite, microcline, and small amounts of illite, montmorillonite, and calcite in the soil. The grain size distribution curve was determined using a laser particle size analyzer, as shown in <xref ref-type="fig" rid="F1">Figure 1</xref>. The largest particle size observed was 0.046&#xa0;mm. The Atterberg limits of the soil specimen were measured using the falling cone method in accordance with the Standards for Geotechnical Test Methods (2019). The liquid limit was determined to be 36.9%, while the plastic limit was found to be 18.9%. The plasticity index, calculated as the difference between the liquid and plastic limits, was 18.0. Since the plasticity index is greater than 17 and more than 50% of the specimen&#x2019;s mass consists of particles smaller than 0.075 mm, the soil specimen is classified as clay according to the <xref ref-type="bibr" rid="B30">USDA. (1938)</xref> classification.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Mineral composition of the soil specimen.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">Mineral name</th>
<th align="center">Mass percentage (%)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">Albite</td>
<td align="center">46.7</td>
</tr>
<tr>
<td align="center">Kaolinite</td>
<td align="center">27.8</td>
</tr>
<tr>
<td align="center">Microcline</td>
<td align="center">11.1</td>
</tr>
<tr>
<td align="center">Illite</td>
<td align="center">8.3</td>
</tr>
<tr>
<td align="center">Montmorillonite</td>
<td align="center">4.4</td>
</tr>
<tr>
<td align="center">Calcite</td>
<td align="center">1.6</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Soil gradation curve.</p>
</caption>
<graphic xlink:href="feart-11-1216614-g001.tif"/>
</fig>
</sec>
<sec id="s2-2">
<title>2.2 Large-scale direct shear test</title>
<p>Several instruments are used to measure the shear strength of the clay-metal interface, including the soil-metal adapter, static lateral adhesion apparatus, shear plate apparatus, and direct shear apparatus (<xref ref-type="bibr" rid="B49">Zumsteg and Puzrin, 2012</xref>; <xref ref-type="bibr" rid="B25">Peila et al., 2015</xref>; <xref ref-type="bibr" rid="B2">Basmenj et al., 2016</xref>; <xref ref-type="bibr" rid="B3">Bircha et al., 2016</xref>). However, there are limitations associated with some of these instruments. For instance, in the static lateral adhesion and soil-metal adapter tests, it is not possible to apply normal pressure on the soil specimen. Additionally, the shear stress on the plate is assumed to be equal, which is clearly unreasonable in the shear plate test. To overcome these limitations, the shear strength of the clay-metal interface was evaluated using a large-scale direct shear apparatus (<xref ref-type="fig" rid="F2">Figure 2</xref>). The testing methodology aligns with that of a typical direct shear device. The direct shear box has dimensions of 15&#xa0;cm in length and 15&#xa0;cm in width, with the top and bottom halves of the box each measuring 7.5&#xa0;cm in height. The soil specimen is placed in the upper section of the box, while the metal block is placed in the lower section. By applying normal pressure to the specimen, the shear strength of the clay-metal interface can be determined.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Large-scale direct shear apparatus.</p>
</caption>
<graphic xlink:href="feart-11-1216614-g002.tif"/>
</fig>
<p>The metal block was cleaned using alcohol, and after natural drying, an anti-adhesion substance was applied. The metal block was once again dried after spraying the anti-adhesion agent. The hydrophilicity of the metal surface, as indicated by the contact angle, is a key factor influencing the shear strength of the clay-metal interface. The contact angle of water on a solid surface reflects the hydrophilicity of that material. A decrease in the contact angle signifies increased hydrophilicity of the solid material. The water contact angles observed on the coated and untreated metal blocks were 85.48&#xb0; and 62.04&#xb0;, respectively.</p>
<p>The large-scale direct shear test involved the following major steps:<list list-type="simple">
<list-item>
<p>(1) The soil samples were dried at 105&#xb0;C for a minimum of 24&#xa0;h. Any agglomerated soil was broken using a rubber hammer, ensuring that the soil particles were not damaged. To achieve the desired water content, the dry soil specimen weighing 3&#xa0;kg was mixed with water and left undisturbed for 24&#xa0;h to allow complete water absorption.</p>
</list-item>
<list-item>
<p>(2) The lower portion of the direct shear box was filled with the metal block. The upper and lower halves of the box were aligned and securely fixed using clamping screws. The prepared soil specimen was then placed layer by layer in the upper portion of the box until its surface was approximately 1&#xa0;cm below the top of the box.</p>
</list-item>
<list-item>
<p>(3) The specimen was covered with filter paper and a loading plate. The required normal pressure was applied to the specimen. In this study, the fast shear test, which is an undrained and unconsolidated shear test, was conducted to simulate the release of muck during shield tunneling without drainage and consolidation.</p>
</list-item>
<list-item>
<p>(4) After applying the necessary pressure, the clamping screws were removed, and the shear test was initiated. The shear stress and displacement were monitored at a frequency of 1 time per second, and the shear rate was set to 1&#xa0;mm/min, following the Standards for Geotechnical Test Methods.</p>
</list-item>
<list-item>
<p>(5) The measured data were recorded and analyzed after the completion of the shearing process. The actual water content of the soil sample next to the metal block was also measured.</p>
</list-item>
</list>
</p>
<p>A series of extensive direct shear tests were conducted under various normal pressures to investigate the effect of the anti-adhesion coating on the prevention of shield clogging, as presented in <xref ref-type="table" rid="T2">Table 2</xref>.</p>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Large-scale direct shear test conditions.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">Anti-adhesion coating</th>
<th align="center">Normal pressure values (kPa)</th>
<th align="center">Water content range (%)</th>
<th align="center">Consistency index (I<sub>c</sub>)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td rowspan="2" align="center">Uncoated</td>
<td align="center">100</td>
<td rowspan="4" align="center">10&#x2013;30</td>
<td rowspan="4" align="center">0.3&#x2013;1.6</td>
</tr>
<tr>
<td align="center">200</td>
</tr>
<tr>
<td rowspan="2" align="center">Coated</td>
<td align="center">300</td>
</tr>
<tr>
<td align="center">400</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</sec>
<sec id="s3">
<title>3 Results of the direct shear test</title>
<sec id="s3-1">
<title>3.1 Shearing curve</title>
<p>
<xref ref-type="fig" rid="F3">Figure 3</xref> illustrates the shearing curves of soil sample with 10% water content obtained from the direct shear testing. Initially, as the shear displacement increased, there was a significant rise in shear stress at the metal-clay interface. As the shear displacement approached the point where the contact between clay and metal was disrupted, the shear stress increased gradually. Finally, the shear stress then reached a relatively constant level. When the difference between five consecutive readings is less than 0.5&#xa0;kPa, it is considered that the shear stress has reached a stable state. The average shear stress during this stable stage was considered to represent the shear strength of the clay-metal interface.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Shearing curves between uncoated metal block and clay with 10% water content.</p>
</caption>
<graphic xlink:href="feart-11-1216614-g003.tif"/>
</fig>
</sec>
<sec id="s3-2">
<title>3.2 Variations in the shear strength of the clay-metal interface with the consistency index at different pressures</title>
<p>Due to the variation in Atterberg limits among different clay types with the same water content, they exhibit different degrees of softness. The consistency index (I<sub>c</sub>) takes into account the water content and Atterberg limits of the clay. When the water content is at the liquid limit, the consistency index is 0, whereas it is 1 at the plastic limit. For values between the liquid and plastic limits, the consistency index represents the corresponding degree of softness, ranging from 0 to 1. Thus, the consistency index, as represented by Eq. <xref ref-type="disp-formula" rid="e1">1</xref>, is a normalized value that characterizes the softness state of clay.<disp-formula id="e1">
<mml:math id="m1">
<mml:mrow>
<mml:msub>
<mml:mi>I</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>w</mml:mi>
<mml:mi>l</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>w</mml:mi>
</mml:mrow>
<mml:msub>
<mml:mi>I</mml:mi>
<mml:mi mathvariant="normal">p</mml:mi>
</mml:msub>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>
</p>
<p>
<xref ref-type="fig" rid="F4">Figure 4</xref> illustrates the variation of shear strength of the clay-metal interface with the consistency index, obtained by converting the water content into the consistency index. Each data point represents the average of two experimental results. When the consistency index was below 0.6, the shear strength of the clay-metal interface was very low. A slight increase in shear strength was observed as the consistency index increased. Notably, a significant increase in shear strength occurred within the consistency index range of 0.6&#x2013;1.2. Once the consistency index exceeded 1.2, the shear strength of the clay-metal interface showed minimal variations. Additionally, when the consistency index was below 0.6, there was minimal variation in the shear strength of the clay-metal interface at different normal pressures. However, for consistency indexes above 0.6, the shear strength exhibited a significant increase with increasing normal pressure.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Variations in the shear strength between uncoated metal block and clay with the consistency index.</p>
</caption>
<graphic xlink:href="feart-11-1216614-g004.tif"/>
</fig>
</sec>
<sec id="s3-3">
<title>3.3 Effect of anti-adhesion coating on the shear strength of the clay-metal interface</title>
<p>
<xref ref-type="fig" rid="F5">Figure 5</xref> compares the shear strength between coated and uncoated metal blocks and clay at normal pressures of 100, 200, 300, and 400&#xa0;kPa. The shear strength between the coated metal block and clay exhibited a similar trend to the shear strength between the uncoated metal block and clay, varying with the consistency index. However, the shear strength between the coated metal block and clay was weaker compared to the uncoated metal block under the same consistency index and standard pressure. Furthermore, the difference in shear strength increased as the shear strength of the clay-metal interface increased. The high shear strength of the clay-metal interface, such as the cutter head and cutter, was identified as the primary factor causing shield clogging. The test results showed that the anti-adhesion coating significantly reduced the shear strength of the clay-metal interface. Consequently, the application of an anti-adhesion coating can effectively reduce the likelihood of shield clogging in the adhesive stratum.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Comparison of shear strength between coated or uncoated metal block and clay under normal pressure of <bold>(A)</bold> 100, <bold>(B)</bold> 200, <bold>(C)</bold> 300, and <bold>(D)</bold> 400&#xa0;kPa.</p>
</caption>
<graphic xlink:href="feart-11-1216614-g005.tif"/>
</fig>
</sec>
</sec>
<sec id="s4">
<title>4 Discussion on the mechanism of anti-adhesion coating</title>
<p>A water film theory for soil adhesion was proposed by <xref ref-type="bibr" rid="B1">Akiyama and Yokoi. (1972)</xref>. In this theory, the interaction between clay and the metal block was modeled as a plate-water-plate interface, considering the lamellar structure of clay particles (<xref ref-type="bibr" rid="B26">Ren et al., 1990</xref>). This conceptualization is illustrated in <xref ref-type="fig" rid="F6">Figure 6</xref>. The normal force acting on the clay-metal interface is calculated using the Laplace <xref ref-type="disp-formula" rid="e2">formula (2)</xref>, which can be expressed as follows (<xref ref-type="bibr" rid="B12">Huang et al., 2013</xref>):<disp-formula id="e2">
<mml:math id="m2">
<mml:mrow>
<mml:mi>W</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mi>&#x3c0;</mml:mi>
<mml:msup>
<mml:mi>R</mml:mi>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:msub>
<mml:mi>&#x3b3;</mml:mi>
<mml:mi>L</mml:mi>
</mml:msub>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>cos</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:msub>
<mml:mi>&#x3b8;</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>cos</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:msub>
<mml:mi>&#x3b8;</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
<mml:mi>h</mml:mi>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(2)</label>
</disp-formula>where <italic>h</italic> and <italic>R</italic> stand for the thickness and radius of the water film, respectively, &#x3b8;<sub>1</sub> and &#x3b8;<sub>2</sub> for the metal block and clay&#x2019;s respective contact angles, and &#x3b3;<sub>L</sub> for the water&#x2019;s surface tension. Thus, the following is the tangential force on the clay-metal interface:<disp-formula id="e3">
<mml:math id="m3">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>&#x3bc;</mml:mi>
<mml:mi>W</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mi>&#x3bc;</mml:mi>
<mml:mi>&#x3c0;</mml:mi>
<mml:msup>
<mml:mi>R</mml:mi>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:msub>
<mml:mi>&#x3b3;</mml:mi>
<mml:mi>L</mml:mi>
</mml:msub>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>cos</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:msub>
<mml:mi>&#x3b8;</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>cos</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:msub>
<mml:mi>&#x3b8;</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
<mml:mi>h</mml:mi>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(3)</label>
</disp-formula>where the coefficient of friction between the clay and the metal is denoted by &#x3bc;. According to Eq. <xref ref-type="disp-formula" rid="e3">3</xref>, the shear strength of the clay-metal interface is inversely proportional to the thickness of the water film (h) and directly proportional to the area of the water film (&#x3c0;R<sup>2</sup>). <xref ref-type="bibr" rid="B44">Zhang et al. (2004)</xref> reported that as the water content of clay increases from zero to the liquid limit, the water film at the clay-metal interface undergoes three stages: slow increase, rapid growth, and saturation. With an increase in water content or a decrease in consistency, the water film between the clay and metal interface gradually enlarges, leading to an increase in the water film area. Consequently, the shear strength of the clay-metal interface gradually increases during the first stage. When the water content reaches a certain level, the clay-metal interface becomes completely covered by water, and the water film area typically saturates during the second stage. The water film thickness rapidly increases, causing a rapid decrease in the shear strength of the clay-metal interface. In the third stage, the water film thickness at the clay-metal interface approaches saturation, resulting in a gradual decrease in the shear strength as the water content increases. Therefore, as the water content increases or the consistency index decreases, the shear strength of the clay-metal interface initially increases gradually, then decreases rapidly, and finally decreases slowly (<xref ref-type="fig" rid="F4">Figure 4</xref>). The consistency index and normal pressure are factors that influence the area and thickness of the water film. Under the same normal pressure and consistency index, it can be assumed that the area and thickness of the water film between the clay and metal blocks are similar. In this case, the shear strength of the clay-metal interface is determined by the contact angle (&#x3b8;<sub>1</sub>) of the metal block. The uncoated and coated metal block surfaces have contact angles of 62.04&#xb0; and 85.48&#xb0;, respectively. The coated metal block surface has a higher contact angle than the uncoated metal block. However, as the contact angle &#x3b8;<sub>1</sub> increases, the value of cos&#x3b8;<sub>1</sub> decreases. Consequently, the adhesion between the coated metal block and clay has a lower strength compared to the uncoated metal block (<xref ref-type="fig" rid="F5">Figure 5</xref>).</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>Plate-water-plate model.</p>
</caption>
<graphic xlink:href="feart-11-1216614-g006.tif"/>
</fig>
</sec>
<sec sec-type="conclusion" id="s5">
<title>5 Conclusion</title>
<p>The shear strength of the clay-metal interface was investigated in relation to the consistency index using the large-scale direct shear test. A comparison was made between the shear strength of the clay-metal interface with coated and uncoated metal blocks. Furthermore, the mechanism of the anti-adhesion coating was further discussed. The main conclusions of the study are as follows:<list list-type="simple">
<list-item>
<p>(1) With an increase in shear displacement, the shear stress between the clay and metal blocks increased rapidly. However, it tended to stabilize after reaching a certain shear displacement magnitude.</p>
</list-item>
<list-item>
<p>(2) As the consistency index increased, the shear strength of the clay-metal interface exhibited a gradual increase, followed by a significant increase, and eventually approached a stabilized state. When the consistency index was less than 0.6, the shear strength of the clay-metal interface was relatively consistent under various normal pressures. However, for consistency indexes higher than 0.6, the shear strength of the clay-metal interface varied significantly under different normal pressures.</p>
</list-item>
<list-item>
<p>(3) The application of the anti-adhesion coating resulted in a decrease in the hydrophilicity of the metal block surface and an increase in the contact angle. Consequently, under the same normal pressure and consistency index, the shear strength between the coated metal block and clay was lower compared to that between the uncoated metal block and clay. This suggests that the anti-adhesion coating has the potential to reduce the occurrence of shield clogging in the adhesive stratum.</p>
</list-item>
</list>
</p>
<p>This study introduces a novel approach to prevent shield clogging, which involves applying anti-sticking coatings on the surface of the cutter and cutting tools. However, the current research is limited to laboratory experiments, and the specific effectiveness needs further validation through field testing. Other properties of the coatings, such as wear resistance and high-temperature durability, also require further investigation.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="s6">
<title>Data availability statement</title>
<p>The original contributions presented in the study are included in the article/supplementary material, further inquiries can be directed to the corresponding author.</p>
</sec>
<sec id="s7">
<title>Author contributions</title>
<p>PL: conceptualization, methodology, investigation, funding acquisition, and formal analysis; SS: resources and supervision; ZY: investigation and writing&#x2013;original draft; FJ: software, data curation, and writing&#x2013;review and editing; CX: software; supervision; HZ: validation. All authors contributed to the article and approved the submitted version.</p>
</sec>
<sec id="s8">
<title>Funding</title>
<p>The financial support from the China Postdoctoral Science Foundation (Grant No. 2022M723536) are acknowledged and appreciated.</p>
</sec>
<sec sec-type="COI-statement" id="s9">
<title>Conflict of interest</title>
<p>Authors PL, ZY, JF, and CX were by the CCCC Second Harbor Engineering Company Ltd. Author SS was employed by the CCCC First Harbor Engineering Company Ltd.</p>
<p>The remaining author declares 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>
<p>The reviewer CZ declared a shared affiliation with the author HZ to the handling editor at the time of review.</p>
</sec>
<sec sec-type="disclaimer" id="s10">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
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