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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">1216747</article-id>
<article-id pub-id-type="doi">10.3389/fmats.2023.1216747</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>A new experimental method to measure and calculate the tensile strength of concrete</article-title>
<alt-title alt-title-type="left-running-head">Chai 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.2023.1216747">10.3389/fmats.2023.1216747</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Chai</surname>
<given-names>Qihui</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Huang</surname>
<given-names>Shasha</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Wan</surname>
<given-names>Fang</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/2267104/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Wu</surname>
<given-names>Feng</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Feng</surname>
<given-names>Lingyun</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>School of Water Resources</institution>, <institution>North China University of Water Resources and Electric Power</institution>, <addr-line>Zhengzhou</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Henan Key Laboratory of Water Resources Conservation and Intensive Utilization in the Yellow River Basin</institution>, <addr-line>Zhengzhou</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/2012752/overview">Wei Ge</ext-link>, Zhengzhou University, 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/2307385/overview">Wei Dongle</ext-link>, Dalian University of Technology, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1696816/overview">Zhang Lei</ext-link>, Yellow River Institute of Hydraulic Research, China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Fang Wan, <email>wanxf1023@163.com</email>
</corresp>
</author-notes>
<pub-date pub-type="epub">
<day>20</day>
<month>07</month>
<year>2023</year>
</pub-date>
<pub-date pub-type="ecorrected">
<day>22</day>
<month>05</month>
<year>2026</year>
</pub-date>
<pub-date pub-type="collection">
<year>2023</year>
</pub-date>
<volume>10</volume>
<elocation-id>1216747</elocation-id>
<history>
<date date-type="received">
<day>04</day>
<month>05</month>
<year>2023</year>
</date>
<date date-type="accepted">
<day>28</day>
<month>06</month>
<year>2023</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2023 Chai, Huang, Wan, Wu and Feng.</copyright-statement>
<copyright-year>2023</copyright-year>
<copyright-holder>Chai, Huang, Wan, Wu and Feng</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>
<sec>
<title>Introduction</title>
<p>A new method is introduced to test the tensile strength of concrete: the cylinder transverse splitting test. Compared with the cylinder splitting (or Brazilian) test, the cylinder transverse splitting test involves different load positions and offers the advantages of doubling the data volume with the same number of specimens and improving the detection accuracy.</p>
</sec>
<sec>
<title>Methods</title>
<p>Finite element analysis software was used to simulate the concrete cylinder transverse splitting test and the stress distribution on the failure surface was determined.</p>
</sec>
<sec>
<title>Results and Discussion</title>
<p>The results show that the fracture of a cylinder is mainly determined by tensile stress. The splitting strength of normal concrete and crumb rubber concrete, a new environmentally friendly concrete material that has gathered considerable attention in recent years, was obtained by cylinder transverse and cube splitting tests. The cylinder transverse splitting test data show a stable correlation with the cube splitting test data and well characterize the concrete strength. The relationship between the cylinder nominal transverse splitting strength (<italic>f</italic>
<sub>2</sub>) and cube splitting strength (<italic>f</italic>
<sub>1</sub>) was established on the basis of linear analysis of the test data: <italic>f</italic>
<sub>1</sub> &#x3d; 0.51<italic>f</italic>
<sub>2</sub>. The calculated cube splitting strength is in good agreement with the test values.</p>
</sec>
</abstract>
<kwd-group>
<kwd>cylinder transverse splitting method</kwd>
<kwd>nominal transverse splitting strength</kwd>
<kwd>cube splitting strength</kwd>
<kwd>crumb rubber concrete</kwd>
<kwd>rubber content</kwd>
</kwd-group>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-at-acceptance</meta-name>
<meta-value>Structural Materials</meta-value>
</custom-meta>
</custom-meta-wrap>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>The tensile strength of concrete is substantially less than its compressive strength. Cracks in concrete easily propagate under tension, which can affect its service life and durability (<xref ref-type="bibr" rid="B4">Bhanja and Sengupta, 2005</xref>; <xref ref-type="bibr" rid="B11">Ge et al., 2022</xref>). A large number of laboratory studies have evaluated the tensile strength of concrete using three main methods: direct tensile tests; beam flexural tests; and splitting tensile tests (<xref ref-type="bibr" rid="B30">Rashid, et al., 2002</xref>; <xref ref-type="bibr" rid="B23">Lu and Li, 2011</xref>). Direct tension is theoretically considered to yield a tensile strength similar to the true strength of the concrete under pure uniaxial tension (<xref ref-type="bibr" rid="B46">Wu et al., 2012</xref>), but is often difficult to apply owing to the lack of control over the initial crack position, local stress concentrations, and eccentricity strain (<xref ref-type="bibr" rid="B38">Swaddiwudhipong et al., 2003</xref>; <xref ref-type="bibr" rid="B57">Zi et al., 2008</xref>; <xref ref-type="bibr" rid="B32">Sarfarazi et al., 2018</xref>). Furthermore, tensile strength values derived from beam flexural tests tend to be higher than those obtained from direct tensile tests (<xref ref-type="bibr" rid="B29">Raphael, 1984</xref>). There are two types of splitting tensile tests listed in <xref ref-type="bibr" rid="B10">GB/T50081-2002. (2002)</xref>: the cube splitting test (<xref ref-type="fig" rid="F1">Figure 1A</xref>) and the cylinder splitting (or Brazilian) test (<xref ref-type="fig" rid="F1">Figure 1B</xref>). Previous studies have shown that the tensile strength obtained from cylinder splitting tests are closer to the true tensile strength than flexural tests (<xref ref-type="bibr" rid="B25">Mindess et al., 2002</xref>; <xref ref-type="bibr" rid="B44">Wang et al., 2022</xref>). The results of cylinder splitting tests have also been shown to provide better tensile strength predications than cube splitting tests (<xref ref-type="bibr" rid="B26">Nilsson, 1961</xref>).</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Two types of concrete specimen splitting tests: the cube splitting test <bold>(A)</bold> and the cylinder splitting test <bold>(B)</bold>.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g001.tif"/>
</fig>
<p>The measurement of concrete strength is important for evaluating the construction quality of completed concrete projects. The drilled-core method is commonly used to detect the concrete structure strength because of its immediacy and reliability (<xref ref-type="bibr" rid="B12">Ge et al., 2020</xref>). In this approach, cylindrical specimens with a diameter of 100 mm are drilled from a concrete structure and the compressive strength and splitting strength are tested. The Brazilian test is used to measure the tensile strength of concrete within the core-drilling method. The drilling position and number of samples is stipulated to ensure minimum damage to the concrete structure within the detection range (<xref ref-type="bibr" rid="B17">JGJ/T384-2016, 2016</xref>), which can be difficult. The drilled-core method has strict requirements on the height-diameter ratio, perpendicularity, and flatness of the end face of the cylindrical specimen, which increases the difficulty of drilling and specimen processing.</p>
<p>The following limitations are often encountered when using cylinder splitting to measure the tensile strength of concrete following the drilled-core method (<xref ref-type="bibr" rid="B17">JGJ/T384-2016, 2016</xref>). 1) Differing from cylindrical specimens made in the laboratory, cylindrical core specimens that are drilled on concrete structures often have variable lengths with uneven end faces. Cylinder core specimens must thus be processed prior to testing with a height-to-diameter ratio of 2. 2) Tensile strength data are often limited because each cylindrical core specimen has only one tensile strength value and concrete structures have a limited amount of available specimen owing to drill core damage (<xref ref-type="bibr" rid="B43">Wang et al., 2023</xref>). 3) Specialized skills, tools, and working conditions are required to obtain a complete concrete cylinder core. To improve this situation, <xref ref-type="bibr" rid="B53">Yuan et al. (2006)</xref> presented the cylinder transverse splitting method to test the splitting strength of concrete cylinder specimens. Differing from the Brazilian test, the load in the cylinder transverse splitting method is applied across the diameter and perpendicular to the central axis. The direction of the specimen bus bar is thus pulled, which results in splitting tensile failure of the cross-section (<xref ref-type="fig" rid="F2">Figure 2</xref>). The transverse splitting method has the following advantages: 1) increased amount of tensile strength data (a concrete cylinder specimen can be split multiple times); 2) reduced concrete core specimen processing procedure (the end of the concrete core specimen does not need to be cut and leveled); and 3) increased use ratio of the concrete core specimen (a specimen that is shorter than the minimum length specified in <xref ref-type="bibr" rid="B17">JGJ/T384-2016. (2016)</xref> can be tested).</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Cylinder transverse splitting method.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g002.tif"/>
</fig>
<p>
<xref ref-type="bibr" rid="B52">Yu et al. (2010)</xref> theoretically verified the rationality of multiple transverse cleavage rafting and concluded that higher specimen quantity improves the detection accuracy and reduces the confidence interval difference and upper limit of the variation coefficient. An experimental study by <xref ref-type="bibr" rid="B47">Xiao et al. (2011)</xref> showed that the splitting strength (detected by the cylinder transverse splitting method) of a concrete cylinder correlates well with the concrete compressive strength, and that the cylinder transverse splitting method can be used to more accurately and conveniently determine the concrete materiality than traditional core axial compression methods. <xref ref-type="bibr" rid="B54">Yuan et al. (2016)</xref> used a finite element model to analyze the rationality of the stress distribution on the transection of cylindrical concrete and found that the tensile failure of the transection depends on the cylinder&#x2019;s axial tensile stress.</p>
<p>Although the cylinder transverse splitting method has been shown to be feasible for testing the concrete tensile strength in many aspects (e.g., testing, mathematical statistics, finite element modeling), the cylinder transverse splitting strength is difficult to determine using a reasonable calculation formula. The cylinder transverse splitting strength was previously expressed by the nominal transverse splitting strength, <italic>P</italic>/<italic>A</italic>, where <italic>P</italic> is the failure load and <italic>A</italic> is the surface area cleavage. In this study, a strong correlation is found between the nominal transverse splitting strength of cylindrical concrete obtained by the cylinder transverse splitting method and the splitting strength of cubic concrete. A calculation formula to test the concrete tensile strength by the cylindrical transverse splitting method is established using the regression of a large number of experimental data. On the basis of previous tests, this study developed an improved specimen clamp for the cylinder transverse splitting method. In addition to normal concrete (NC), crumb rubber concrete (CRC) was also investigated to increase the amount of data and explore a wider range of concrete composition.</p>
<p>CRC is a new environmentally friendly concrete material made by the addition of rubber particles (e.g., crushed automobile tire waste) into ordinary concrete and has broad engineering application prospects (<xref ref-type="bibr" rid="B22">Lin et al., 2023</xref>). The rubber particles have a good elasticity, which can alleviate the stress concentration inside the concrete and reduce the probability of primary crack formation and concrete structural damage caused by an external load (<xref ref-type="bibr" rid="B51">Youssf et al., 2023</xref>). The addition of rubber particles to NC improves its crack resistance (<xref ref-type="bibr" rid="B21">Li et al., 2021</xref>; <xref ref-type="bibr" rid="B6">Elsayed et al., 2022</xref>; <xref ref-type="bibr" rid="B7">Feng et al., 2022</xref>), impact resistance (<xref ref-type="bibr" rid="B40">Topcu and Avcular, 1997</xref>), freeze-thaw durability (<xref ref-type="bibr" rid="B33">Savas et al., 1997</xref>; <xref ref-type="bibr" rid="B28">Paine and Dhir, 2002</xref>; <xref ref-type="bibr" rid="B20">Khan et al., 2021</xref>), abrasion resistance (<xref ref-type="bibr" rid="B15">Hang and Fan, 2011</xref>; <xref ref-type="bibr" rid="B37">Sun et al., 2021</xref>; <xref ref-type="bibr" rid="B55">Zhang et al., 2023</xref>), and reduces its elasticity modulus (<xref ref-type="bibr" rid="B16">Hernandez et al., 2002</xref>; <xref ref-type="bibr" rid="B3">Benazzouk et al., 2003</xref>; <xref ref-type="bibr" rid="B13">Haldar and Karmakar, 2021</xref>). Rubber particles can also reduce the concrete strength (<xref ref-type="bibr" rid="B49">Xu et al., 2020</xref>; <xref ref-type="bibr" rid="B48">Xu et al., 2021</xref>; <xref ref-type="bibr" rid="B14">Han et al., 2023</xref>). <xref ref-type="bibr" rid="B35">Segre et al. (2002)</xref> pointed out that zinc stearate tends to reduce the binding force between rubber particles and cement by infrared rays and chemical titration. Although <xref ref-type="bibr" rid="B34">Segre and Jocke (2000)</xref> found that rubber particles soaked in saturated NaOH solution for 20 min prior to mixing with the cement slurry improved the compressive strength, splitting strength, and bending strength of rubber cement mortar, they were unable to reach the strength level without the addition of rubber particles. The CRC tensile strength testing method must be thoroughly investigated to ensure engineering application safety (<xref ref-type="bibr" rid="B1">Adeboje et al., 2020</xref>).</p>
</sec>
<sec sec-type="materials|methods" id="s2">
<title>2 Materials and methods</title>
<sec id="s2-1">
<title>2.1 Materials</title>
<p>Ordinary Portland Cement 42.5 was used in this study and its properties are listed in <xref ref-type="table" rid="T1">Table 1</xref>. The coarse aggregates were limestone gravel and the fine aggregates were natural river sand and rubber particles of 1&#x2013;3 and 3&#x2013;6 mm, the latter of which were obtained by crushing scrap tires. The properties of the coarse and fine aggregates are listed in <xref ref-type="table" rid="T2">Table 2</xref>. The apparent density of the rubber particles is 1119 kg/m<sup>3</sup>. The grading curve of the fine aggregates and rubber particles is shown in <xref ref-type="fig" rid="F3">Figure 3</xref>. The indexes of the fine and coarse aggregates meet the requirements of <xref ref-type="bibr" rid="B8">GB/T14684-2011. (2011)</xref> and <xref ref-type="bibr" rid="B9">GB/T14685-2011. (2011)</xref>.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Cement properties.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th colspan="2" align="center">Setting time</th>
<th colspan="2" align="center">Compressive strength</th>
<th colspan="2" align="center">Flexural strength</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">Initial</td>
<td align="center">Final</td>
<td align="center">3 days</td>
<td align="center">28 days</td>
<td align="center">3d ays</td>
<td align="center">28 days</td>
</tr>
<tr>
<td align="center">169 min</td>
<td align="center">278 min</td>
<td align="center">21.5 MPa</td>
<td align="center">48.3 MPa</td>
<td align="center">5.4 MPa</td>
<td align="center">9.4 MPa</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Aggregate properties.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Material</th>
<th align="left">Size (mm)</th>
<th align="left">Apparent density (kg/m<sup>3</sup>)</th>
<th align="left">Mud content (%)</th>
<th align="left">Crushed index (%)</th>
<th align="left">Fineness modulus</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">coarse aggregates</td>
<td align="left">5&#x223c;20</td>
<td align="left">2710</td>
<td align="left">0.42</td>
<td align="left">9.3</td>
<td align="left">--</td>
</tr>
<tr>
<td align="left">aggregates</td>
<td align="left">0&#x223c;4.75</td>
<td align="left">2650</td>
<td align="left">1.5</td>
<td align="left">--</td>
<td align="left">2.7</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Grading curves of sand and rubber particles.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g003.tif"/>
</fig>
</sec>
<sec id="s2-2">
<title>2.2 Mixtures</title>
<p>Six water-cement ratios (W/C) were used, as listed in <xref ref-type="table" rid="T3">Table 3</xref>. The CRC was produced by partially replacing the fine aggregates with rubber particles in volumetric proportions of 1%, 3%, 5%, 10%, and 15% (<xref ref-type="table" rid="T4">Table 4</xref>). The samples covered a relevant concrete strength range that is commonly used in concrete engineering.</p>
<table-wrap id="T3" position="float">
<label>TABLE 3</label>
<caption>
<p>Mixture proportions of NC (kg/m<sup>3</sup>).</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Mixtures</th>
<th align="left">Water&#x2013;cement ratio</th>
<th align="left">Water</th>
<th align="left">Cement</th>
<th align="left">Crushed stones</th>
<th align="left">Sand</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">NC0.74</td>
<td align="left">0.74</td>
<td align="left">195</td>
<td align="left">262.4</td>
<td align="left">1197.3</td>
<td align="left">733.8</td>
</tr>
<tr>
<td align="left">NC0.62</td>
<td align="left">0.62</td>
<td align="left">195</td>
<td align="left">312.2</td>
<td align="left">1170.6</td>
<td align="left">717.5</td>
</tr>
<tr>
<td align="left">NC0.54</td>
<td align="left">0.54</td>
<td align="left">195</td>
<td align="left">362.1</td>
<td align="left">1143.8</td>
<td align="left">701.1</td>
</tr>
<tr>
<td align="left">NC0.42</td>
<td align="left">0.42</td>
<td align="left">195</td>
<td align="left">461.9</td>
<td align="left">1161.6</td>
<td align="left">598.4</td>
</tr>
<tr>
<td align="left">NC0.38</td>
<td align="left">0.38</td>
<td align="left">195</td>
<td align="left">511.7</td>
<td align="left">1133.1</td>
<td align="left">583.7</td>
</tr>
<tr>
<td align="left">NC0.35</td>
<td align="left">0.35</td>
<td align="left">195</td>
<td align="left">557.14</td>
<td align="left">1107.48</td>
<td align="left">570.52</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="T4" position="float">
<label>TABLE 4</label>
<caption>
<p>Mixture proportions of CRC (kg/m<sup>3</sup>).</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Mixtures</th>
<th align="left">Rubber content (%)</th>
<th align="left">Water&#x2013;cement ratio</th>
<th align="left">Water</th>
<th align="left">Cement</th>
<th align="left">Crushed stones</th>
<th align="left">Sand</th>
<th align="left">Rubber</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">CRC0.74-1</td>
<td rowspan="5" align="left">1</td>
<td align="left">0.74</td>
<td align="left">195</td>
<td align="left">262.4</td>
<td align="left">1197.3</td>
<td align="left">726.5</td>
<td align="left">3.00</td>
</tr>
<tr>
<td align="left">CRC0.54-1</td>
<td align="left">0.54</td>
<td align="left">195</td>
<td align="left">362.1</td>
<td align="left">1143.8</td>
<td align="left">694.1</td>
<td align="left">2.90</td>
</tr>
<tr>
<td align="left">CRC0.42-1</td>
<td align="left">0.42</td>
<td align="left">195</td>
<td align="left">461.9</td>
<td align="left">1161.6</td>
<td align="left">592.4</td>
<td align="left">2.48</td>
</tr>
<tr>
<td align="left">CRC0.38-1</td>
<td align="left">0.38</td>
<td align="left">195</td>
<td align="left">511.7</td>
<td align="left">1133.1</td>
<td align="left">577.9</td>
<td align="left">2.42</td>
</tr>
<tr>
<td align="left">CRC0.35-1</td>
<td align="left">0.35</td>
<td align="left">195</td>
<td align="left">557.14</td>
<td align="left">1107.48</td>
<td align="left">564.8</td>
<td align="left">2.36</td>
</tr>
<tr>
<td align="left">CRC0.74-3</td>
<td rowspan="5" align="left">3</td>
<td align="left">0.74</td>
<td align="left">195</td>
<td align="left">262.4</td>
<td align="left">1197.3</td>
<td align="left">711.8</td>
<td align="left">9.00</td>
</tr>
<tr>
<td align="left">CRC0.54-3</td>
<td align="left">0.54</td>
<td align="left">195</td>
<td align="left">362.1</td>
<td align="left">1143.8</td>
<td align="left">680</td>
<td align="left">8.71</td>
</tr>
<tr>
<td align="left">CRC0.42-3</td>
<td align="left">0.42</td>
<td align="left">195</td>
<td align="left">461.9</td>
<td align="left">1161.6</td>
<td align="left">580</td>
<td align="left">7.43</td>
</tr>
<tr>
<td align="left">CRC0.38-3</td>
<td align="left">0.38</td>
<td align="left">195</td>
<td align="left">511.7</td>
<td align="left">1133.1</td>
<td align="left">566.2</td>
<td align="left">7.25</td>
</tr>
<tr>
<td align="left">CRC0.35-3</td>
<td align="left">0.35</td>
<td align="left">195</td>
<td align="left">557.14</td>
<td align="left">1107.48</td>
<td align="left">553.4</td>
<td align="left">7.09</td>
</tr>
<tr>
<td align="left">CRC0.74-5</td>
<td rowspan="5" align="left">5</td>
<td align="left">0.74</td>
<td align="left">195</td>
<td align="left">262.4</td>
<td align="left">1197.3</td>
<td align="left">679.3</td>
<td align="left">15.00</td>
</tr>
<tr>
<td align="left">CRC0.54-5</td>
<td align="left">0.54</td>
<td align="left">195</td>
<td align="left">362.1</td>
<td align="left">1143.8</td>
<td align="left">666.1</td>
<td align="left">14.50</td>
</tr>
<tr>
<td align="left">CRC0.42-5</td>
<td align="left">0.42</td>
<td align="left">195</td>
<td align="left">461.9</td>
<td align="left">1161.6</td>
<td align="left">568.4</td>
<td align="left">12.40</td>
</tr>
<tr>
<td align="left">CRC0.38-5</td>
<td align="left">0.38</td>
<td align="left">195</td>
<td align="left">511.7</td>
<td align="left">1133.1</td>
<td align="left">554.7</td>
<td align="left">12.10</td>
</tr>
<tr>
<td align="left">CRC0.35-5</td>
<td align="left">0.35</td>
<td align="left">195</td>
<td align="left">557.14</td>
<td align="left">1107.48</td>
<td align="left">541.92</td>
<td align="left">11.80</td>
</tr>
<tr>
<td align="left">CRC0.74-10</td>
<td rowspan="5" align="left">10</td>
<td align="left">0.74</td>
<td align="left">195</td>
<td align="left">262.4</td>
<td align="left">1197.3</td>
<td align="left">660.8</td>
<td align="left">30.00</td>
</tr>
<tr>
<td align="left">CRC0.54-10</td>
<td align="left">0.54</td>
<td align="left">195</td>
<td align="left">362.1</td>
<td align="left">1143.8</td>
<td align="left">631.1</td>
<td align="left">29.00</td>
</tr>
<tr>
<td align="left">CRC0.42-10</td>
<td align="left">0.42</td>
<td align="left">195</td>
<td align="left">461.9</td>
<td align="left">1161.6</td>
<td align="left">538.4</td>
<td align="left">24.80</td>
</tr>
<tr>
<td align="left">CRC0.38-10</td>
<td align="left">0.38</td>
<td align="left">195</td>
<td align="left">511.7</td>
<td align="left">1133.1</td>
<td align="left">525.7</td>
<td align="left">24.20</td>
</tr>
<tr>
<td align="left">CRC0.35-10</td>
<td align="left">0.35</td>
<td align="left">195</td>
<td align="left">557.14</td>
<td align="left">1107.48</td>
<td align="left">513.3</td>
<td align="left">23.60</td>
</tr>
<tr>
<td align="left">CRC0.74-15</td>
<td rowspan="5" align="left">15</td>
<td align="left">0.74</td>
<td align="left">195</td>
<td align="left">262.4</td>
<td align="left">1197.3</td>
<td align="left">624.3</td>
<td align="left">45.00</td>
</tr>
<tr>
<td align="left">CRC0.54-15</td>
<td align="left">0.54</td>
<td align="left">195</td>
<td align="left">362.1</td>
<td align="left">1143.8</td>
<td align="left">596.1</td>
<td align="left">43.50</td>
</tr>
<tr>
<td align="left">CRC0.42-15</td>
<td align="left">0.42</td>
<td align="left">195</td>
<td align="left">461.9</td>
<td align="left">1161.6</td>
<td align="left">508.4</td>
<td align="left">37.20</td>
</tr>
<tr>
<td align="left">CRC0.38-15</td>
<td align="left">0.38</td>
<td align="left">195</td>
<td align="left">511.7</td>
<td align="left">1133.1</td>
<td align="left">496.7</td>
<td align="left">36.30</td>
</tr>
<tr>
<td align="left">CRC0.35-15</td>
<td align="left">0.35</td>
<td align="left">195</td>
<td align="left">557.14</td>
<td align="left">1107.48</td>
<td align="left">484.7</td>
<td align="left">35.40</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s2-3">
<title>2.3 Specimen preparation</title>
<p>Each mixture proportion contained cubic and cylindrical transverse splitting specimens. The specimens for testing the mechanical properties were prepared based on <xref ref-type="bibr" rid="B36">SL352-2006. (2006)</xref> and the number and size are listed in <xref ref-type="table" rid="T5">Table 5</xref>.</p>
<table-wrap id="T5" position="float">
<label>TABLE 5</label>
<caption>
<p>Specimen number and size for each group.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">Test</th>
<th align="center">Number</th>
<th align="center">Size</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">Standard cube splitting strength</td>
<td align="center">3</td>
<td align="center">150 mm &#xd7; 150 mm &#xd7; 150 mm</td>
</tr>
<tr>
<td align="center">Non-standard cylinder transverse splitting method</td>
<td align="center">3</td>
<td align="center">&#x2205; 100 mm &#xd7; 200 mm</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s2-4">
<title>2.4 Test method</title>
<sec id="s2-4-1">
<title>2.4.1 Finite element simulations</title>
<p>ANSYS software was used to simulate the transverse splitting tests of the concrete cylinders. The simulations included solid 65 as the concrete material, a sample size of &#x3a6;0.1 &#xd7; 0.1 m, elastic modulus of 30,000 MPa, and Poisson&#x2019;s ratio of 0.2. The constitutive relation adopts the Drucher-Prager model. The failure criterion is an improved William-Warnke five-parameter failure surface, which requires that the following parameters be defined: uniaxial tensile strength; uniaxial compression strength; biaxial compression strength; and uniaxial and biaxial compression strength under a certain confining pressure. Owing to the lack of multi-axis test parameters, ANSYS only requires uniaxial tensile strength and uniaxial compression strength input values, and the other parameters were calculated by the ANSYS default formula. The fracture opening shear transfer coefficient of concrete was 0.3, the fracture closing shear transfer coefficient was 0.9, and the uniaxial tensile strength was 3 MPa. Concrete crushing failure was not considered in the calculation. The remaining concrete parameters were set to the ANSYS default values. The parameters are selected according to the mechanical properties of the most common C30 concrete. The elastic modulus is about 30000 MPa, and the tensile strength is about 3 MPa (1/10 of the compressive strength). The shear stress transfer coefficient of open fissure in concrete is 0.3&#x2013;0.5, which is 0.3 in this paper. The shear stress transfer coefficient of closed cracks is 0.9&#x2013;1.0, which is 0.9 in this paper.</p>
</sec>
<sec id="s2-4-2">
<title>2.4.2 Cube splitting tests</title>
<p>Cube splitting tests were performed in accordance with <xref ref-type="bibr" rid="B36">SL352-2006. (2006)</xref>. The test instrument was a hydraulic universal testing machine with a maximum test force of 2000 kN. The experimental device is shown in <xref ref-type="fig" rid="F4">Figure 4</xref>, which includes a steel square filler strip with a cross-section of 5 &#xd7; 5 mm and length of 200 mm. To apply a linear uniform load on the concrete surface, the filler strip was placed between the concrete surface and pressure plate (<xref ref-type="bibr" rid="B39">Tang, 1994</xref>; <xref ref-type="bibr" rid="B31">Rocco et al., 2000</xref>; <xref ref-type="bibr" rid="B27">Olesen et al., 2006</xref>). The cube splitting strength of concrete was calculated according to:<disp-formula id="e1">
<mml:math id="m4">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mi>&#x3c0;</mml:mi>
<mml:msub>
<mml:mi>A</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.637</mml:mn>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>A</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>where <inline-formula id="inf4">
<mml:math id="m5">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the cube splitting strength (MPa), <inline-formula id="inf5">
<mml:math id="m6">
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the failure load (N), and <inline-formula id="inf6">
<mml:math id="m7">
<mml:mrow>
<mml:msub>
<mml:mi>A</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the cross-sectional area (mm<sup>2</sup>).</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Cube splitting test.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g004.tif"/>
</fig>
</sec>
<sec id="s2-4-3">
<title>2.4.3 Cylinder transverse splitting method</title>
<p>The setup used in the cylinder transverse splitting test is shown in <xref ref-type="fig" rid="F5">Figure 5</xref>. One of each of the upper and lower pressure plates of the hydraulic servo universal testing machine was used (<xref ref-type="fig" rid="F6">Figure 6</xref>). The test instrument was a hydraulic universal testing machine with a maximum test force of 1000 kN. The contact position with the concrete specimen was an anti-arc pressure cutter (equivalent of a filler strip) and the contact surface was 5-mm wide.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Schematic diagram of the test fixture: &#x2460; pressing plate; &#x2461; stiffening rib; &#x2462; pressure cutter; and &#x2463; connecting bolt.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g005.tif"/>
</fig>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>Setup installation.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g006.tif"/>
</fig>
<p>The cylinder transverse splitting test process was as follows. The cylinder specimens were cured in a standard curing room for 28 days and immediately tested after removing the surface moisture. A pencil was used to mark the circumference parallel to the specimen cross-section to determine the splitting position (<xref ref-type="fig" rid="F7">Figure 7A</xref>). The displacement boundary conditions of the cylinder specimens are related closely to the cylinder shape (<xref ref-type="bibr" rid="B18">Jia, 1997</xref>; <xref ref-type="bibr" rid="B19">Kanos et al., 2006</xref>; <xref ref-type="bibr" rid="B50">Yang and Li, 2002</xref>; <xref ref-type="bibr" rid="B56">Zhou et al., 2008</xref>; <xref ref-type="bibr" rid="B45">Wu et al., 2021</xref>) and the height-diameter ratio is the basic parameter that reflects the cylinder shape characteristics. <xref ref-type="bibr" rid="B54">Yuan et al. (2016)</xref> found that the transverse fracture failure load changed little with increasing specimen height when the cylinder height-diameter ratio was greater than or equal to 0.7 and is thus considered stable. The cylinder specimen could therefore be uniformly split three times. The height-diameter ratio was 2 in the first splitting and 1 in the second and third splittings (<xref ref-type="fig" rid="F7">Figure 7B</xref>). A vernier caliper was used to measure the cylinder diameter along the predetermined splitting position. The mean value of three measurements was taken as the effective specimen diameter to calculate the cross-sectional area <inline-formula id="inf7">
<mml:math id="m8">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">A</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. The sample was placed between the aligned upper and lower pressure knives according to the predetermined splitting position. The failure load <inline-formula id="inf8">
<mml:math id="m9">
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> was recorded at 0.04&#x2013;0.06 MPa/s.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Transverse splitting position of cylinder specimen (D &#x3d; 100 mm, L &#x3d; 200 mm, l &#x3d; 50 mm) <bold>(A)</bold>. The cylinder specimen could be uniformly split three times <bold>(B)</bold>.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g007.tif"/>
</fig>
<p>The cylinder nominal transverse strength of concrete is defined as:<disp-formula id="e2">
<mml:math id="m10">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>A</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(2)</label>
</disp-formula>where <inline-formula id="inf9">
<mml:math id="m11">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the nominal cylinder transverse strength (MPa), <inline-formula id="inf10">
<mml:math id="m12">
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the failure load (N), and <inline-formula id="inf11">
<mml:math id="m13">
<mml:mrow>
<mml:msub>
<mml:mi>A</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the cross-sectional area (mm<sup>2</sup>).</p>
</sec>
</sec>
</sec>
<sec sec-type="results|discussion" id="s3">
<title>3 Results and discussion</title>
<sec id="s3-1">
<title>3.1 Comparison of forces</title>
<p>In the cube splitting tests, an evenly distributed compression load was applied to the middle of the upper and lower surfaces of the concrete specimen (<xref ref-type="fig" rid="F8">Figure 8A</xref>). The compression load caused compressive stress in the axial surface of the concrete specimen (same plane as the load) and uniform tensile stress in most of the middle area (<xref ref-type="fig" rid="F8">Figure 8B</xref>). The fracture surface exhibited failure under tensile stress (<xref ref-type="fig" rid="F8">Figure 8C</xref>). The cylinder transverse splitting tests differed in that the cylinder specimen was uniformly loaded on the cross-sectional curve along the circumference (<xref ref-type="fig" rid="F9">Figure 9A</xref>). The load direction was the plumb direction, the same as in the cube splitting tests. The results from the ANSYS stress analysis show that the concrete specimen cross-section was under a state of tension and compression complex stress (<xref ref-type="fig" rid="F9">Figure 9B</xref>), whereas most of the central area was under a state of tension stress, which influences the splitting failure. The fracture surface performance is consistent with the stress analysis results (<xref ref-type="fig" rid="F9">Figure 9C</xref>), which indicates that the cylinder transverse splitting test can be used to effectively measure the concrete splitting strength.</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>In the cube splitting tests, an evenly distributed compression load was applied to the middle of the upper and lower surfaces of the concrete specimen <bold>(A)</bold>. The compression load caused compressive stress in the axial surface of the concrete specimen and uniform tensile stress in most of the middle area <bold>(B)</bold>. The fracture surface exhibited failure under tensile stress <bold>(C)</bold>.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g008.tif"/>
</fig>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>In the cylinder transverse splitting tests, the cylinder specimen was uniformly loaded on the cross-sectional curve along the circumference <bold>(A)</bold>. The concrete specimen cross-section was under a state of tension and compression complex stress <bold>(B)</bold>, whereas most of the central area was under a state of tension stress, which influences the splitting failure. The fracture surface performance is consistent with the stress analysis results <bold>(C)</bold>.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g009.tif"/>
</fig>
</sec>
<sec id="s3-2">
<title>3.2 Comparison of standard deviations</title>
<p>Three batches of cubic and cylindrical specimens of NC were made at different times (in 2011, 2014, and 2017) for the cube and cylinder transverse splitting tests. The standard deviation indicates the degree of data dispersion; smaller standard deviations reflect more concentrated data distributions. The relative precision of the test data can thus be explained by comparing the standard deviations obtained during the cylinder transverse splitting <italic>versus</italic> the cube splitting tensile failure loads. Each group of the second test (in 2014) consisted of three cubic and two cylindrical specimens and thus involved three cubic splitting tensile failure tests and six cylinder transverse splitting failure tests, as shown in <xref ref-type="table" rid="T6">Table 6</xref>. The standard deviation of the cylinder transverse splitting test results are generally smaller than those obtained from the cube splitting test results. The precision of the concrete tensile strength values obtained by the cylinder transverse splitting test is slightly higher than that of the cube splitting tests.</p>
<table-wrap id="T6" position="float">
<label>TABLE 6</label>
<caption>
<p>Test result.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">W/C</th>
<th colspan="4" align="center">0.75</th>
<th colspan="4" align="center">0.54</th>
</tr>
<tr>
<th align="center">Particle size and mixing amount of rubber</th>
<th align="center">Cube splitting tensile failure load</th>
<th align="center">Standard deviation</th>
<th align="center">Cylinder transverse splitting tensile failure load</th>
<th align="center">Standard deviation</th>
<th align="center">Cube splitting tensile failure load</th>
<th align="center">Standard deviation</th>
<th align="center">Cylinder transverse splitting tensile failure load</th>
<th align="center">Standard deviation</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td rowspan="6" align="center">NC</td>
<td align="center">48.07</td>
<td rowspan="3" align="center">10.10</td>
<td align="center">25.24</td>
<td rowspan="6" align="center">2.15</td>
<td align="center">90.46</td>
<td align="center">3.48</td>
<td align="center">13.19</td>
<td align="center">9.97</td>
</tr>
<tr>
<td align="center">70.74</td>
<td align="center">31.46</td>
<td align="center">88.42</td>
<td align="left"/>
<td align="center">41.92</td>
<td align="left"/>
</tr>
<tr>
<td align="center">68.00</td>
<td align="center">27.20</td>
<td align="center">96.61</td>
<td align="left"/>
<td align="center">34.92</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">27.77</td>
<td align="left"/>
<td align="left"/>
<td align="center">41.07</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">27.83</td>
<td align="left"/>
<td align="left"/>
<td align="center">37.75</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">30.89</td>
<td align="left"/>
<td align="left"/>
<td align="center">40.35</td>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">3&#x2013;6mm, 5%</td>
<td align="center">63.07</td>
<td rowspan="3" align="center">6.10</td>
<td align="center">28.65</td>
<td rowspan="6" align="center">3.85</td>
<td align="center">93.13</td>
<td align="center">3.67</td>
<td align="center">32.95</td>
<td align="center">4.24</td>
</tr>
<tr>
<td align="center">59.44</td>
<td align="center">37.66</td>
<td align="center">88.00</td>
<td align="left"/>
<td align="center">45.44</td>
<td align="left"/>
</tr>
<tr>
<td align="center">73.80</td>
<td align="center">27.40</td>
<td align="center">84.18</td>
<td align="left"/>
<td align="center">39.23</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">28.20</td>
<td align="left"/>
<td align="left"/>
<td align="center">33.07</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">25.89</td>
<td align="left"/>
<td align="left"/>
<td align="center">36.49</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">27.86</td>
<td align="left"/>
<td align="left"/>
<td align="center">38.16</td>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">3&#x2013;6mm, 10%</td>
<td align="center">53.59</td>
<td rowspan="3" align="center">6.80</td>
<td align="center">17.53</td>
<td rowspan="6" align="center">6.35</td>
<td align="center">85.70</td>
<td align="center">1.05</td>
<td align="center">33.26</td>
<td align="center">4.3</td>
</tr>
<tr>
<td align="center">61.15</td>
<td align="center">38.63</td>
<td align="center">83.17</td>
<td align="left"/>
<td align="center">43.89</td>
<td align="left"/>
</tr>
<tr>
<td align="center">70.23</td>
<td align="center">25.57</td>
<td align="center">84.81</td>
<td align="left"/>
<td align="center">39.21</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">23.10</td>
<td align="left"/>
<td align="left"/>
<td align="center">31.87</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">26.09</td>
<td align="left"/>
<td align="left"/>
<td align="center">36.86</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">27.95</td>
<td align="left"/>
<td align="left"/>
<td align="center">32.33</td>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">3&#x2013;6mm, 15%</td>
<td align="center">72.00</td>
<td rowspan="3" align="center">8.04</td>
<td align="center">20.79</td>
<td rowspan="6" align="center">2.39</td>
<td align="center">82.74</td>
<td align="center">4.31</td>
<td align="center">31.98</td>
<td align="center">2.98</td>
</tr>
<tr>
<td align="center">52.42</td>
<td align="center">28.07</td>
<td align="center">72.78</td>
<td align="left"/>
<td align="center">39.89</td>
<td align="left"/>
</tr>
<tr>
<td align="center">60.47</td>
<td align="center">23.29</td>
<td align="center">80.80</td>
<td align="left"/>
<td align="center">34.59</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">21.69</td>
<td align="left"/>
<td align="left"/>
<td align="center">32.59</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">24.90</td>
<td align="left"/>
<td align="left"/>
<td align="center">30.68</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">22.61</td>
<td align="left"/>
<td align="left"/>
<td align="center">32.78</td>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">1&#x2013;3mm, 5%</td>
<td align="center">59.61</td>
<td rowspan="3" align="center">4.04</td>
<td align="center">21.08</td>
<td rowspan="6" align="center">2.49</td>
<td align="center">83.15</td>
<td align="center">4.46</td>
<td align="center">24.08</td>
<td align="center">4.81</td>
</tr>
<tr>
<td align="center">67.23</td>
<td align="center">28.31</td>
<td align="center">83.15</td>
<td align="left"/>
<td align="center">38.16</td>
<td align="left"/>
</tr>
<tr>
<td align="center">57.95</td>
<td align="center">27.26</td>
<td align="center">92.61</td>
<td align="left"/>
<td align="center">36.28</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">27.15</td>
<td align="left"/>
<td align="left"/>
<td align="center">37.55</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">27.81</td>
<td align="left"/>
<td align="left"/>
<td align="center">36.57</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">24.81</td>
<td align="left"/>
<td align="left"/>
<td align="center">34.15</td>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">1&#x2013;3mm, 10%</td>
<td align="center">62.33</td>
<td rowspan="3" align="center">4.11</td>
<td align="center">17.15</td>
<td rowspan="6" align="center">2.49</td>
<td align="center">78.59</td>
<td align="center">2.30</td>
<td align="center">28.77</td>
<td align="center">2.28</td>
</tr>
<tr>
<td align="center">56.88</td>
<td align="center">24.09</td>
<td align="center">80.16</td>
<td align="left"/>
<td align="center">35.93</td>
<td align="left"/>
</tr>
<tr>
<td align="center">52.28</td>
<td align="center">24.01</td>
<td align="center">84.05</td>
<td align="left"/>
<td align="center">32.92</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">23.08</td>
<td align="left"/>
<td align="left"/>
<td align="center">35.14</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">24.37</td>
<td align="left"/>
<td align="left"/>
<td align="center">32.56</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">22.50</td>
<td align="left"/>
<td align="left"/>
<td align="center">33.16</td>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">1&#x2013;3mm, 15%</td>
<td align="center">53.11</td>
<td rowspan="3" align="center">1.04</td>
<td align="center">14.29</td>
<td rowspan="6" align="center">2.58</td>
<td align="center">83.23</td>
<td align="center">4.43</td>
<td align="center">28.10</td>
<td align="center">1.93</td>
</tr>
<tr>
<td align="center">50.70</td>
<td align="center">18.51</td>
<td align="center">79.14</td>
<td align="left"/>
<td align="center">33.48</td>
<td align="left"/>
</tr>
<tr>
<td align="center">51.19</td>
<td align="center">22.12</td>
<td align="center">72.48</td>
<td align="left"/>
<td align="center">29.63</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">21.60</td>
<td align="left"/>
<td align="left"/>
<td align="center">32.15</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">19.61</td>
<td align="left"/>
<td align="left"/>
<td align="center">33.28</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">20.34</td>
<td align="left"/>
<td align="left"/>
<td align="center">31.30</td>
<td align="left"/>
</tr>
</tbody>
</table>
<table>
<thead valign="top">
<tr>
<th align="center">W/C</th>
<th colspan="4" align="center">0.42</th>
<th colspan="4" align="center">0.38</th>
</tr>
<tr>
<th align="center">Particle size and mixing amount of rubber</th>
<th align="center">Split tensile failure load of cube</th>
<th align="center">standard deviation</th>
<th align="center">transverse Split tensile failure load of cylinder</th>
<th align="center">standard deviation</th>
<th align="center">Split tensile failure load of cube</th>
<th align="center">standard deviation</th>
<th align="center">transverse Split tensile failure load of cylinder</th>
<th align="center">standard deviation</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td rowspan="6" align="center">NC</td>
<td align="center">102.06</td>
<td rowspan="3" align="center">4.92</td>
<td align="center">45.96</td>
<td rowspan="6" align="center">3.18</td>
<td align="center">133.99</td>
<td align="center">7.01</td>
<td align="center">48.44</td>
<td align="center">3.87</td>
</tr>
<tr>
<td align="center">108.71</td>
<td align="center">54.59</td>
<td align="center">116.91</td>
<td align="left"/>
<td align="center">59.16</td>
<td align="left"/>
</tr>
<tr>
<td align="center">114.1</td>
<td align="center">45.65</td>
<td align="center">124.01</td>
<td align="left"/>
<td align="center">52.81</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">47.27</td>
<td align="left"/>
<td align="left"/>
<td align="center">56.8</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">45.42</td>
<td align="left"/>
<td align="left"/>
<td align="center">55.18</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">46.92</td>
<td align="left"/>
<td align="left"/>
<td align="center">49.25</td>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">3&#x2013;6mm, 5%</td>
<td align="center">107.49</td>
<td rowspan="3" align="center">4.41</td>
<td align="center">37.58</td>
<td rowspan="6" align="center">5.81</td>
<td align="center">122.75</td>
<td align="center">3.22</td>
<td align="center">49.11</td>
<td align="center">2.46</td>
</tr>
<tr>
<td align="center">99.8</td>
<td align="center">56.35</td>
<td align="center">123.21</td>
<td align="left"/>
<td align="center">57</td>
<td align="left"/>
</tr>
<tr>
<td align="center">110.23</td>
<td align="center">45.94</td>
<td align="center">116.17</td>
<td align="left"/>
<td align="center">52.06</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">43.16</td>
<td align="left"/>
<td align="left"/>
<td align="center">50.41</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">42.02</td>
<td align="left"/>
<td align="left"/>
<td align="center">52.96</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">47.62</td>
<td align="left"/>
<td align="left"/>
<td align="center">51.95</td>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">3&#x2013;6mm, 10%</td>
<td align="center">106.14</td>
<td rowspan="3" align="center">5.73</td>
<td align="center">46.02</td>
<td rowspan="6" align="center">5.67</td>
<td align="center">85.70</td>
<td align="center">3.06</td>
<td align="center">43.96</td>
<td align="center">7.39</td>
</tr>
<tr>
<td align="center">101.56</td>
<td align="center">56.98</td>
<td align="center">83.17</td>
<td align="left"/>
<td align="center">66.39</td>
<td align="left"/>
</tr>
<tr>
<td align="center">92.37</td>
<td align="center">43.34</td>
<td align="center">84.81</td>
<td align="left"/>
<td align="center">50.03</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">44.27</td>
<td align="left"/>
<td align="left"/>
<td align="center">46.49</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">40.51</td>
<td align="left"/>
<td align="left"/>
<td align="center">48.34</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">39.98</td>
<td align="left"/>
<td align="left"/>
<td align="center">47.16</td>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">3&#x2013;6mm, 15%</td>
<td align="center">80.46</td>
<td rowspan="3" align="center">8.04</td>
<td align="center">40.94</td>
<td rowspan="6" align="center">6.23</td>
<td align="center">110.43</td>
<td align="center">5.96</td>
<td align="center">38.59</td>
<td align="center">7.63</td>
</tr>
<tr>
<td align="center">96.78</td>
<td align="center">57.3</td>
<td align="center">96.26</td>
<td align="left"/>
<td align="center">61.51</td>
<td align="left"/>
</tr>
<tr>
<td align="center">98.18</td>
<td align="center">40.64</td>
<td align="center">100.34</td>
<td align="left"/>
<td align="center">45.97</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">41.83</td>
<td align="left"/>
<td align="left"/>
<td align="center">41.26</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">40.65</td>
<td align="left"/>
<td align="left"/>
<td align="center">44.26</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">39.43</td>
<td align="left"/>
<td align="left"/>
<td align="center">40.4</td>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">1&#x2013;3mm, 5%</td>
<td align="center">109.46</td>
<td rowspan="3" align="center">5.42</td>
<td align="center">39.34</td>
<td rowspan="6" align="center">5.92</td>
<td align="center">123.14</td>
<td align="center">9.26</td>
<td align="center">51.71</td>
<td align="center">2.71</td>
</tr>
<tr>
<td align="center">106.56</td>
<td align="center">58.04</td>
<td align="center">102.16</td>
<td align="left"/>
<td align="center">58.77</td>
<td align="left"/>
</tr>
<tr>
<td align="center">96.78</td>
<td align="center">45.68</td>
<td align="center">120.09</td>
<td align="left"/>
<td align="center">51.63</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">42.4</td>
<td align="left"/>
<td align="left"/>
<td align="center">50.61</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">43.09</td>
<td align="left"/>
<td align="left"/>
<td align="center">52.69</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">46.15</td>
<td align="left"/>
<td align="left"/>
<td align="center">51.81</td>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">1&#x2013;3mm, 10%</td>
<td align="center">98.51</td>
<td rowspan="3" align="center">1.91</td>
<td align="center">34.98</td>
<td rowspan="6" align="center">4.44</td>
<td align="center">118.06</td>
<td align="center">7.58</td>
<td align="center">42.66</td>
<td align="center">6.21</td>
</tr>
<tr>
<td align="center">100.94</td>
<td align="center">47.76</td>
<td align="center">110.24</td>
<td align="left"/>
<td align="center">61.37</td>
<td align="left"/>
</tr>
<tr>
<td align="center">103.18</td>
<td align="center">43.88</td>
<td align="center">99.56</td>
<td align="left"/>
<td align="center">47.6</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">45.47</td>
<td align="left"/>
<td align="left"/>
<td align="center">49.68</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">39.7</td>
<td align="left"/>
<td align="left"/>
<td align="center">45.11</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">38.03</td>
<td align="left"/>
<td align="left"/>
<td align="center">44.24</td>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">1&#x2013;3mm, 15%</td>
<td align="center">102.32</td>
<td rowspan="3" align="center">4.92</td>
<td align="center">26.73</td>
<td rowspan="6" align="center">5.07</td>
<td align="center">103.98</td>
<td align="center">7.01</td>
<td align="center">34.53</td>
<td align="center">4.56</td>
</tr>
<tr>
<td align="center">90.36</td>
<td align="center">39.35</td>
<td align="center">107.27</td>
<td align="left"/>
<td align="center">47.76</td>
<td align="left"/>
</tr>
<tr>
<td align="center">95.02</td>
<td align="center">38.2</td>
<td align="center">91.04</td>
<td align="left"/>
<td align="center">40.21</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">40.24</td>
<td align="left"/>
<td align="left"/>
<td align="center">39.05</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">40.42</td>
<td align="left"/>
<td align="left"/>
<td align="center">42.09</td>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">41.83</td>
<td align="left"/>
<td align="left"/>
<td align="center">46.9</td>
<td align="left"/>
</tr>
</tbody>
</table>
<table>
<thead valign="top">
<tr>
<th align="center">W/C</th>
<th colspan="4" align="center">0.35</th>
<th colspan="4" align="left"/>
</tr>
<tr>
<th align="center">Particle size and mixing amount of rubber</th>
<th align="center">Split tensile failure load of cube</th>
<th align="center">standard deviation</th>
<th align="center">transverse Split tensile failure load of cylinder</th>
<th align="center">standard deviation</th>
<th align="left"/>
<th align="left"/>
<th align="left"/>
<th align="left"/>
</tr>
</thead>
<tbody valign="top">
<tr>
<td rowspan="6" align="center">NC</td>
<td align="center">133</td>
<td rowspan="3" align="center">3.22</td>
<td align="center">51.01</td>
<td rowspan="6" align="center">5.03</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">140.19</td>
<td align="center">65.18</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">133.78</td>
<td align="center">62.96</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">58.16</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">60.09</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">53.13</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">3&#x2013;6mm, 5%</td>
<td align="center">137.69</td>
<td rowspan="3" align="center">4.55</td>
<td align="center">44.15</td>
<td rowspan="6" align="center">6.39</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">129.67</td>
<td align="center">62.93</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">126.98</td>
<td align="center">56.98</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">57.08</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">61.87</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">51.47</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">3&#x2013;6mm, 10%</td>
<td align="center">127.91</td>
<td rowspan="3" align="center">20.47</td>
<td align="center">44.13</td>
<td rowspan="6" align="center">5.64</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">93.47</td>
<td align="center">62.58</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">142.24</td>
<td align="center">51.13</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">54.33</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">48.66</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">52.04</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">3&#x2013;6mm, 15%</td>
<td align="center">111.45</td>
<td rowspan="3" align="center">13.31</td>
<td align="center">42.92</td>
<td rowspan="6" align="center">7.71</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">104.12</td>
<td align="center">65.74</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">80.27</td>
<td align="center">46.26</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">44.31</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">46.03</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">50.25</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">1&#x2013;3mm, 5%</td>
<td align="center">126.67</td>
<td rowspan="3" align="center">4.88</td>
<td align="center">46.88</td>
<td rowspan="6" align="center">3.42</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">131.63</td>
<td align="center">56.21</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">119.72</td>
<td align="center">55.92</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">54.38</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">53.93</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">57.3</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">1&#x2013;3mm, 10%</td>
<td align="center">97.12</td>
<td rowspan="3" align="center">12.39</td>
<td align="center">42.91</td>
<td rowspan="6" align="center">5.73</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">115.53</td>
<td align="center">57.48</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">127.21</td>
<td align="center">43.65</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">48.19</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">53.14</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">56.14</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td rowspan="6" align="center">1&#x2013;3mm, 15%</td>
<td align="center">105.45</td>
<td rowspan="3" align="center">1.34</td>
<td align="center">40.72</td>
<td rowspan="6" align="center">5.01</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">108.37</td>
<td align="center">53.52</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="center">105.63</td>
<td align="center">44.65</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">44.95</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">40.71</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
<tr>
<td align="left"/>
<td align="left"/>
<td align="center">51.94</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s3-3">
<title>3.3 NC splitting strength</title>
<p>The cube splitting strength and cylinder nominal transverse splitting strength of the NC show similar negative dependencies with W/C (<xref ref-type="fig" rid="F10">Figure 10</xref>), which is in agreement with the W/C law of Abrams. The cylinder nominal transverse splitting strength is found to be higher than the cube splitting strength for concrete with the same W/C. These results are in agreement with previous studies (<xref ref-type="bibr" rid="B24">Malhotra, 1970</xref>; <xref ref-type="bibr" rid="B15">Hang and Fan, 2011</xref>) mainly because of the size effect.</p>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>Relationship between splitting strength (NC) and W/C: First batch <bold>(A)</bold>; Second batch <bold>(B)</bold>; Third batch <bold>(C)</bold>.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g010.tif"/>
</fig>
</sec>
<sec id="s3-4">
<title>3.4 CRC splitting strength</title>
<p>Similar to NC, the cube splitting strength and cylinder nominal transverse splitting strength of CRC decrease with increasing W/C (<xref ref-type="fig" rid="F11">Figure 11</xref>) and show the same trend regardless of the rubber particle size (3&#x2013;6 or 1&#x2013;3 mm) or rubber particle content (5%, 10%, or 15%). This regularity shows no correlation with rubber particle size and content. The samples with 1% and 3% rubber particle contents show the same behavior and are not discussed further.</p>
<fig id="F11" position="float">
<label>FIGURE 11</label>
<caption>
<p>Relationship between splitting strength (CRC) and W/C: CRC with 5% rubber particles (3&#x2013;6&#x00a0;mm) <bold>(A)</bold>; CRC with 5% rubber particles (1&#x2013;3&#x00a0;mm) <bold>(B)</bold>; CRC with 10% rubber particles (3&#x2013;6&#x00a0;mm) <bold>(C)</bold>; CRC with 10% rubber particles (1&#x2013;3&#x00a0;mm) <bold>(D)</bold>; CRC with 15% rubber particles (3&#x2013;6&#x00a0;mm) <bold>(E)</bold>; CRC with 15% rubber particles (1&#x2013;3&#x00a0;mm) <bold>(F)</bold>.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g011.tif"/>
</fig>
<p>As shown in <xref ref-type="fig" rid="F12">Figure 12</xref>, regardless of rubber particle size (3&#x2013;6 or 1&#x2013;3 mm) and W/C (0.35, 0.42, or 0.74), the cube splitting strength and cylinder nominal transverse splitting strength both consistently decrease with increasing rubber particle content. This is mainly because the rubber particle strength is far less than the sand strength, and the bond strength between the rubber and cement is far less than the bond strength between the sand and cement. The samples with 0.38 and 0.54 W/C show the same behavior and are not discussed here. The influence of rubber particle content on concrete strength is similar to previous results (<xref ref-type="bibr" rid="B5">Eldin and Senouci, 1993</xref>; <xref ref-type="bibr" rid="B41">Topcu, 1995</xref>; <xref ref-type="bibr" rid="B42">Toutanji, 1996</xref>; <xref ref-type="bibr" rid="B2">Ali et al., 2000</xref>). For the same rubber particle content, the cylinder nominal transverse splitting strength is higher than the cube splitting strength.</p>
<fig id="F12" position="float">
<label>FIGURE 12</label>
<caption>
<p>Relationship between splitting strength (CRC) and content of rubber particles: CRC with 0.35W/C and rubber particles 3&#x223c;6&#x00a0;mm <bold>(A)</bold>; CRC with 0.35W/C and rubber particles 1&#x223c;3&#x00a0;mm <bold>(B)</bold>; CRC with 0.42W/C and rubber particles 3&#x223c;6&#x00a0;mm <bold>(C)</bold>; CRC with 0.42W/C and rubber particles 1&#x223c;3&#x00a0;mm <bold>(D)</bold>; CRC with 0.74W/C and rubber particles 3&#x223c;6&#x00a0;mm <bold>(E)</bold>; CRC with 0.74W/C and rubber particles 1&#x223c;3&#x00a0;mm <bold>(F)</bold>.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g012.tif"/>
</fig>
<p>On the basis of the above analysis, the cylinder nominal transverse splitting strength can be used to represent the concrete tensile strength, similar to the cube splitting strength.</p>
</sec>
<sec id="s3-5">
<title>3.5 Relationship between cube and cylinder nominal transverse splitting strength</title>
<p>The cube splitting strength is given in <xref ref-type="bibr" rid="B36">SL352-2006. (2006)</xref> as Eq. <xref ref-type="disp-formula" rid="e1">1</xref>. The concrete splitting surface has a similar stress distribution under the condition of cylinder transverse and cube splitting (<xref ref-type="fig" rid="F8">Figure 8B</xref>; <xref ref-type="fig" rid="F9">Figure 9B</xref>). The cylinder transverse splitting strength is assumed to follow a formula in the same form as the cube splitting strength, namely:<disp-formula id="e3">
<mml:math id="m14">
<mml:mrow>
<mml:msubsup>
<mml:mi>f</mml:mi>
<mml:mn>2</mml:mn>
<mml:mo>&#x2032;</mml:mo>
</mml:msubsup>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>&#x3b3;</mml:mi>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>A</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(3)</label>
</disp-formula>where <inline-formula id="inf12">
<mml:math id="m15">
<mml:mrow>
<mml:msubsup>
<mml:mi>f</mml:mi>
<mml:mn>2</mml:mn>
<mml:mo>&#x2032;</mml:mo>
</mml:msubsup>
</mml:mrow>
</mml:math>
</inline-formula> is the cylinder transverse splitting strength (MPa) and <inline-formula id="inf13">
<mml:math id="m16">
<mml:mrow>
<mml:mi>&#x3b3;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> is the coefficient of stress distribution. The results show that an internal relationship exists between the cube and cylinder transverse splitting strengths for concrete:<disp-formula id="e4">
<mml:math id="m17">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>&#x3b2;</mml:mi>
<mml:msubsup>
<mml:mi>f</mml:mi>
<mml:mn>2</mml:mn>
<mml:mo>&#x2032;</mml:mo>
</mml:msubsup>
</mml:mrow>
</mml:math>
<label>(4)</label>
</disp-formula>where <inline-formula id="inf14">
<mml:math id="m18">
<mml:mrow>
<mml:mi>&#x3b2;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> is the coefficient related to the specimen size. Combined with Eq. <xref ref-type="disp-formula" rid="e1">1</xref> and Eq. <xref ref-type="disp-formula" rid="e2">2</xref>, Eq. <xref ref-type="disp-formula" rid="e3">3</xref>, Eq. <xref ref-type="disp-formula" rid="e4">4</xref>, we obtain:<disp-formula id="e5">
<mml:math id="m19">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>&#x3b2;</mml:mi>
<mml:mi>&#x3b3;</mml:mi>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>A</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>&#x3b2;</mml:mi>
<mml:mi>&#x3b3;</mml:mi>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
<label>(5)</label>
</disp-formula>
</p>
<p>For <inline-formula id="inf15">
<mml:math id="m20">
<mml:mrow>
<mml:mi>&#x3c8;</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>&#x3b2;</mml:mi>
<mml:mi>&#x3b3;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>, the relational expression between the cube and cylinder nominal transverse splitting strength is:<disp-formula id="e6">
<mml:math id="m21">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>&#x3c8;</mml:mi>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
<label>(6)</label>
</disp-formula>
</p>
<p>The linear fitting results (that pass through the origin) of Eq. <xref ref-type="disp-formula" rid="e6">6</xref> are shown in <xref ref-type="fig" rid="F13">Figure 13</xref>. The <inline-formula id="inf16">
<mml:math id="m22">
<mml:mrow>
<mml:mi>&#x3c8;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> of NC (0.50; <xref ref-type="fig" rid="F13">Figure 13A</xref>) differs slightly from that of the CRC (0.50 in <xref ref-type="fig" rid="F13">Figure 13B</xref>, 0.53 in <xref ref-type="fig" rid="F13">Figure 13C</xref>), which indicates that the incorporation of rubber particles into NC has only a small effect on <inline-formula id="inf17">
<mml:math id="m23">
<mml:mrow>
<mml:mi>&#x3c8;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>. The slight difference in <inline-formula id="inf18">
<mml:math id="m24">
<mml:mrow>
<mml:mi>&#x3c8;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> between CRC with 3&#x2013;6 mm (0.50, <xref ref-type="fig" rid="F13">Figure 13B</xref>) and 1&#x2013;3 mm rubber particles (0.53, <xref ref-type="fig" rid="F13">Figure 13C</xref>) shows that the effect of rubber particle size on <inline-formula id="inf19">
<mml:math id="m25">
<mml:mrow>
<mml:mi>&#x3c8;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> is small. When all of the data are combined, <inline-formula id="inf20">
<mml:math id="m26">
<mml:mrow>
<mml:mi>&#x3c8;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> &#x3d; 0.53 with an R<sup>2</sup> (correlation coefficient) of 0.994 (<xref ref-type="fig" rid="F13">Figure 13D</xref>).</p>
<fig id="F13" position="float">
<label>FIGURE 13</label>
<caption>
<p>Linear fitting of Ep. (6): NC <bold>(A)</bold>; CRC (3&#x2013;6&#x00a0;mm rubber particles) <bold>(B)</bold>; CRC (1&#x2013;3&#x00a0;mm rubber particles) <bold>(C)</bold>; All concrete <bold>(D)</bold>.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g013.tif"/>
</fig>
<p>An insertion of the value of <inline-formula id="inf21">
<mml:math id="m27">
<mml:mrow>
<mml:mi mathvariant="normal">&#x3c8;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> into Eq. <xref ref-type="disp-formula" rid="e6">6</xref> yields:<disp-formula id="e7">
<mml:math id="m28">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.53</mml:mn>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
<label>(7)</label>
</disp-formula>
</p>
<p>The test value is compared to the calculated value.</p>
<p>The calculated <inline-formula id="inf22">
<mml:math id="m29">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> values from Eq. <xref ref-type="disp-formula" rid="e7">7</xref> and test value <inline-formula id="inf23">
<mml:math id="m30">
<mml:mrow>
<mml:msubsup>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
<mml:mo>&#x2032;</mml:mo>
</mml:msubsup>
</mml:mrow>
</mml:math>
</inline-formula> are shown in <xref ref-type="table" rid="T7">Table 7</xref>. There are 17 data sets for NC and 54 data sets for CRC (27 for 3&#x2013;6 mm CRC and 27 for 1&#x2013;3 mm CRC) for a total of 71 data sets. Among the 71 data sets, the ratios of the calculated values <inline-formula id="inf24">
<mml:math id="m31">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">f</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> to test value <inline-formula id="inf25">
<mml:math id="m32">
<mml:mrow>
<mml:msubsup>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
<mml:mo>&#x2032;</mml:mo>
</mml:msubsup>
</mml:mrow>
</mml:math>
</inline-formula> gives a minimum of 0.80, maximum of 1.34, mean of 0.99, and mean square error of 0.087. The ratios are relatively centralized and concentrated around 1.00, as shown in <xref ref-type="fig" rid="F14">Figure 14</xref>. The cube splitting strength calculated by the cylinder nominal transverse splitting strength via Eq. <xref ref-type="disp-formula" rid="e7">7</xref> is similar to that obtained by the cube splitting test.</p>
<table-wrap id="T7" position="float">
<label>TABLE 7</label>
<caption>
<p>Calculated and test splitting strengths of concrete.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Concrete</th>
<th colspan="4" align="left">NC</th>
<th colspan="4" align="left">3&#x2013;6 mm CRC</th>
<th colspan="4" align="left">1&#x2013;3 mm CRC</th>
<th rowspan="2" align="left">
<inline-formula id="inf26">
<mml:math id="m33">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mo>/</mml:mo>
<mml:msubsup>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
<mml:mo>&#x2032;</mml:mo>
</mml:msubsup>
</mml:mrow>
</mml:math>
</inline-formula>
<break/>Mean value</th>
<th rowspan="2" align="left">Mean square error</th>
</tr>
<tr>
<th align="left">Sequence Number</th>
<th align="left">
<inline-formula id="inf27">
<mml:math id="m34">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>
</th>
<th align="left">
<inline-formula id="inf28">
<mml:math id="m35">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>
</th>
<th align="left">
<inline-formula id="inf29">
<mml:math id="m36">
<mml:mrow>
<mml:msubsup>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
<mml:mo>&#x2032;</mml:mo>
</mml:msubsup>
</mml:mrow>
</mml:math>
</inline-formula>
</th>
<th align="left">
<inline-formula id="inf30">
<mml:math id="m37">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mo>/</mml:mo>
<mml:msubsup>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
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<th align="left">
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<mml:math id="m44">
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<mml:msubsup>
<mml:mi>f</mml:mi>
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<th align="left">
<inline-formula id="inf38">
<mml:math id="m45">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
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</thead>
<tbody valign="top">
<tr>
<td align="left">1</td>
<td align="left">4.02</td>
<td align="left">2.04</td>
<td align="left">1.80</td>
<td align="left">1.13</td>
<td align="left">3.78</td>
<td align="left">1.94</td>
<td align="left">1.83</td>
<td align="left">1.06</td>
<td align="left">3.63</td>
<td align="left">1.84</td>
<td align="left">2.05</td>
<td align="left">0.90</td>
<td rowspan="27" align="left">0.99</td>
<td rowspan="27" align="left">0.087</td>
</tr>
<tr>
<td align="left">2</td>
<td align="left">5.32</td>
<td align="left">2.70</td>
<td align="left">2.43</td>
<td align="left">1.11</td>
<td align="left">4.99</td>
<td align="left">2.55</td>
<td align="left">2.65</td>
<td align="left">0.96</td>
<td align="left">4.34</td>
<td align="left">2.19</td>
<td align="left">2.58</td>
<td align="left">0.85</td>
</tr>
<tr>
<td align="left">3</td>
<td align="left">5.63</td>
<td align="left">2.86</td>
<td align="left">2.79</td>
<td align="left">1.03</td>
<td align="left">5.86</td>
<td align="left">3.01</td>
<td align="left">2.92</td>
<td align="left">1.03</td>
<td align="left">5.40</td>
<td align="left">2.75</td>
<td align="left">2.53</td>
<td align="left">1.09</td>
</tr>
<tr>
<td align="left">4</td>
<td align="left">6.21</td>
<td align="left">3.16</td>
<td align="left">2.97</td>
<td align="left">1.06</td>
<td align="left">6.13</td>
<td align="left">3.11</td>
<td align="left">3.16</td>
<td align="left">0.98</td>
<td align="left">6.33</td>
<td align="left">3.21</td>
<td align="left">3.15</td>
<td align="left">1.02</td>
</tr>
<tr>
<td align="left">5</td>
<td align="left">7.19</td>
<td align="left">3.67</td>
<td align="left">3.15</td>
<td align="left">1.17</td>
<td align="left">6.51</td>
<td align="left">3.32</td>
<td align="left">3.32</td>
<td align="left">1.00</td>
<td align="left">6.42</td>
<td align="left">3.26</td>
<td align="left">3.65</td>
<td align="left">0.89</td>
</tr>
<tr>
<td align="left">6</td>
<td align="left">6.99</td>
<td align="left">3.57</td>
<td align="left">3.78</td>
<td align="left">0.94</td>
<td align="left">7.40</td>
<td align="left">3.77</td>
<td align="left">4.00</td>
<td align="left">0.94</td>
<td align="left">6.92</td>
<td align="left">3.52</td>
<td align="left">3.71</td>
<td align="left">0.95</td>
</tr>
<tr>
<td align="left">7</td>
<td align="left">3.62</td>
<td align="left">1.84</td>
<td align="left">1.93</td>
<td align="left">0.95</td>
<td align="left">4.23</td>
<td align="left">2.14</td>
<td align="left">2.39</td>
<td align="left">0.90</td>
<td align="left">3.99</td>
<td align="left">2.04</td>
<td align="left">2.34</td>
<td align="left">0.87</td>
</tr>
<tr>
<td align="left">8</td>
<td align="left">4.44</td>
<td align="left">2.24</td>
<td align="left">2.60</td>
<td align="left">0.86</td>
<td align="left">4.50</td>
<td align="left">2.30</td>
<td align="left">1.72</td>
<td align="left">1.34</td>
<td align="left">3.90</td>
<td align="left">1.99</td>
<td align="left">2.49</td>
<td align="left">0.80</td>
</tr>
<tr>
<td align="left">9</td>
<td align="left">6.07</td>
<td align="left">3.11</td>
<td align="left">3.10</td>
<td align="left">1.00</td>
<td align="left">5.72</td>
<td align="left">2.91</td>
<td align="left">2.63</td>
<td align="left">1.11</td>
<td align="left">5.10</td>
<td align="left">2.60</td>
<td align="left">2.76</td>
<td align="left">0.94</td>
</tr>
<tr>
<td align="left">10</td>
<td align="left">6.83</td>
<td align="left">3.47</td>
<td align="left">3.50</td>
<td align="left">0.99</td>
<td align="left">6.00</td>
<td align="left">3.06</td>
<td align="left">3.00</td>
<td align="left">1.02</td>
<td align="left">6.02</td>
<td align="left">3.06</td>
<td align="left">2.82</td>
<td align="left">1.09</td>
</tr>
<tr>
<td align="left">11</td>
<td align="left">7.44</td>
<td align="left">3.77</td>
<td align="left">3.80</td>
<td align="left">0.99</td>
<td align="left">7.54</td>
<td align="left">3.83</td>
<td align="left">3.50</td>
<td align="left">1.09</td>
<td align="left">6.23</td>
<td align="left">3.16</td>
<td align="left">2.87</td>
<td align="left">1.10</td>
</tr>
<tr>
<td align="left">12</td>
<td align="left">4.09</td>
<td align="left">2.09</td>
<td align="left">2.37</td>
<td align="left">0.88</td>
<td align="left">7.02</td>
<td align="left">3.57</td>
<td align="left">3.70</td>
<td align="left">0.96</td>
<td align="left">6.60</td>
<td align="left">3.37</td>
<td align="left">3.49</td>
<td align="left">0.97</td>
</tr>
<tr>
<td align="left">13</td>
<td align="left">4.80</td>
<td align="left">2.45</td>
<td align="left">2.53</td>
<td align="left">0.97</td>
<td align="left">3.73</td>
<td align="left">1.89</td>
<td align="left">1.85</td>
<td align="left">1.02</td>
<td align="left">3.32</td>
<td align="left">1.68</td>
<td align="left">1.71</td>
<td align="left">0.98</td>
</tr>
<tr>
<td align="left">14</td>
<td align="left">6.19</td>
<td align="left">3.16</td>
<td align="left">2.66</td>
<td align="left">1.19</td>
<td align="left">4.79</td>
<td align="left">2.45</td>
<td align="left">2.60</td>
<td align="left">0.94</td>
<td align="left">4.39</td>
<td align="left">2.24</td>
<td align="left">2.40</td>
<td align="left">0.93</td>
</tr>
<tr>
<td align="left">15</td>
<td align="left">6.32</td>
<td align="left">3.21</td>
<td align="left">2.96</td>
<td align="left">1.08</td>
<td align="left">5.78</td>
<td align="left">2.96</td>
<td align="left">3.00</td>
<td align="left">0.99</td>
<td align="left">5.83</td>
<td align="left">2.96</td>
<td align="left">3.02</td>
<td align="left">0.99</td>
</tr>
<tr>
<td align="left">16</td>
<td align="left">7.10</td>
<td align="left">3.62</td>
<td align="left">3.51</td>
<td align="left">1.03</td>
<td align="left">6.62</td>
<td align="left">3.37</td>
<td align="left">3.40</td>
<td align="left">0.99</td>
<td align="left">6.74</td>
<td align="left">3.42</td>
<td align="left">3.42</td>
<td align="left">1.01</td>
</tr>
<tr>
<td align="left">17</td>
<td align="left">7.60</td>
<td align="left">3.88</td>
<td align="left">3.57</td>
<td align="left">1.09</td>
<td align="left">7.10</td>
<td align="left">3.62</td>
<td align="left">3.70</td>
<td align="left">0.98</td>
<td align="left">7.08</td>
<td align="left">3.62</td>
<td align="left">3.61</td>
<td align="left">1.01</td>
</tr>
<tr>
<td align="left">18</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left">3.38</td>
<td align="left">1.73</td>
<td align="left">1.75</td>
<td align="left">0.99</td>
<td align="left">2.89</td>
<td align="left">1.48</td>
<td align="left">1.60</td>
<td align="left">0.93</td>
</tr>
<tr>
<td align="left">19</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left">4.61</td>
<td align="left">2.35</td>
<td align="left">2.40</td>
<td align="left">0.98</td>
<td align="left">4.22</td>
<td align="left">2.14</td>
<td align="left">2.42</td>
<td align="left">0.89</td>
</tr>
<tr>
<td align="left">20</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left">5.76</td>
<td align="left">2.96</td>
<td align="left">2.80</td>
<td align="left">1.06</td>
<td align="left">5.30</td>
<td align="left">2.70</td>
<td align="left">2.90</td>
<td align="left">0.93</td>
</tr>
<tr>
<td align="left">21</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left">6.42</td>
<td align="left">3.26</td>
<td align="left">3.20</td>
<td align="left">1.02</td>
<td align="left">6.18</td>
<td align="left">3.16</td>
<td align="left">3.13</td>
<td align="left">1.02</td>
</tr>
<tr>
<td align="left">22</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left">6.64</td>
<td align="left">3.37</td>
<td align="left">3.40</td>
<td align="left">0.99</td>
<td align="left">6.41</td>
<td align="left">3.26</td>
<td align="left">3.31</td>
<td align="left">0.99</td>
</tr>
<tr>
<td align="left">23</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left">3.01</td>
<td align="left">1.53</td>
<td align="left">1.71</td>
<td align="left">0.89</td>
<td align="left">2.48</td>
<td align="left">1.28</td>
<td align="left">1.51</td>
<td align="left">0.85</td>
</tr>
<tr>
<td align="left">24</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left">4.31</td>
<td align="left">2.20</td>
<td align="left">2.20</td>
<td align="left">1.00</td>
<td align="left">3.99</td>
<td align="left">2.04</td>
<td align="left">2.22</td>
<td align="left">0.93</td>
</tr>
<tr>
<td align="left">25</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left">5.54</td>
<td align="left">2.81</td>
<td align="left">2.70</td>
<td align="left">1.04</td>
<td align="left">4.82</td>
<td align="left">2.45</td>
<td align="left">2.71</td>
<td align="left">0.91</td>
</tr>
<tr>
<td align="left">26</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left">5.77</td>
<td align="left">2.96</td>
<td align="left">2.90</td>
<td align="left">1.02</td>
<td align="left">5.32</td>
<td align="left">2.70</td>
<td align="left">2.90</td>
<td align="left">0.93</td>
</tr>
<tr>
<td align="left">27</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left">6.28</td>
<td align="left">3.21</td>
<td align="left">3.00</td>
<td align="left">1.07</td>
<td align="left">5.88</td>
<td align="left">3.01</td>
<td align="left">3.03</td>
<td align="left">1.00</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F14" position="float">
<label>FIGURE 14</label>
<caption>
<p>Distribution of ratio of calculated and tested cube splitting strength.</p>
</caption>
<graphic xlink:href="fmats-10-1216747-g014.tif"/>
</fig>
</sec>
</sec>
<sec sec-type="conclusion" id="s4">
<title>4 Conclusion</title>
<p>The cube and cylinder nominal transverse splitting strengths of NC and CRC were determined and compared. On the basis of the results, the following conclusions can be drawn.<list list-type="simple">
<list-item>
<p>&#x2022; The stress distribution in the tensile direction of concrete is obtained by simulating the cylinder transverse splitting test using finite element analysis software. The tensile stress distribution area of the splitting tensile failure surface is large, which is similar to the stress distribution of the cube splitting tensile failure surface. This indicates that failure during concrete cylinder transverse splitting tests is mainly determined by the tensile stress.</p>
</list-item>
<list-item>
<p>&#x2022; The standard deviation of each group of concrete cylinder transverse splitting failure load tests is slightly lower than that obtained from the cube splitting failure load tests. This indicates a slightly higher precision of the cylinder tensile strength detected by the cylinder transverse splitting tests than that obtained by the cube splitting tensile tests.</p>
</list-item>
<list-item>
<p>&#x2022; The cube and cylinder nominal transverse splitting strengths of NC and CRC regularly decrease with increasing water-cement ratio and rubber content, which indicates a certain internal relationship between the cube and cylinder nominal transverse splitting strengths.</p>
</list-item>
<list-item>
<p>&#x2022; The relationship between the cube (150 &#xd7; 150 &#xd7; 150 mm) and cylinder (&#x2205;100 mm) nominal transverse splitting strength is established, <inline-formula id="inf39">
<mml:math id="m46">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.53</mml:mn>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>, with a correlation coefficient R<sup>2</sup> &#x3d; 0.994. The influence of rubber particle content and particle size on <inline-formula id="inf40">
<mml:math id="m47">
<mml:mrow>
<mml:mi>&#x3c8;</mml:mi>
</mml:mrow>
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</inline-formula> is small over the investigated range and can be ignored.</p>
</list-item>
</list>
</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/<xref ref-type="sec" rid="s11">Supplementary material</xref>, further inquiries can be directed to the corresponding author.</p>
</sec>
<sec sec-type="author-contributions" id="s6">
<title>Author contributions</title>
<p>QC and SH performed material preparation, data collection, and modeling. FW performed result analysis and discussion. FW edited the manuscript. LF reviewed the manuscript. All authors contributed to the article and approved the submitted version.</p>
</sec>
<sec id="s7">
<title>Funding</title>
<p>The research was supported by The National Key Research and Development Program of China (2022YFC3202300), Major Science and Technology Special Projects in Henan Province (201300311400), General Science Foundation Program of Henan Province (222300420491).</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="correction-note" id="s9">
<title>Correction note</title>
<p>This article has been corrected with minor changes. These changes do not impact the scientific content of the article.</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>
<sec sec-type="supplementary-material" id="s11">
<title>Supplementary material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/fmats.2023.1216747/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fmats.2023.1216747/full&#x23;supplementary-material</ext-link>
</p>
<supplementary-material xlink:href="DataSheet1.docx" id="SM1" mimetype="application/docx" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
<ref-list>
<title>References</title>
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