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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mater.</journal-id>
<journal-title>Frontiers in Materials</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mater.</abbrev-journal-title>
<issn pub-type="epub">2296-8016</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">1513872</article-id>
<article-id pub-id-type="doi">10.3389/fmats.2024.1513872</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Materials</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Study on acoustic emission characteristics under compression and fractal dimension of pore structure of polyvinyl alcohol fiber engineered cementitious composites</article-title>
<alt-title alt-title-type="left-running-head">Li 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/fmats.2024.1513872">10.3389/fmats.2024.1513872</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Li</surname>
<given-names>Yueqiang</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/2867488/overview"/>
<role content-type="https://credit.niso.org/contributor-roles/conceptualization/"/>
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<role content-type="https://credit.niso.org/contributor-roles/methodology/"/>
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<role content-type="https://credit.niso.org/contributor-roles/visualization/"/>
<role content-type="https://credit.niso.org/contributor-roles/writing-original-draft/"/>
<role content-type="https://credit.niso.org/contributor-roles/Writing - review &#x26; editing/"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Huang</surname>
<given-names>Xin</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<role content-type="https://credit.niso.org/contributor-roles/formal-analysis/"/>
<role content-type="https://credit.niso.org/contributor-roles/project-administration/"/>
<role content-type="https://credit.niso.org/contributor-roles/validation/"/>
<role content-type="https://credit.niso.org/contributor-roles/Writing - review &#x26; editing/"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Zhao</surname>
<given-names>Yangcan</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<role content-type="https://credit.niso.org/contributor-roles/data-curation/"/>
<role content-type="https://credit.niso.org/contributor-roles/investigation/"/>
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<role content-type="https://credit.niso.org/contributor-roles/Writing - review &#x26; editing/"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Qiao</surname>
<given-names>Yanyang</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
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<aff id="aff1">
<sup>1</sup>
<institution>School of Civil Engineering, Institute of Disaster Prevention</institution>, <addr-line>Sanhe</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Hebei Technology Innovation Center for Multi-Hazard Resilience and Emergency Handling of Engineering Structures, Institute of Disaster Prevention</institution>, <addr-line>Sanhe</addr-line>, <country>China</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>School of Geological Engineering, Institute of Disaster Prevention</institution>, <addr-line>Sanhe</addr-line>, <country>China</country>
</aff>
<aff id="aff4">
<sup>4</sup>
<institution>School of Mechanics and Civil Engineering, China University of Mining and Technology</institution>, <addr-line>Beijing</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/205849/overview">Jialai Wang</ext-link>, University of Alabama, United States</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/1079905/overview">Pavlo Maruschak</ext-link>, Ternopil Ivan Pului National Technical University, Ukraine</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1316952/overview">Chuanqing Fu</ext-link>, Zhejiang University of Technology, China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Xin Huang, <email>154273083@qq.com</email>
</corresp>
</author-notes>
<pub-date pub-type="epub">
<day>20</day>
<month>12</month>
<year>2024</year>
</pub-date>
<pub-date pub-type="collection">
<year>2024</year>
</pub-date>
<volume>11</volume>
<elocation-id>1513872</elocation-id>
<history>
<date date-type="received">
<day>19</day>
<month>10</month>
<year>2024</year>
</date>
<date date-type="accepted">
<day>03</day>
<month>12</month>
<year>2024</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2024 Li, Huang, Zhao and Qiao.</copyright-statement>
<copyright-year>2024</copyright-year>
<copyright-holder>Li, Huang, Zhao and Qiao</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>Fiber adding to engineered cementitious composites (ECC) can effectively improve the performance of material. This study used the acoustic emission (AE) technique to study the influence of polyvinyl alcohol (PVA) fibre content on compressive strength and damage evolution of ECC and used the fractal theory to analyse the pore structure of PVA-ECC, which innovatively explored the mechanical properties and durability of PVA-ECC from macro and micro perspectives. In terms of mechanical properties, the compressive strength of ECC with 1% PVA volume content was the highest. PVA changed the compression damage mechanism of ECC, showing a decrease in internal tensile cracking and an increase in shear cracking through RA-AF values. ECC developed from brittle damage to ductile damage. In terms of microstructure and durability, ECC with 1% PVA volume content had the best impermeability and pore structure fractal characteristics, and PVA had a great influence on the fractal characteristics of transition pores and capillary pores. The fractal dimension had a good correlation with porosity, total pore volume, most probable aperture, compressive strength and chloride diffusion coefficient, indicating that the mechanical strength and impermeability of ECC were closely related to the complex spatial structure and distribution characteristics of pores. The fractal dimension can be used to comprehensively characterise the mechanical properties and durability of ECC.</p>
</abstract>
<kwd-group>
<kwd>polyvinyl alcohol fiber</kwd>
<kwd>ringing counts</kwd>
<kwd>RA-AF</kwd>
<kwd>pore structure</kwd>
<kwd>fractal dimension</kwd>
</kwd-group>
<contract-sponsor id="cn001">Langfang Municipal Science and Technology Bureau<named-content content-type="fundref-id">10.13039/501100010106</named-content>
</contract-sponsor>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-at-acceptance</meta-name>
<meta-value>Structural Materials</meta-value>
</custom-meta>
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</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>Cementitious materials remain important civil engineering materials in modern construction. The high strength, ductility, and durability of these materials can ensure the safety and stability of structures (<xref ref-type="bibr" rid="B29">Sun, et al., 2023</xref>; <xref ref-type="bibr" rid="B37">Yang, et al., 2024</xref>). Ordinary cementitious materials are brittle (<xref ref-type="bibr" rid="B24">Rajput and Iqbal, 2017</xref>; <xref ref-type="bibr" rid="B31">Wagh, et al., 2024</xref>). Currently, various fiber materials incorporating can improve the mechanical properties of cementitious materials to some extent, such as steel fiber, polypropylene fiber, PVA fibers, basalt fibers, etc., (<xref ref-type="bibr" rid="B13">Li B. et al., 2023</xref>; <xref ref-type="bibr" rid="B45">Zhao, et al., 2024</xref>). <xref ref-type="bibr" rid="B23">Rahmani et al. (2012)</xref> studied the effect of cellulose, polypropylene and steel fibers on the impact resistance of cementitious materials, with the addition of steel fibers having the most significant effect of increasing the average number of failure blows by 375%. <xref ref-type="bibr" rid="B14">Li J. Y. et al. (2023)</xref> tested the tensile and compressive properties of polypropylene fiber concrete at room temperature and after high temperatures. When fiber content is low, polypropylene fibers significantly improve the mechanical properties of concrete after high temperature. However, with the increase of fiber content, compressive strength after high temperature shows a tendency to increase first and then decrease at the same temperature. <xref ref-type="bibr" rid="B26">Shen et al. (2024)</xref> used SHPB equipment to conduct mechanical property experiments on steel-polypropylene fiber-reinforced concrete after high temperatures. It is found that the dynamic compressive strength of hybrid fiber concrete with optimum admixture increases by 97.1% compared to C40 plain concrete at 800&#xb0;C temperature group.</p>
<p>PVA fibers are advantageous for practical engineering applications due to their high toughness, good affinity with cementitious materials and low production cost (<xref ref-type="bibr" rid="B30">Sundar et al., 2017</xref>; <xref ref-type="bibr" rid="B43">Zhang et al., 2024</xref>). PVA-ECC is a polymer composite material. <xref ref-type="bibr" rid="B28">Stukhlyak et al. (2015)</xref> proposed a multi-scale analysis method for composite materials and believed that the self-organizing system of materials and the interaction between different deformation scales are factors that cannot be ignored in evaluating material properties. Therefore, for polymer composites, the deformation and crack characteristics are analyzed from macro-scale, meso-scale and micro-scale. The initiation of initial crack is controlled by the micro-scale mechanism, and the propagation of crack is defined by the macro-scale fracture mechanism. In the study of macroscopic mechanical properties of PVA-ECC, <xref ref-type="bibr" rid="B41">Zhang et al. (2019)</xref> concluded that PVA fibers can improve the impact resistance and tensile properties of cementitious materials through drop-weight tests and uniaxial tensile tests. <xref ref-type="bibr" rid="B7">Farhan and Jagdish (2021)</xref> replaced cement with fly ash and iron slag, and used PVA fiber as an additive with contents of 0%, 2%, and 3%. Compared with the concrete without PVA fibers, the compressive strength, flexural strength, and split tensile strength of the concrete containing PVA fibers are improved, and the mechanical property indexes are optimal when the additives are 3%. <xref ref-type="bibr" rid="B35">Wu et al. (2024)</xref> analyzed the effect of steel-PVA hybrid fibers on the flexural properties of slab concrete by three-point bending test, the development of cracks in concrete by using DIC technique and SEM experiments, and the evolution of cracks based on fractal theory quantitatively. It is concluded that the steel-PVA hybrid fibers increase the proportional ultimate strength and residual flexural strength of the concrete. The presence of PVA fibers further reduce the rate of crack development and crack area compared to steel fiber reinforced concrete. The best flexural properties of concrete are achieved when the steel fiber content is 1.0% and PVA fiber content is 0.2%.</p>
<p>In the study of micro crack propagation and damage evolution of PVA-ECC, AE technology is widely used in experimental studies of concrete. AE signals can quantitatively or qualitatively analyze the pressure damage process and damage evolution of materials (<xref ref-type="bibr" rid="B17">Lockner, 1993</xref>; <xref ref-type="bibr" rid="B22">Nair and Cai, 2010</xref>; <xref ref-type="bibr" rid="B1">Bi et al., 2020</xref>; <xref ref-type="bibr" rid="B42">Zhang and Li, 2020</xref>; <xref ref-type="bibr" rid="B21">Lyu, et al., 2024</xref>). <xref ref-type="bibr" rid="B9">Huang et al. (2019)</xref> have analyzed the compression damage characteristics of PVA fiber concrete after high temperature using acoustic emission technology. The results showed that the fibres resulted in a wider distribution of energy count rates in the specimens, with relatively small peak energy count rates, and it was concluded that PVA fibres could improve the high temperature resistance of the concrete by comparing it with the reference concrete. <xref ref-type="bibr" rid="B3">Chen et al. (2022)</xref> implemented preloading of concrete with and without added cementitious materials at different ages with different strengths, and studied the law of the effect of early damage on long-term strength of concrete based on the AE technique. It was found that the pozzolanic effect of cementitious materials and hydrates produced C-S-H gels to fill the pores and repair the early damage caused by preloading. The addition of cementitious materials resulted in higher compressive strength of 270 days age specimens than ordinary concrete. <xref ref-type="bibr" rid="B4">Chen et al. (2023)</xref> classified and localized cracks in corroded concrete columns under eccentric loading by the AE technique, and proposed a simple four-step method of crack identification based on the results of GMM calculations, which provided a quantitative analysis of the proportion of tensile and shear cracks in compressive damage.</p>
<p>In the study of microporous structure of PVA-ECC, <xref ref-type="bibr" rid="B2">Chen et al. (2021)</xref> measured the effective chloride diffusion coefficients of cement mortars at different water-cement ratios. It was found that higher water-cement ratios led to a porous structure, which increased the chloride diffusion coefficient in cement mortar. <xref ref-type="bibr" rid="B8">He et al. (2023)</xref> found that the dielectric constant can characterize water-cement ratio of plastic concrete, while water-cement ratio affects the microporous structure of concrete. The changes in pore structure of material have impact on mechanical properties, durability, etc (<xref ref-type="bibr" rid="B6">Fan et al., 2022</xref>). With the development of high-performance concrete and indepth study of the pore structure of the material, traditional pore structure parameters, such as porosity, pore volume and pore size distribution are unable to quantitatively characterise the complexity of the pores. Scholars have established a variety of fractal models of concrete pore structure to describe the complexity of pore structure in terms of the size of fractal dimension, and the relationship between microscopic pore structure and macroscopic mechanical properties has been established through the fractal dimension. <xref ref-type="bibr" rid="B16">Liu et al. (2023)</xref> determined the compressive strength and pore structure parameters of steel-PVA hybrid fibre concrete with different dosage, and calculated the fractal dimension under different pore size distributions based on the thermodynamic fractal model. The article concluded that the fractal dimension was consistent with the change rule of compressive strength affected by the fibres, and the fractal dimension of gel pores and capillary pores varied greatly. <xref ref-type="bibr" rid="B15">Li et al. (2024)</xref> concluded that the pore structure of steel fibre ground polymer recycled concrete had significant fractal characteristics. The fractal dimension was negatively correlated with porosity and most probable aperture, positively correlated with curvature coefficient, and positively correlated with cubic compressive strength, split tensile strength and flexural strength. <xref ref-type="bibr" rid="B44">Zhao J. et al. (2023)</xref> calculated the fractal dimension of pore structure of basalt-polypropylene fibre concrete based on optical method, and found that fractal dimension had a strong correlation with porosity, spacing coefficient, compressive strength, and splitting tensile strength. The fractal dimension can reflect the complexity of material pore structure and the influence of pore structure on mechanical properties. <xref ref-type="bibr" rid="B11">Jin et al. (2017)</xref>, <xref ref-type="bibr" rid="B38">Zarnaghi et al. (2018)</xref>, and <xref ref-type="bibr" rid="B20">Lv et al. (2019)</xref> found a linear relationship between the fractal dimension and strength of concrete.</p>
<p>Most current research of PVA-ECC focuses on the effects of fiber content on mechanical properties, such as compressive, flexural, tensile, and macroscopic damage characteristics. However, fewer studies investigate the stages of internal crack development and pore structure characteristics under different PVA contents. Based on the AE technology, this paper investigated the characteristic parameters of AE and the development of tensile cracks and shear cracks in specimens with different PVA content, and analysed the influence of PVA on the uniaxial compression damage characteristics of ECC. The pore structure parameters and chloride diffusion coefficient were obtained through mercury intrusion porosimetry (MIP) tests and chloride penetration tests, and the influence of PVA fibre on the fractal characteristics of pore structure was analysed based on fractal theory. The correlations between fractal dimensions and mechanical parameters, pore structure parameters, and chloride diffusion coefficient were also analysed. This study aims to provide a theoretical basis for the application of PVA fibers in ECC from micro and macro perspective.</p>
</sec>
<sec id="s2">
<title>2 Test</title>
<sec id="s2-1">
<title>2.1 Test materials</title>
<p>In these tests, the cements are sulfoaluminate double fast cement of strength 42.5. Fly ash is the first grade low calcium fly ash with the specific surface area of 420 m<sup>2</sup>/kg. Silica ash has a specific surface area of 2000 m<sup>2</sup>/kg. Fine quartz sand specification are 100&#x2013;200 mesh, which came from Anhui Fengyang County Shengli Quartz Sand Factory. High-efficiency polycarboxylic acid water reducing agents were produced by Zhengzhou Xinghui Chemical Raw Material Company, while retarders from Shandong Zhongda New Material Company and dilatants from CNBM Zhongyan Technology Co, as shown in <xref ref-type="table" rid="T1">Table 1</xref>. PVA fibers were produced at the Shangwanwei raw material plant. The PVA parameters are shown in <xref ref-type="table" rid="T2">Table 2</xref>.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Chemical composition of material (%).</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">Index</th>
<th align="center">Loss on ignition</th>
<th align="center">SiO<sub>2</sub>
</th>
<th align="center">Al<sub>2</sub>O<sub>3</sub>
</th>
<th align="center">Fe<sub>2</sub>O<sub>3</sub>
</th>
<th align="center">CaO</th>
<th align="center">MgO</th>
<th align="center">TiO<sub>2</sub>
</th>
<th align="center">K<sub>2</sub>O</th>
<th align="center">Na<sub>2</sub>O</th>
<th align="center">SO<sub>3</sub>
</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">cement</td>
<td align="center">4.48</td>
<td align="center">8.21</td>
<td align="center">23.28</td>
<td align="center">2.02</td>
<td align="center">41.91</td>
<td align="center">2.98</td>
<td align="center">1.28</td>
<td align="center">0.42</td>
<td align="center">0.21</td>
<td align="center">12.87</td>
</tr>
<tr>
<td align="center">fly ash</td>
<td align="center">1.05</td>
<td align="center">52.94</td>
<td align="center">34.86</td>
<td align="center">2.52</td>
<td align="center">2.63</td>
<td align="center">0.77</td>
<td align="center">1.25</td>
<td align="center">1.76</td>
<td align="center">0.47</td>
<td align="center">0.31</td>
</tr>
<tr>
<td align="center">silica ash</td>
<td align="center">2.43</td>
<td align="center">92.82</td>
<td align="center">0.21</td>
<td align="center">0.23</td>
<td align="center">0.49</td>
<td align="center">0.95</td>
<td align="center">-</td>
<td align="center">0.86</td>
<td align="center">0.67</td>
<td align="center">-</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Related parameters of PVA fibers.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">Material</th>
<th align="center">Density/(g/cm<sup>3</sup>)</th>
<th align="center">Tensile strength/(MPa)</th>
<th align="center">Elastic modulus/(Gpa)</th>
<th align="center">Diameter/(mm)</th>
<th align="center">Length/(mm)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">PVA fibers</td>
<td align="center">1.29</td>
<td align="center">1830</td>
<td align="center">40</td>
<td align="center">0.100</td>
<td align="center">12</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The PVA-ECC substrate formulation is shown in <xref ref-type="table" rid="T3">Table 3</xref>. PVA fibers are added in volume fractions of 0%, 0.5%, 1.0%, 1.5%, and 2.0%, corresponding to specimen numbers P0, P0.5, P1, P1.5, P2, as shown in <xref ref-type="table" rid="T4">Table 4</xref>.</p>
<table-wrap id="T3" position="float">
<label>TABLE 3</label>
<caption>
<p>Mix ratio of base materials.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">Cement</th>
<th align="center">Fly ash</th>
<th align="center">Silica ash</th>
<th align="center">Quartz sand</th>
<th align="center">Water reducing agent</th>
<th align="center">Retarder</th>
<th align="center">Dilatant</th>
<th align="center">Water</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">0.65</td>
<td align="center">0.20</td>
<td align="center">0.05</td>
<td align="center">0.20</td>
<td align="center">0.0150</td>
<td align="center">0.005</td>
<td align="center">0.03</td>
<td align="center">0.35</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="T4" position="float">
<label>TABLE 4</label>
<caption>
<p>PVA fiber content and number.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">Fiber volume fraction/%</th>
<th align="center">0</th>
<th align="center">0.5</th>
<th align="center">1</th>
<th align="center">1.5</th>
<th align="center">2</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">Number</td>
<td align="center">P0</td>
<td align="center">P0.5</td>
<td align="center">P1</td>
<td align="center">P1.5</td>
<td align="center">P2</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s2-2">
<title>2.2 Specimens preparation</title>
<p>There are two specimen standards for this test, as shown in <xref ref-type="fig" rid="F1">Figure 1</xref>. One is a cube with a size of 100 mm &#xd7; 100 mm &#xd7;100 mm, which is used for uniaxial compression tests and AE tests. There are 3 groups of P0-P2, a total of 15 groups of specimens. The other is a flat cylinder with a diameter of 100 mm and a thickness of 50 mm P0-P2 are 4 groups, a total of 20 groups of specimens. Three groups were used for chloride penetration tests, and one group was used for MIP tests.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Three-dimensional dimensioned sample of the specimens. <bold>(A)</bold>Cubic specimen <bold>(B)</bold>Flat cylinder specimen.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g001.tif"/>
</fig>
<p>Firstly, dry materials such as cement, fly ash, silica ash, quartz sand, expansion agent, etc.,. were put into the mixer for stirring for 1.5 min, and the dry materials were stirred evenly. Subsequently, water was poured into the mixer in batches, and PVA fibers were gradually poured evenly. Water reducing agents were poured according to the wetting degree of materials in mixer. After all the materials were stirred evenly, the mixer was closed, and the stirred cement paste was put out for use.</p>
<p>Pour half of the cement paste into mold, then put it on the vibration table, open the vibration table to discharge air in cement paste, and then pour the other half of the cement paste into mold. Repeat above vibration process to make the cement paste more even. Finally, the cement paste was wrapped with preservative film together with the mold. The purpose was to allow the cement paste to continue hydration heat reaction in curing film, thereby effectively inhibiting the generation of microcracks. These were placed in the standard curing room with indoor temperature of 20&#xb0;C &#xb1; 2&#xb0;C, humidity of 95%, and curing for 28 days.</p>
<p>After standard curing, the specimens were polished to make the surface smooth and flat. The six surfaces of cube specimens and the upper and lower surfaces of flat cylinders were polished using 20 mesh coarse sandpaper.</p>
</sec>
<sec id="s2-3">
<title>2.3 Test methods and equipments</title>
<sec id="s2-3-1">
<title>2.3.1 Uniaxial compression and acoustic emission test</title>
<p>For the static loading device, we adopted a micro-controlled electro-hydraulic servo rigidity test press, capable of a maximum test force of 2t and an internal piston range of 100 mm. The strain gauges with a width of 3 mm were selected, and two opposite sides were selected from four sides of the specimen. Floating ash on the surface was erased, and strain gauges were pasted on two opposite sides of the specimen in a positive T and inverted T fashion.</p>
<p>The multi-channel acoustic emission detection system was produced by American Physical Acoustics Company, as shown in <xref ref-type="fig" rid="F2">Figure 2</xref>. Experimental acoustic signals were set to a thresh-old value of 40 dB. Add 2/4/6-AST amplifier. The function was to expand the signals collected by sensor and then transmit it to host computer, which made the test results more accurate. Ring sensor fixtures were specially made. Before the test, ring fixtures were fixed on the surface of specimen with glue. During the test, sensor probe was smeared with coupling agent such as vaseline and then put into the fixture. It can ensure that the probe is fixed, in good contact with cementitious specimen, and not damaged.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Schematic diagram of uniaxial compression and acoustic emission test.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g002.tif"/>
</fig>
</sec>
<sec id="s2-3-2">
<title>2.3.2 Chlorine penetration test</title>
<p>The tests were conducted using NEL method proposed by <xref ref-type="bibr" rid="B18">Lu (1997)</xref> from Tsinghua University. The test instruments were NEL-VJH intelligent vacuum water saturator for concrete and NELD-CCM540 chloride diffusion coefficient tester for cement produced by Beijing NELD Company. According to &#x201c;The method for determining the chloride diffusion coefficient for cement mortar&#x201d; (JC/T1086-2008), the specimens were placed in a vacuum environment and soaked with NaCl solution to fully saturate specimens with salt, so that the specimens contained only one conductive ion, chloride ion. After that, the specimen was fixed between electrodes and a DC voltage of 1V&#x2013;10 V was applied. The conductivity was derived from voltage values and electric current values of the specimens, then the chloride diffusion coefficient was derived from the Nernst-Einstein equation with <xref ref-type="disp-formula" rid="e1">Equation 1</xref>. The resistance of material to chloride penetration was evaluated according to the magnitude of diffusion coefficient.<disp-formula id="e1">
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</sec>
<sec id="s2-3-3">
<title>2.3.3 MIP test</title>
<p>MIP tests adopted Micromeritic AutoPore IV 9510 automatic mercury porosimeter produced by American Mac company, which could measure the pore size range of 3&#x2013;360000 nm. The specimens were crushed into particles less than 14 mm in diameter and height. The particles were cleaned and subsequently dried at 60&#xb0;C for 24 h. Then the dried particles were sealed with expansion agent matched by mercury porosimeter, and the pore structure characteristic parameters were measured according to the Washburn equation (<xref ref-type="bibr" rid="B32">Washburn, 1921</xref>). As shown in <xref ref-type="disp-formula" rid="e2">Equation 2</xref>:<disp-formula id="e2">
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</sec>
</sec>
</sec>
<sec sec-type="results|discussion" id="s3">
<title>3 Results and discussion</title>
<sec id="s3-1">
<title>3.1 Stress-strain curves and AE ringing counts</title>
<p>AE characteristic parameters can reflect the evolution of internal cracks during the damage process of cementitious, rock and other materials. In this paper, ringing counts and cumulative ringing counts are selected to analyse the AE characteristics. Ringing counts refers to the number of oscillations exceeding threshold, which can reflect the intensity and frequency of AE signals. Compressive damage of the specimen is a continuous development process. The speed and strength of internal crack development can be known by the response of ringing counts (<xref ref-type="bibr" rid="B5">Dong, et al., 1995</xref>; <xref ref-type="bibr" rid="B10">Ji, et al., 2000</xref>). Uniaxial compression tests were carried out on 5 groups of specimens, and stress-strain curves were obtained. As shown in <xref ref-type="fig" rid="F3">Figure 3</xref>, the compressive strength increased first and then decreased with the increase of PVA content. When volume fraction of PVA was 1%, the compressive strength was 57.49MPa, reaching the maximum value, which was 25.6% higher than that of the reference specimen P0. When volume fraction of PVA was 2%, the compressive strength was 15.2% lower than that of the reference specimen P0, indicating that more fibers would reduce the strength of materials.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Stress-strain curves of test specimens with different PVA content.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g003.tif"/>
</fig>
<p>
<xref ref-type="fig" rid="F4">Figure 4</xref> shows the stress-time-ringing counts-cumulative ringing counts curves of PVA-ECC specimens. According to the change of stress curve slope, compression damage process can be divided into different stages (<xref ref-type="bibr" rid="B47">Zhou et al., 2020</xref>). In this paper, it was divided into densification stage, linear-elastic stage, elastic-plastic stage and destruction stage. <xref ref-type="table" rid="T5">Table 5</xref> shows the proportion of load duration and AE ringing counts in each stage.<list list-type="simple">
<list-item>
<p>Stage I: The densification stage is defined as the period from the beginning of loading to 30% of peak stress. At the initial stage of loading, original pores and initial defects in specimen began to be continuously compressed. The stress increased nonlinearly, and the growth rate gradually accelerated. Ringing counts were few and sparse, signal intensity was weak, and there were no obvious cracks propagation. PVA reduced the proportion of bearing time and ringing count in densification stage to varying degrees, which was due to the filling of PVA to reduce internal microcracks of ECC.</p>
</list-item>
<list-item>
<p>Stage II: The linear-elastic stage occurs from 30% to 80% of peak stress. At this stage, specimen began to bear pressure, stress curve increased linearly, and ringing counts gradually became dense and increased. That indicated meso-cracks in the material began to develop, but macro-cracks had not yet occurred.</p>
</list-item>
<list-item>
<p>Stage III: The elastic-plastic stage spans from 80% to 100% of peak stress. The stress growth rate slowed down until it reached the maximum strength. Ringing counts increased sharply at the peak stress, and cumulative ringing counts curve increased exponentially. It showed that the meso-cracks inside specimen expanded to outer surface, and the surfaces of specimen began to show cross-connected interconnecting macro-cracks. Accumulated deformation energy inside the specimen was released in form of strain waves, and AE signals were frequent. PVA began to play a role in toughness, and played a bridging and crack resistance effect on the cracking damage of specimen, which increased AE events. The proportion of ringing counts of P0.5, P1 and P1.5 were greater than that of P0.</p>
</list-item>
<list-item>
<p>Stage IV: The destruction stage refers to the decrease from 100% of peak stress to 50%. The test set automatically stopped when it dropped to 50% of the peak stress. P0 showed obvious brittle damage after the peak, and stress curve decreased almost linearly. PVA-ECC showed strong ductility characteristics after the peak, and the time proportion of destruction stage with PVA was 28.96%&#x2013;57.8%, which was 53%&#x2013;205% higher than that of P0. This demonstrated that PVA fibers increased residual stress post-damage, changing the damage mode from brittle to ductile and maintaining a certain bearing capacity after damage. The ringing counst in destruction stage accounted for 68%&#x2013;94.95%. After peak stress, the increase of each ringing count represented that specimen had new macro cracks, AE signal intensity increased, and the bearing capacity of specimen decreased rapidly. Ringing counts of P1 still surged in post-peak stage, indicating that its post-peak bearing capacity was large. P2 had the largest proportion of ringing counts in post-peak stage, indicating that its ductility was the largest.</p>
</list-item>
</list>
</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Stress-time-ringing counts-cumulative ringing counts curves. <bold>(A)</bold> P0. <bold>(B)</bold> P0.5. <bold>(C)</bold> P1. <bold>(D)</bold> P1.5. <bold>(E)</bold> P2.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g004.tif"/>
</fig>
<table-wrap id="T5" position="float">
<label>TABLE 5</label>
<caption>
<p>Proportion of ringing counts and bearing time in each stage of the loading process.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th rowspan="2" align="center">Number</th>
<th colspan="2" align="center">Densification stage</th>
<th colspan="2" align="center">Linear-elastic stage</th>
<th colspan="2" align="center">Elastic-plastic stage</th>
<th colspan="2" align="center">Destruction stage</th>
</tr>
<tr>
<th align="center">Proportion of ringing counts</th>
<th align="center">Proportion of bearing time</th>
<th align="center">Proportion of ringing counts</th>
<th align="center">Proportion of bearing time</th>
<th align="center">Proportion of ringing counts</th>
<th align="center">Proportion of bearing time</th>
<th align="center">Proportion of ringing counts</th>
<th align="center">Proportion of bearing time</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">P0</td>
<td align="center">2.76%</td>
<td align="center">58.11%</td>
<td align="center">4.35%</td>
<td align="center">13.76%</td>
<td align="center">8.31%</td>
<td align="center">9.17%</td>
<td align="center">84.59%</td>
<td align="center">18.92%</td>
</tr>
<tr>
<td align="center">P0.5</td>
<td align="center">2.00%</td>
<td align="center">33.36%</td>
<td align="center">2.77%</td>
<td align="center">8.16%</td>
<td align="center">15.56%</td>
<td align="center">5.71%</td>
<td align="center">79.68%</td>
<td align="center">52.74%</td>
</tr>
<tr>
<td align="center">P1</td>
<td align="center">1.10%</td>
<td align="center">47.02%</td>
<td align="center">1.86%</td>
<td align="center">15.80%</td>
<td align="center">29.04%</td>
<td align="center">8.22%</td>
<td align="center">68.00%</td>
<td align="center">28.96%</td>
</tr>
<tr>
<td align="center">P1.5</td>
<td align="center">1.52%</td>
<td align="center">40.27%</td>
<td align="center">2.17%</td>
<td align="center">11.86%</td>
<td align="center">12.11%</td>
<td align="center">11.90%</td>
<td align="center">84.19%</td>
<td align="center">35.94%</td>
</tr>
<tr>
<td align="center">P2</td>
<td align="center">1.19%</td>
<td align="center">26.68%</td>
<td align="center">1.76%</td>
<td align="center">9.55%</td>
<td align="center">2.10%</td>
<td align="center">5.96%</td>
<td align="center">94.95%</td>
<td align="center">57.80%</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s3-2">
<title>3.2 RA-AF distribution characteristics based on Gaussian mixture model</title>
<p>Tensile damage and shear damage mainly occur during the compression damage process of PVA-ECC. The RA-AF value in AE parameters can characterize tensile cracks and shear cracks. RA is the ratio of rise time to amplitude, and AF is the ratio of ringing count to duration. The study found that (<xref ref-type="bibr" rid="B25">Reboul, et al., 2020</xref>) AE signal waveform change gradient under tensile damage is large and signal frequency is high, and the performance is higher AF value and lower RA value; on the contrary, AE signals under shear damage show lower AF values and higher RA values. However, there is no accurate standard for the evaluation of RA and AF values, and the slope method with k as diagonal is commonly used. This method considers that crack above the slash is a tensile crack, and crack below the slash is a shear crack, as shown in <xref ref-type="fig" rid="F5">Figure 5</xref>.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Crack damage type based on RA-AF.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g005.tif"/>
</fig>
<p>Since the RA-AF threshold of ECC is usually difficult to unify, it is difficult to accurately classify the crack types only by slope method. In recent years, scholars have introduced Gaussian Mixture Model (GMM) to cluster RA-AF values. Based on the probability model, GMM classifies data by probability distribution, and calculates m single Gaussian models under different weight coefficients, and uses the Expectation-Maximization (EM) algorithm to fit m mixed Gaussian distributions. The expression of single Gaussian model is shown in <xref ref-type="disp-formula" rid="e3">Equation 3</xref> (<xref ref-type="bibr" rid="B19">Luo, et al., 2024</xref>; <xref ref-type="bibr" rid="B27">Shi, et al., 2024</xref>):<disp-formula id="e3">
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<mml:msub>
<mml:mi>&#x3b1;</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mi>N</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>x</mml:mi>
<mml:mo>&#x7c;</mml:mo>
<mml:msub>
<mml:mi>u</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>,</mml:mo>
<mml:munder>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:munder>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(4)</label>
</disp-formula>where <inline-formula id="inf16">
<mml:math id="m20">
<mml:mrow>
<mml:mi>m</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> &#x3d; the number of models; <inline-formula id="inf17">
<mml:math id="m21">
<mml:mrow>
<mml:msub>
<mml:mi>&#x3b1;</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> &#x3d; the weight of mixed model; <inline-formula id="inf18">
<mml:math id="m22">
<mml:mrow>
<mml:mi>N</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>x</mml:mi>
<mml:mo>&#x7c;</mml:mo>
<mml:msub>
<mml:mi>u</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>,</mml:mo>
<mml:msub>
<mml:mo>&#x2211;</mml:mo>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula> &#x3d; the <inline-formula id="inf19">
<mml:math id="m23">
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> th single Gaussian model density function.</p>
<p>The crack propagation types of PVA-ECC under uniaxial compression are classified by GMM model. <xref ref-type="fig" rid="F6">Figure 6</xref> describes the distribution of RA-AF and the proportion of tensile cracks and shear cracks under five PVA contents. It can be seen from (a) that ECC without PVA were dominated by tensile damage during the damage process, and tensile cracks account for 70%. The addition of PVA changed the propagation mode of internal cracks in ECC. The proportion of shear cracks in PVA-ECC under uniaxial compression exceeded 50%, and the proportion of shear cracks increased first and then decreased with the increase of PVA contents. When PVA content was 1%, the proportion of shear cracks was the largest, reaching 62.57%.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>RA-AF scatter plot and the proportion of tensile cracks and shear cracks. <bold>(A)</bold> P0. <bold>(B)</bold> P0.5. <bold>(C)</bold> P1. <bold>(D)</bold> P1.5. <bold>(E)</bold> P2.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g006.tif"/>
</fig>
<p>The compression of ECC first led to tensile stress, which caused micro-cracks to form in the interior. As shown in <xref ref-type="table" rid="T6">Table 6</xref>, in densification stages, linear-elasticity stages, and elastic-plastic stages, the number of cracks was small, and the internal cracks were mostly caused by tensile damage. When stress reached the maximum value, the number of cracks increased sharply after the specimen was destroyed, which was consistent with AE event signal activity. In destruction stage, the proportion of shear cracks increased, which was due to the bridging effect of PVA, so that the bite force at crack propagation increased, and internal shear stress of the specimen increased. After shear stress bears part of stress, the degree of crack tensile cracking decreased. The damage mode transited from tensile damage to shear damage. The specimen was not split by a single vertical crack, but formed a multi-directional irregular shear crack, which inhibited the formation of interconnecting cracks and the release of deformation energy. PVA changed internal compression damage mechanism of specimen and improved tensile, shear and fracture toughness of ECC.</p>
<table-wrap id="T6" position="float">
<label>TABLE 6</label>
<caption>
<p>The number and proportion of tensile cracks and shear cracks in each damage stage.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">Number</th>
<th align="center">Damage stage</th>
<th align="center">Number of tensile crack</th>
<th align="center">Number of shear crack</th>
<th align="center">Percentage of tensile crack</th>
<th align="center">Percentage of shear crack</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td rowspan="4" align="center">P0</td>
<td align="center">densification stage</td>
<td align="center">2,678</td>
<td align="center">755</td>
<td align="center">78.01%</td>
<td align="center">21.99%</td>
</tr>
<tr>
<td align="center">linear-elastic stage</td>
<td align="center">4,680</td>
<td align="center">958</td>
<td align="center">83.01%</td>
<td align="center">16.99%</td>
</tr>
<tr>
<td align="center">elastic-plastic stage</td>
<td align="center">8,782</td>
<td align="center">2,588</td>
<td align="center">77.24%</td>
<td align="center">22.76%</td>
</tr>
<tr>
<td align="center">destruction stage</td>
<td align="center">56,388</td>
<td align="center">26,943</td>
<td align="center">67.67%</td>
<td align="center">32.33%</td>
</tr>
<tr>
<td rowspan="4" align="center">P0.5</td>
<td align="center">densification stage</td>
<td align="center">7,142</td>
<td align="center">4,530</td>
<td align="center">61.19%</td>
<td align="center">38.81%</td>
</tr>
<tr>
<td align="center">linear-elastic stage</td>
<td align="center">12,447</td>
<td align="center">3,460</td>
<td align="center">78.25%</td>
<td align="center">21.75%</td>
</tr>
<tr>
<td align="center">elastic-plastic stage</td>
<td align="center">17,286</td>
<td align="center">11,189</td>
<td align="center">60.71%</td>
<td align="center">39.29%</td>
</tr>
<tr>
<td align="center">destruction stage</td>
<td align="center">170,677</td>
<td align="center">274,045</td>
<td align="center">38.38%</td>
<td align="center">61.62%</td>
</tr>
<tr>
<td rowspan="4" align="center">P1</td>
<td align="center">densification stage</td>
<td align="center">1,692</td>
<td align="center">679</td>
<td align="center">71.36%</td>
<td align="center">28.64%</td>
</tr>
<tr>
<td align="center">linear-elastic stage</td>
<td align="center">2,199</td>
<td align="center">436</td>
<td align="center">83.45%</td>
<td align="center">16.55%</td>
</tr>
<tr>
<td align="center">elastic-plastic stage</td>
<td align="center">3,787</td>
<td align="center">2019</td>
<td align="center">65.23%</td>
<td align="center">34.77%</td>
</tr>
<tr>
<td align="center">destruction stage</td>
<td align="center">79,066</td>
<td align="center">141,902</td>
<td align="center">35.78%</td>
<td align="center">64.22%</td>
</tr>
<tr>
<td rowspan="4" align="center">P1.5</td>
<td align="center">densification stage</td>
<td align="center">3,175</td>
<td align="center">1,617</td>
<td align="center">66.26%</td>
<td align="center">33.74%</td>
</tr>
<tr>
<td align="center">linear-elastic stage</td>
<td align="center">6,053</td>
<td align="center">1,470</td>
<td align="center">80.46%</td>
<td align="center">19.54%</td>
</tr>
<tr>
<td align="center">elastic-plastic stage</td>
<td align="center">24,562</td>
<td align="center">14,893</td>
<td align="center">62.25%</td>
<td align="center">37.75%</td>
</tr>
<tr>
<td align="center">destruction stage</td>
<td align="center">106,127</td>
<td align="center">167,327</td>
<td align="center">38.81%</td>
<td align="center">61.19%</td>
</tr>
<tr>
<td rowspan="4" align="center">P2</td>
<td align="center">densification stage</td>
<td align="center">1,334</td>
<td align="center">936</td>
<td align="center">58.77%</td>
<td align="center">41.23%</td>
</tr>
<tr>
<td align="center">linear-elastic stage</td>
<td align="center">4,883</td>
<td align="center">1,489</td>
<td align="center">76.63%</td>
<td align="center">23.37%</td>
</tr>
<tr>
<td align="center">elastic-plastic stage</td>
<td align="center">6,396</td>
<td align="center">1873</td>
<td align="center">77.35%</td>
<td align="center">22.65%</td>
</tr>
<tr>
<td align="center">destruction stage</td>
<td align="center">106,043</td>
<td align="center">133,388</td>
<td align="center">44.29%</td>
<td align="center">55.71%</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s3-3">
<title>3.3 Chloride diffusion coefficient</title>
<p>Chlorine penetration tests were carried out on ECC with different fiber content. Three tests were carried out on the same batch of specimens to take the average value to obtain the chloride diffusion coefficient of the material as shown in <xref ref-type="table" rid="T7">Table 7</xref> and <xref ref-type="fig" rid="F7">Figure 7</xref>. The chloride diffusion coefficients show firstly decrease and then increase with increasing PVA fiber content. When PVA fiber content is 1%, the chloride diffusion coefficient is the smallest, which decreases by 44.2% compared with the baseline specimen P0, and the specimen has the best impermeability performance.</p>
<table-wrap id="T7" position="float">
<label>TABLE 7</label>
<caption>
<p>Chloride diffusion coefficients (10<sup>&#x2212;12</sup>) of the materials.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">Number</th>
<th align="center">P0</th>
<th align="center">P0.5</th>
<th align="center">P1.0</th>
<th align="center">P1.5</th>
<th align="center">P2</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">diffusion coefficient 1</td>
<td align="center">6.325</td>
<td align="center">5.863</td>
<td align="center">3.368</td>
<td align="center">7.024</td>
<td align="center">8.267</td>
</tr>
<tr>
<td align="center">diffusion coefficient 2</td>
<td align="center">5.889</td>
<td align="center">4.598</td>
<td align="center">3.223</td>
<td align="center">7.810</td>
<td align="center">8.313</td>
</tr>
<tr>
<td align="center">diffusion coefficient 3</td>
<td align="center">6.23</td>
<td align="center">4.883</td>
<td align="center">3.693</td>
<td align="center">6.917</td>
<td align="center">7.894</td>
</tr>
<tr>
<td align="center">Average</td>
<td align="center">6.148</td>
<td align="center">5.114</td>
<td align="center">3.428</td>
<td align="center">7.250</td>
<td align="center">8.158</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Chloride diffusion coefficients of PVA-ECC.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g007.tif"/>
</fig>
</sec>
<sec id="s3-4">
<title>3.4 Pore structure parameters</title>
<p>Among the pore structure parameters, porosity, total pore volume and most probable aperture are important parameters affecting the macroscopic properties of concrete (<xref ref-type="bibr" rid="B15">Li, et al., 2024</xref>). <xref ref-type="fig" rid="F8">Figure 8A</xref> depicts the pore size distribution curves. Most probable aperture is the pore size with the highest probability of occurrence, which corresponds to the peak of distribution density in pore size distribution curve. From (a), it is clear that P1 has the smallest most probable aperture. <xref ref-type="fig" rid="F8">Figure 8B</xref> depicts the cumulative porosity curves, where P1 porosity is the smallest at 23.68%. <xref ref-type="table" rid="T8">Table 8</xref> shows the measured values of porosity, total pore volume, and most probable aperture for five groups of specimens in MIP tests. It can be seen that porosity, total pore volume and most probable aperture of PVA-ECC show a pattern of firstly decreasing and then increasing with increasing PVA content. The pore structure is optimal at 1% PVA fiber content, suggesting that a moderate amount of PVA fibers improves pore structure and increases compactness, reducing initial defects. However, excessive PVA fibers are difficult to disperse, forming groups that negatively affect fluidity, adhesion, and polymerization, increasing internal porosity and microscopic defects, thus adversely affecting pore size distribution and compressive strength.</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>MIP results of PVA-ECC. <bold>(A)</bold> Pore size distribution curves <bold>(B)</bold> Cumulative porosity curves.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g008.tif"/>
</fig>
<table-wrap id="T8" position="float">
<label>TABLE 8</label>
<caption>
<p>Pore structure parameters.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">Number</th>
<th align="center">Porosity/%</th>
<th align="center">Total pore volume/(mg/L)</th>
<th align="center">Most probable aperture/nm</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">P0</td>
<td align="center">25.43</td>
<td align="center">0.1458</td>
<td align="center">1,046</td>
</tr>
<tr>
<td align="center">P0.5</td>
<td align="center">25.08</td>
<td align="center">0.1425</td>
<td align="center">672</td>
</tr>
<tr>
<td align="center">P1</td>
<td align="center">23.68</td>
<td align="center">0.1339</td>
<td align="center">183</td>
</tr>
<tr>
<td align="center">P1.5</td>
<td align="center">29.21</td>
<td align="center">0.1802</td>
<td align="center">1,310</td>
</tr>
<tr>
<td align="center">P2</td>
<td align="center">29.32</td>
<td align="center">0.1769</td>
<td align="center">1,310</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The pore sizes are categorized into four ranges: gel pores (&#x3c;100 nm), transition pores (100&#x2013;1,000 nm), capillary pores (1,000&#x2013;10000 nm), and macropores (&#x3e;10,000 nm) (<xref ref-type="bibr" rid="B46">Zhao Y. C. et al., 2023</xref>). The percentage of different pore size ranges in total pore volume is shown in <xref ref-type="fig" rid="F9">Figure 9</xref>.</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>The percentage of different pore size ranges to the total pore volume.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g009.tif"/>
</fig>
<p>Gel pores are harmless or less harmful pores, which are mainly formed by cement hydration reaction and gas produced by water evaporation during mixing. Transition pores, capillary pores and macropores are harmful pores. Transition pores are generated by the gap between cement particles. Capillary pores are the voids left by cementitious particles that are not filled by hydration products. Macropores are mainly cracks caused by uneven distribution of aggregates in materials. Harmful pores affect the mechanical properties and durability of ECC. It was found that PVA mainly affected the number of gel pores and capillary pores. Appropriate amount of PVA increased the number of gel pores and decreased the number of capillary pores. Excessive fibers led to poor dispersion of the material, resulting in uneven distribution between aggregates, which made the number of capillary pores and macropores increase.</p>
</sec>
<sec id="s3-5">
<title>3.5 Fractal dimension of pore structure</title>
<p>Fractal theory effectively analyzes the pore size distribution of materials, characterizing the pore structure (<xref ref-type="bibr" rid="B34">Winslow, 1985</xref>; <xref ref-type="bibr" rid="B36">Xuan, et al., 2018</xref>). Menger sponge model and thermodynamic-based fractal model were used to calculate the fractal dimension. The Menger sponge model assumes a square unit cell with side length R, which is divided equally into n small cubes with r. The contents were obtained by the residual relative volume formula (<xref ref-type="bibr" rid="B33">Wei, et al., 2007</xref>), as shown in <xref ref-type="disp-formula" rid="e5">Equations 5</xref>-<xref ref-type="disp-formula" rid="e7">7</xref>:<disp-formula id="e5">
<mml:math id="m24">
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</disp-formula>
<disp-formula id="e6">
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</disp-formula>
<disp-formula id="e7">
<mml:math id="m26">
<mml:mrow>
<mml:mi>D</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>3</mml:mn>
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<mml:mfenced open="(" close=")" separators="|">
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<mml:mi>P</mml:mi>
</mml:mrow>
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</mml:mrow>
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<mml:mrow>
<mml:mi>lg</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>r</mml:mi>
<mml:mo>/</mml:mo>
<mml:mi>R</mml:mi>
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</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(7)</label>
</disp-formula>where D &#x3d; fractal dimension; <italic>p</italic> &#x3d; material porosity, which is the cumulative percentage of mercury that entering material at a given pressure value in mercury compression experiments; r &#x3d; corresponding pore size at pressure value; R &#x3d; maximum pore size. R/R responds to the pore size distribution of material. A larger fractal dimension D indicates a more complex pore space and better pore structure of material.</p>
<p>
<xref ref-type="bibr" rid="B40">Zhang and Li (1995)</xref> proposed thermodynamic fractal model based on the principle of energy conservation, which suggests that the work done by external environment on mercury in MIP test is equal to the increase in surface energy of the mercury that enters pores. Its expression is <xref ref-type="disp-formula" rid="e8">Equation 8</xref>:<disp-formula id="e8">
<mml:math id="m27">
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<mml:msubsup>
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<mml:mi>&#x3c3;</mml:mi>
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<mml:mi mathvariant="normal">d</mml:mi>
<mml:mi>S</mml:mi>
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<label>(8)</label>
</disp-formula>where <italic>p</italic> &#x3d; the pressure applied when pressing mercury. V &#x3d; the amount of mercury pressed in specimen. S &#x3d; the pore surface area.</p>
<p>Pore specific surface area, pore size and mercury intake are correlated by fractal analysis, and after quantitative analysis, the relationship is expressed as shown in <xref ref-type="disp-formula" rid="e9">Equation 9</xref>:<disp-formula id="e9">
<mml:math id="m28">
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<mml:mi>n</mml:mi>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>D</mml:mi>
</mml:mrow>
</mml:msubsup>
<mml:msubsup>
<mml:mi>V</mml:mi>
<mml:mi>n</mml:mi>
<mml:mrow>
<mml:mi>D</mml:mi>
<mml:mo>/</mml:mo>
<mml:mn>3</mml:mn>
</mml:mrow>
</mml:msubsup>
</mml:mrow>
</mml:math>
<label>(9)</label>
</disp-formula>where <inline-formula id="inf20">
<mml:math id="m29">
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> &#x3d; Pressure at <inline-formula id="inf21">
<mml:math id="m30">
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> th pressurization, (Pa); <inline-formula id="inf22">
<mml:math id="m31">
<mml:mrow>
<mml:mo>&#x394;</mml:mo>
<mml:msub>
<mml:mi>V</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> &#x3d; Mercury feed at the <inline-formula id="inf23">
<mml:math id="m32">
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> th pressing of mercury, (m<sup>3</sup>); <inline-formula id="inf24">
<mml:math id="m33">
<mml:mrow>
<mml:msub>
<mml:mi>r</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> &#x3d; Pore size at <inline-formula id="inf25">
<mml:math id="m34">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> th pressing of mercury, (m); <inline-formula id="inf26">
<mml:math id="m35">
<mml:mrow>
<mml:msub>
<mml:mi>V</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> &#x3d; Cumulative mercury feed at stage <inline-formula id="inf27">
<mml:math id="m36">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>, (m<sup>3</sup>); <inline-formula id="inf28">
<mml:math id="m37">
<mml:mrow>
<mml:msup>
<mml:mi>C</mml:mi>
<mml:mo>&#x2032;</mml:mo>
</mml:msup>
</mml:mrow>
</mml:math>
</inline-formula> &#x3d; Constant factor; <inline-formula id="inf29">
<mml:math id="m38">
<mml:mrow>
<mml:mi>D</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> &#x3d; Fractal dimensions based on thermodynamic relations.</p>
<p>We demand <inline-formula id="inf30">
<mml:math id="m39">
<mml:mrow>
<mml:msub>
<mml:mi>W</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mstyle displaystyle="true">
<mml:msubsup>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mi>n</mml:mi>
</mml:msubsup>
</mml:mstyle>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>&#x394;</mml:mo>
<mml:msub>
<mml:mi>V</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>, <inline-formula id="inf31">
<mml:math id="m40">
<mml:mrow>
<mml:msub>
<mml:mi>Q</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:msubsup>
<mml:mi>V</mml:mi>
<mml:mi>n</mml:mi>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>/</mml:mo>
<mml:mn>3</mml:mn>
</mml:mrow>
</mml:msubsup>
<mml:mo>/</mml:mo>
<mml:msub>
<mml:mi>r</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>, logarithmic conversion is performed to obtain <xref ref-type="disp-formula" rid="e10">Equation 10</xref>:<disp-formula id="e10">
<mml:math id="m41">
<mml:mrow>
<mml:mi>lg</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msub>
<mml:mi>W</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
<mml:mo>/</mml:mo>
<mml:msubsup>
<mml:mi>r</mml:mi>
<mml:mi>n</mml:mi>
<mml:mn>2</mml:mn>
</mml:msubsup>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>D</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:mi>lg</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:msub>
<mml:mi>Q</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>lg</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:msup>
<mml:mi>C</mml:mi>
<mml:mo>&#x2032;</mml:mo>
</mml:msup>
</mml:mrow>
</mml:math>
<label>(10)</label>
</disp-formula>
</p>
<p>The five groups fractal dimensions of specimens were calculated based on two fractal models, and the relationship curves for P0 were fitted. As shown in <xref ref-type="fig" rid="F10">Figure 10</xref>, the fractal curves based on thermodynamic relationship present a high degree of linear correlation, and the correlation coefficients <italic>R</italic>
<sup>2</sup> are all greater than 0.999, indicating that this model can more accurately reflect the fractal characteristics of pore size distribution of PVA-ECC. Fractal dimensions increased and then decreased with the increase of PVA contents. The larger fractal dimension is, the more complex internal structure of pores is, and the more reasonable pore size distribution is.</p>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>Fractal dimension of PVA-ECC. <bold>(A)</bold> Menger sponge model <bold>(B)</bold> Fractal model based on thermodynamic relationships.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g010.tif"/>
</fig>
<p>In order to further study the effect of PVA on pore size distribution, the fractal dimensions of gel pores, transition pores, capillary pores and macropores of five groups of specimens were calculated in <xref ref-type="table" rid="T9">Table 9</xref>. According to three-dimensional Euclidean space, the fractal dimension D of ECC is between 2 and 3. The transition pores and capillary pores in table have D<sub>S</sub>&#x3e;3. At present, scholars believe that this is due to the presence of ink bottle-shaped pores in cementitious materials (<xref ref-type="bibr" rid="B39">Zeng, et al., 2010</xref>; <xref ref-type="bibr" rid="B12">Lee and Jacobsen, 2011</xref>). Ink bottle-shaped pores are usually formed by evaporation of water during hardening process of cementitious materials. In MIP test, only when the intrusion pressure is large, mercury will enter the small pore. At this time, the small pore volume is recorded, but it is actually the total volume of large pore and small pore in the ink bottle-shaped pore. According to the data of <xref ref-type="table" rid="T9">Table 9</xref>, it is speculated that PVA cause ink bottle-shaped pores in specimen.</p>
<table-wrap id="T9" position="float">
<label>TABLE 9</label>
<caption>
<p>Fractal dimension of different pore size range.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th rowspan="2" align="center">Number</th>
<th colspan="2" align="center">Gel pore</th>
<th colspan="2" align="center">Transition pore</th>
<th colspan="2" align="center">Capillary pore</th>
<th colspan="2" align="center">Macropore</th>
</tr>
<tr>
<th align="center">D<sub>S</sub>
</th>
<th align="center">
<italic>R</italic>
<sup>2</sup>
</th>
<th align="center">D<sub>S</sub>
</th>
<th align="center">
<italic>R</italic>
<sup>2</sup>
</th>
<th align="center">D<sub>S</sub>
</th>
<th align="center">
<italic>R</italic>
<sup>2</sup>
</th>
<th align="center">D<sub>S</sub>
</th>
<th align="center">
<italic>R</italic>
<sup>2</sup>
</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">P0</td>
<td align="center">2.903</td>
<td align="center">0.9998</td>
<td align="center">2.953</td>
<td align="center">0.9997</td>
<td align="center">2.999</td>
<td align="center">0.9965</td>
<td align="center">2.807</td>
<td align="center">0.9999</td>
</tr>
<tr>
<td align="center">P0.5</td>
<td align="center">2.883</td>
<td align="center">0.9998</td>
<td align="center">2.957</td>
<td align="center">0.9998</td>
<td align="center">3.098</td>
<td align="center">0.9990</td>
<td align="center">2.827</td>
<td align="center">0.9999</td>
</tr>
<tr>
<td align="center">P1.0</td>
<td align="center">2.902</td>
<td align="center">0.9999</td>
<td align="center">3.115</td>
<td align="center">0.9999</td>
<td align="center">2.947</td>
<td align="center">0.9992</td>
<td align="center">2.817</td>
<td align="center">0.9999</td>
</tr>
<tr>
<td align="center">P1.5</td>
<td align="center">2.906</td>
<td align="center">0.9998</td>
<td align="center">2.931</td>
<td align="center">0.9999</td>
<td align="center">3.055</td>
<td align="center">0.9994</td>
<td align="center">2.831</td>
<td align="center">0.9999</td>
</tr>
<tr>
<td align="center">P2.0</td>
<td align="center">2.923</td>
<td align="center">0.9998</td>
<td align="center">2.895</td>
<td align="center">0.9999</td>
<td align="center">3.074</td>
<td align="center">0.9974</td>
<td align="center">2.818</td>
<td align="center">0.9999</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>
<xref ref-type="fig" rid="F11">Figure 11</xref> describes the change of fractal dimension of each pore range under different PVA content. PVA had a great influence on the fractal characteristics of transition pores and capillary pores, and had little influence on the fractal characteristics of gel pores and macropores. This was because the fiber diameter was in range of capillary pore diameter, and the most probable apertures in five groups of specimens were in range of transition pores and capillary pores. Therefore, the fiber had a great influence on the spatial structure distribution of transition pores and capillary pores.</p>
<fig id="F11" position="float">
<label>FIGURE 11</label>
<caption>
<p>The variation law of fractal dimension in each pore size range.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g011.tif"/>
</fig>
</sec>
<sec id="s3-6">
<title>3.6 The correlation between fractal dimension and pore structure parameters</title>
<p>Studies have shown that the fractal dimension of fiber reinforced concrete has a certain correlation with pore structure parameters and mechanical parameters (<xref ref-type="bibr" rid="B15">Li, et al., 2024</xref>; <xref ref-type="bibr" rid="B44">Zhao J. et al., 2023</xref>). <xref ref-type="fig" rid="F12">Figure 12</xref> shows the relationship between porosity, total pore volume, most probable aperture of P0, P0.5, P1, P1.5, P2 and their fractal dimension. It can be found that the porosity, total pore volume, and most probable aperture of PVA-ECC have a strong negative correlation with the fractal dimension, and the correlation coefficients <italic>R</italic>
<sup>2</sup> are 0.970, 0.981, and 0.863 respectively. The porosity, total pore volume and most probable aperture decrease with the increase of fractal dimension. Fractal dimension can be used to comprehensively characterize pore structure characteristics. The larger fractal dimension leads to the higher complexity of internal pore structure space and the higher ability of pore size occupying the space. This also leads to a smaller most probable aperture, which avoids development of the internal connected pore size to the larger pore size, and reduces the probability and proportion of the larger pore size, while makes the overall porosity and total pore volume lower.</p>
<fig id="F12" position="float">
<label>FIGURE 12</label>
<caption>
<p>The correlation between fractal dimension and pore structural parameters. <bold>(A)</bold> Porosity <bold>(B)</bold> Total pore volume <bold>(C)</bold> Most probable aperture.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g012.tif"/>
</fig>
</sec>
<sec id="s3-7">
<title>3.7 The correlation between fractal dimension and compressive strength, chloride diffusion coefficient</title>
<p>
<xref ref-type="fig" rid="F13">Figure 13</xref> depicts the correlation between fractal dimension and compressive strength. The correlation coefficient <italic>R</italic>
<sup>2</sup> is 0.804. Compressive strength has a good positive correlation with fractal dimension, and increases with the increase of fractal dimension. The increase in fractal dimension represents a higher spatial complexity of the pore structure, which indicates an increase in multidirectionality of the initial defects, inhomogeneity and asymmetry of the fracture structure. During initial deformation stage, the internal stresses have not been concentrated due to the randomness of initial defect distribution. During loading process, some of the initial defects and cracks are compacted, while others are &#x201c;activated&#x201d; and gradually evolve into connected cracks, resulting in internal stress concentrations. The fractal dimension, representing the spatial complexity of microstructure, is closely related to this &#x201c;competition&#x201d; between compact deformation and crack evolution. When fractal dimension is large, it is difficult to form connecting cracks within structure, and stress concentration phenomenon is not easy to occur, while the compressive capacity of specimen is improved to a certain extent.</p>
<fig id="F13" position="float">
<label>FIGURE 13</label>
<caption>
<p>The correlation between fractal dimension and compressive strength.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g013.tif"/>
</fig>
<p>
<xref ref-type="fig" rid="F14">Figure 14</xref> depicts the correlation between fractal dimension and chloride diffusion coefficient. The correlation coefficient <italic>R</italic>
<sup>2</sup> is 0.873. Chloride diffusion coefficient has a good negative correlation with fractal dimension, and decreases with the increase of fractal dimension. With spatial structure becoming complex, the interconnecting pores become less, and the ions is more difficult to flow between pores, so that chloride diffusion coefficient becomes lower, and the impermeability of material is improved.</p>
<fig id="F14" position="float">
<label>FIGURE 14</label>
<caption>
<p>The correlation between fractal dimension and chloride diffusion coefficient.</p>
</caption>
<graphic xlink:href="fmats-11-1513872-g014.tif"/>
</fig>
<p>Fractal dimension indicates that the mechanical strength and impermeability of ECC are closely related to the pore structure characteristics. The fractal dimension can be used to assess or predict the mechanical strength, impermeability and microstructure of PVA-ECC in advance, and to make a comprehensive evaluation of the mechanical properties and durability of material.</p>
</sec>
</sec>
<sec sec-type="conclusion" id="s4">
<title>4 Conclusion</title>
<p>In this paper, the influences of PVA on compressive damage mechanism and pore structure fractal characteristics of ECC are obtained through experimental research. The conclusions are as follows:<list list-type="simple">
<list-item>
<p>(1) When volume fraction of PVA is less than 2%, the compressive strength increases first and then decreases with increase of PVA. and the peak point appears when the fiber content is 1%. The uniaxial compression damage of specimen can be divided into four stages: densification stage, linear-elastic stage, elastic-plastic stage and destruction stage. The number of AE ringing counts is small in densification stage and linear elastic stage, reflecting the compaction of initial pores and the generation of meso-cracks; It increases exponentially in elastic-plastic stage, reflecting the expansion of internal cracks to the surface to form macro-cracks. PVA increase the toughness of ECC and slow down the decrease of post-peak stress curve, while prolong post-peak bearing time and activate AE signals. ECC develops from brittle damage to ductile damage.</p>
</list-item>
<list-item>
<p>(2) The characteristics of RA-AF are analyzed by GMM model. In compression damage, the proportion of tensile cracks in P0 is 70%, the proportion of shear cracks in PVA-ECC is more than 50%, and the proportion of shear cracks increases first and then decreases with the increase of PVA content. The bridging effect of PVA transforms internal tensile stress of ECC into shear stress, which inhibits the generation of penetrating cracks. The effect of PVA on proportion of shear cracks is consistent with the effect on compressive strength. PVA change the compression damage mechanism and improve the compressive capacity of ECC.</p>
</list-item>
<list-item>
<p>(3) The chloride diffusion coefficient decreases first and then increases with the increase of PVA. Chloride diffusion coefficient of P1 is the smallest, which is 44.2% lower than that of reference specimen P0, and the impermeability of P1 is the best. The porosity, total pore volume and most probable aperture of PVA-ECC decrease first and then increase with the increase of PVA content. When PVA content is 1%, the number and volume of pores are the least, and ECC is the most dense. The influence of PVA on pore structure parameters and chloride diffusion coefficient is consistent. The pore size can be divided into four distribution ranges: gel pores (&#x3c;100 nm), transition pores (100nm&#x2013;1000 nm), capillary pores (1,000nm&#x2013;10000 nm) and macropores (&#x3e;10000 nm). PVA mainly affects the proportion of gel pores and capillary pores.</p>
</list-item>
<list-item>
<p>(4) The fractal model based on thermodynamic relationship can better characterize the fractal characteristics of PVA-ECC. Fractal dimension increases first and then decreases with the increase of PVA content, and P1 has the best fractal characteristics. In pore size distribution, due to the size characteristics of fiber diameter and most probable aperture, PVA has a great influence on the fractal characteristics of transition pores and capillary pores, and has little influence on the fractal characteristics of gel pores and macropores.</p>
</list-item>
<list-item>
<p>(5) Porosity, total pore volume and most probable aperture of PVA-ECC have a strong negative correlation with fractal dimension. Fractal dimension can be used to comprehensively characterize the pore structure characteristics of materials. Compressive strength of PVA-ECC has a good positive correlation with fractal dimension, and chloride diffusion coefficient has a good negative correlation with fractal dimension. The fractal dimension shows that mechanical strength and impermeability of cementitious materials are closely related to the complex spatial structure and distribution characteristics of pores.</p>
</list-item>
</list>
</p>
<p>This study simultaneously analyzes the effect of PVA fiber content on the structure and properties of ECC from both macro and micro perspectives. The mechanical strength, impermeability, pore size distribution, and fractal characteristics of PVA-ECC with 1% volumetric content are best in the range of 0%&#x2013;2% PVA content. The fractal characteristics of materials are closely related to their mechanical properties and durability, and fractal dimension can be used as one of indicators to comprehensively evaluate the mechanical properties and durability of ECC. This paper provides a reference for practical engineering applications.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="s5">
<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 sec-type="author-contributions" id="s6">
<title>Author contributions</title>
<p>YL: Conceptualization, Funding acquisition, Methodology, Software, Visualization, Writing&#x2013;original draft, Writing&#x2013;review and editing. XH: Formal Analysis, Project administration, Validation, Writing&#x2013;review and editing. YZ: Data curation, Investigation, Resources, Writing&#x2013;review and editing. YQ: Data curation, Investigation, Methodology, Writing&#x2013;review and editing.</p>
</sec>
<sec sec-type="funding-information" id="s7">
<title>Funding</title>
<p>The author(s) declare that financial support was received for the research, authorship, and/or publication of this article. This research was funding by Hebei Technology Innovation Center for Multi-Hazard Resilience and Emergency Handling of Engineering Structures (Grant No. FZ246304).</p>
</sec>
<sec sec-type="COI-statement" id="s8">
<title>Conflict of interest</title>
<p>The 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 sec-type="ai-statement" id="s10">
<title>Generative AI statement</title>
<p>The author(s) declare that no Generative AI was used in the creation of this manuscript.</p>
</sec>
<sec sec-type="disclaimer" id="s9">
<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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