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<front>
<journal-meta>
<journal-id journal-id-type="pmc">SDHM</journal-id>
<journal-id journal-id-type="nlm-ta">SDHM</journal-id>
<journal-id journal-id-type="publisher-id">SDHM</journal-id>
<journal-title-group>
<journal-title>Structural Durability &#x0026; Health Monitoring</journal-title>
</journal-title-group>
<issn pub-type="epub">1930-2991</issn>
<issn pub-type="ppub">1930-2983</issn>
<publisher>
<publisher-name>Tech Science Press</publisher-name>
<publisher-loc>USA</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">22629</article-id>
<article-id pub-id-type="doi">10.32604/sdhm.2022.022629</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Article</subject>
</subj-group>
</article-categories>
<title-group>
<article-title>Effect of Freeze-Thaw Cycles on Chloride Transportation in Concrete: Prediction Model and Experiment</article-title><alt-title alt-title-type="left-running-head">Effect of Freeze-thaw Cycles on Chloride Transportation in Concrete: Prediction Model and Experiment</alt-title><alt-title alt-title-type="right-running-head">Effect of Freeze-thaw Cycles on Chloride Transportation in Concrete: Prediction Model and Experiment</alt-title>
</title-group>
<contrib-group>
<contrib id="author-1" contrib-type="author" corresp="yes">
<name name-style="western"><surname>Yan</surname><given-names>Yongdong</given-names></name><email>yand@ujs.edu.cn</email>
</contrib>
<contrib id="author-2" contrib-type="author">
<name name-style="western"><surname>Si</surname><given-names>Youdong</given-names></name>
</contrib>
<contrib id="author-3" contrib-type="author">
<name name-style="western"><surname>Lu</surname><given-names>Chunhua</given-names></name>
</contrib>
<contrib id="author-4" contrib-type="author">
<name name-style="western"><surname>Wu</surname><given-names>Keke</given-names></name>
</contrib>
<aff id="aff-1"><institution>Faculty of Civil Engineering and Mechanics, Jiangsu University</institution>, <addr-line>Zhenjiang, 212013</addr-line>, <country>China</country></aff>
</contrib-group><author-notes><corresp id="cor1"><label>&#x002A;</label>Corresponding Author: Yongdong Yan. Email: <email>yand@ujs.edu.cn</email></corresp></author-notes>
<pub-date date-type="collection" publication-format="electronic">
<year>2023</year></pub-date>
<pub-date date-type="pub" publication-format="electronic"><day>26</day><month>6</month><year>2023</year></pub-date>
<volume>17</volume>
<issue>3</issue>
<fpage>225</fpage>
<lpage>238</lpage>
<history>
<date date-type="received"><day>18</day><month>3</month><year>2022</year></date>
<date date-type="accepted"><day>11</day><month>7</month><year>2022</year></date>
</history>
<permissions>
<copyright-statement>&#x00A9; 2023 Yan et al.</copyright-statement>
<copyright-year>2023</copyright-year>
<copyright-holder>Yan et al.</copyright-holder>
<license xlink:href="https://creativecommons.org/licenses/by/4.0/">
<license-p>This work is licensed under a <ext-link ext-link-type="uri" xlink:type="simple" xlink:href="https://creativecommons.org/licenses/by/4.0/">Creative Commons Attribution 4.0 International License</ext-link>, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.</license-p>
</license>
</permissions>
<self-uri content-type="pdf" xlink:href="TSP_SDHM_22629.pdf"></self-uri>
<abstract>
<p>This research aims to investigate the effect of frost damage on chloride transportation mechanism in ordinary and fiber concrete with both theoretical and experimental methods. The proposed theoretical model takes into account the varying damage levels caused by concrete cover depth and freeze-thaw cycles, which are the two primary parameters affecting the expression of the chloride diffusion coefficient. In the experiment, three types of concrete were prepared: ordinary Portland concrete (OPC), polypropylene fiber concrete (PFC), and steel fiber concrete (SFC). These were then immersed in NaCl solution for 120 days after undergoing 10, 25, and 50 freeze-thaw cycles. The damage coefficient of the tested concrete was determined by measuring the dynamic elastic modulus. The results indicated that the relative dynamic elasticity modulus of the specimens decreased with each freeze-thaw cycle, and the chloride diffusion coefficient of the specimens increased as the degree of frost degradation increased. Samples containing steel and polypropylene fibers exhibited greater resistance to cyclic water freezing compared to the controlled concrete without fibers. A model has been also developed that takes into account the damage caused by freezing-thawing cycles and the depth of the concrete, which can predict variations in free chloride concentration at different depths. The calculated values were in good agreement with the test results for depths between 10 to 30 mm. This new damage-induced diffusion model can help fill the gap in research on the effects of freeze-thaw cycles on chloride diffusion.</p>
</abstract>
<kwd-group kwd-group-type="author">
<kwd>Damaged concrete</kwd>
<kwd>steel fiber</kwd>
<kwd>polypropylene fiber</kwd>
<kwd>chloride ion</kwd>
<kwd>freeze-thaw cycle</kwd>
</kwd-group>
<funding-group>
<award-group id="awg1">
<funding-source>Graduate Research Innovation Program of Jiangsu University</funding-source>
<award-id>Si Y. D., SJCX21_1689</award-id>
</award-group>
<award-group id="awg2">
<funding-source>National Natural Science Foundation of China</funding-source>
<award-id>Yan Y. D., 51608233</award-id>
</award-group>
</funding-group>
</article-meta>
</front>
<body>
<sec id="s1">
<label>1</label>
<title>Introduction</title>
<p>Most of the concrete cast in cold areas has to possess adequate freeze-thaw durability in the cold season [<xref ref-type="bibr" rid="ref-1">1</xref>&#x2013;<xref ref-type="bibr" rid="ref-3">3</xref>]. After freeze-thaw cycles, the strength [<xref ref-type="bibr" rid="ref-4">4</xref>] and elastic modulus [<xref ref-type="bibr" rid="ref-5">5</xref>] of concrete will be weakened. In view of this phenomenon, the durability deterioration characteristics of concrete structures after freeze-thaw cycles was studied by scholars in related fields, and some results have been achieved. Rao et al. [<xref ref-type="bibr" rid="ref-6">6</xref>] found that the fly ash in concrete increases the pores and microcracks of the specimen structure subjected to freeze-thaw cycle. Pogorelov et al. [<xref ref-type="bibr" rid="ref-7">7</xref>] pointed out that the pore structure in the concrete matrix can be improved by adding dispersed reinforcement, so as to improve the frost resistance of concrete to a certain extent. Wen et al. [<xref ref-type="bibr" rid="ref-8">8</xref>] found that the ordinary concrete exhibited a more serious damage phenomenon, and the frost resistance of concrete was improved with the increase of the content of steel slag aggregate. Luo et al. [<xref ref-type="bibr" rid="ref-9">9</xref>,<xref ref-type="bibr" rid="ref-10">10</xref>] found that adding rubber particles can improve the durability under freeze-thaw environment, but its mechanical properties are significantly reduced. The research of concrete durability and test methods mainly focus on the concrete surface scaling and internal damage caused by the freeze-thaw action, while the influence of the frost action on permeability and chloride transportation gained little attention. It is the fact that the diffusivity of chloride ions in concrete reaches a significantly higher value under cyclic freeze-thaw conditions [<xref ref-type="bibr" rid="ref-11">11</xref>]. Therefore, it is important to investigate the transport property of concrete to predict the initial time of rebar corrosion and the service life of concrete structures.</p>
<p>As the crack [<xref ref-type="bibr" rid="ref-12">12</xref>,<xref ref-type="bibr" rid="ref-13">13</xref>] and porosity [<xref ref-type="bibr" rid="ref-14">14</xref>] in concrete developed due to the frost attack, more interconnecting flow channels would emerge, which accelerate the ingress of aggressive agents, such as chlorides [<xref ref-type="bibr" rid="ref-15">15</xref>]. Many researchers have attempted to investigate the influence of freezing-thawing cycles on the diffusivity of concrete in the past few decades. Kuosa et al. [<xref ref-type="bibr" rid="ref-16">16</xref>] found that the relative dynamic modulus of concrete (RDM) was decreased by the freezing-thawing cycles, and the chloride migration coefficient increased with the decrease of the RDM. Jacobsen et al. [<xref ref-type="bibr" rid="ref-17">17</xref>] studied characteristics of cracks induced by freeze-thaw cycling and the effect of cracks on chloride transport properties. It was found that the chloride penetration rate increased to 7.9 times after 95 cycles compared to the sound specimen. Wieczorek et al. [<xref ref-type="bibr" rid="ref-18">18</xref>] pointed out that the high volume of crack density and the increase in crack width induced by freeze-thaw cycle improved the intrinsic coefficient of permeability by several orders of magnitude. The increase of transport properties, gas permeability, and water absorption coefficient was less pronounced until 75 freeze&#x2013;thaw cycles. Wittmann et al. [<xref ref-type="bibr" rid="ref-19">19</xref>] found that the chloride penetration was quite facilitated after 50 and 150 freezing-thawing cycles. Wang et al. [<xref ref-type="bibr" rid="ref-20">20</xref>] found the chloride ion diffusion coefficient first decreased and then increased as the number of cycles increased, and he proposed a new method to consider the damage resulting from freeze&#x2013;thaw cycling.</p>
<p>The damage of concrete matrix is a continued, accumulated and irreversible deterioration process [<xref ref-type="bibr" rid="ref-21">21</xref>]. However, there is a lack of analytical prediction models, especially for the chloride ion diffusion in frost damaged concrete. In this paper, a frost damage model in relation to dynamic elastic modulus is firstly proposed to represent the variation of chloride diffusion coefficient, and then the chloride concentration is predicted accordingly and compared with the test results.</p>
</sec>
<sec id="s2">
<label>2</label>
<title>A Model Predicting Chloride Transport in Damaged Concrete</title>
<sec id="s2_1">
<label>2.1</label>
<title>Damage Model</title>
<p>Concrete can be regarded as a homogeneous material when it is not damaged by environmental actions or loading. Thus, the chloride diffusion coefficient in undamaged concrete could be regarded as the same in each direction. However, this value will be different from the surface to inner part after freeze and thaw cycles, as the frost would cause more damage on the concrete surface than that on the inner part concrete [<xref ref-type="bibr" rid="ref-22">22</xref>]. A model considering the damage in response to freezing-thawing cycle and concrete depth is developed in this paper. Three reasonable assumptions are put forward for the model:<list list-type="simple"><list-item><label>(1)</label>
<p>Concrete is homogeneous before frost attack.</p></list-item><list-item><label>(2)</label>
<p>The boundary of concrete confronts with the same aggressive environment in the process of freezing-thawing cycle, and the variation of damage in concrete is exclusive with the same distance from the concrete surface.</p></list-item><list-item><label>(3)</label>
<p>The damage of frost concrete shows a linear relationship with the dynamic elastic modulus.</p></list-item></list></p>
<p>According to the above assumptions, the damage of frost concrete can be expressed as:<disp-formula id="eqn-1"><label>(1)</label>
<mml:math id="mml-eqn-1" display="block"><mml:mi>d</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>n</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">d</mml:mi></mml:mrow><mml:mn>0</mml:mn></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mrow></mml:mstyle></mml:math>
</disp-formula>where <italic>d</italic>(<italic>n</italic>) is the overall damage of concrete related to freeze-thaw cycles. <italic>E</italic><sub>dn</sub> is the dynamic elastic modulus after &#x201C;<italic>n</italic>&#x201D; cycles of frost action, and <italic>E</italic><sub>d0</sub> is the initial dynamic elastic modulus. According to <xref ref-type="disp-formula" rid="eqn-1">Eq. (1)</xref>, it can be seen that the damage of concrete increases with the freezing-thawing cycle, which is consistent with the actual condition.</p>
<p>The damage of frost concrete can be expressed as a function of concrete depth and freeze-thaw cycle:<disp-formula id="eqn-2"><label>(2)</label>
<mml:math id="mml-eqn-2" display="block"><mml:mi>d</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mtext>&#x00A0;</mml:mtext><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mi>exp</mml:mi><mml:mo>&#x2061;</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:mi mathvariant="normal">&#x03BB;</mml:mi></mml:mrow><mml:mi>n</mml:mi><mml:mo>+</mml:mo><mml:mi>v</mml:mi><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math>
</disp-formula>where <italic>&#x03BB;</italic> is a time correlation coefficient, which represents the influence of freeze-thaw cycle on concrete damage; <italic>v</italic> is a position correlation coefficient, which represents the influence of concrete depth, <italic>x</italic>.</p>
<p>After <italic>n</italic> cycles of frost attack, the overall damage of the concrete matrix can be expressed as the integral of <xref ref-type="disp-formula" rid="eqn-3">Eq. (3)</xref>:<disp-formula id="eqn-3"><label>(3)</label>
<mml:math id="mml-eqn-3" display="block"><mml:mtable columnalign="left" rowspacing=".5em" columnspacing="thickmathspace" displaystyle="true"><mml:mtr><mml:mtd><mml:mi>d</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>n</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mspace width="1em" /><mml:mo>=</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mn>2</mml:mn><mml:mi>h</mml:mi></mml:mfrac></mml:mrow><mml:msubsup><mml:mo>&#x222B;</mml:mo><mml:mn>0</mml:mn><mml:mrow><mml:mi>h</mml:mi><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:mrow><mml:mi>d</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mtext>&#x00A0;</mml:mtext><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mi>d</mml:mi><mml:mi>x</mml:mi></mml:mstyle></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mspace width="1em" /><mml:mo>=</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mn>2</mml:mn><mml:mi>h</mml:mi></mml:mfrac></mml:mrow><mml:msubsup><mml:mo>&#x222B;</mml:mo><mml:mn>0</mml:mn><mml:mrow><mml:mi>h</mml:mi><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup><mml:mrow><mml:mo stretchy="false">[</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mi>exp</mml:mi><mml:mo>&#x2061;</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:mi mathvariant="normal">&#x03BB;</mml:mi></mml:mrow><mml:mi>n</mml:mi><mml:mo>+</mml:mo><mml:mi>v</mml:mi><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo stretchy="false">]</mml:mo></mml:mrow><mml:mi>d</mml:mi><mml:mi>x</mml:mi></mml:mstyle></mml:mtd></mml:mtr></mml:mtable></mml:math>
</disp-formula>where <italic>h</italic> is the depth of concrete, which can be regarded as 100&#x2005;mm for the standard specimen (100&#x2005;mm&#x2009;&#x00D7;&#x2009;100&#x2005;mm&#x2009;&#x00D7;&#x2009;400&#x2005;mm) of freeze-thaw cycle test.</p>
<p>The output of <xref ref-type="disp-formula" rid="eqn-3">Eq. (3)</xref> should be equal to <xref ref-type="disp-formula" rid="eqn-1">Eq. (1)</xref> as both of them represent the overall damage of the concrete specimen. Therefore, <xref ref-type="disp-formula" rid="eqn-4">Eq. (4)</xref> could be obtained as:<disp-formula id="eqn-4"><label>(4)</label>
<mml:math id="mml-eqn-4" display="block"><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi></mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mrow><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mn>2</mml:mn><mml:mrow><mml:mi>h</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:mfrac></mml:mrow><mml:mi>exp</mml:mi><mml:mo>&#x2061;</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:mi mathvariant="normal">&#x03BB;</mml:mi></mml:mrow><mml:mi>n</mml:mi><mml:mo>+</mml:mo><mml:mi>v</mml:mi><mml:mi>h</mml:mi><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:mn>2</mml:mn><mml:mo stretchy="false">)</mml:mo><mml:mo>+</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mn>2</mml:mn><mml:mrow><mml:mi>h</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:mfrac></mml:mrow><mml:mi>exp</mml:mi><mml:mo>&#x2061;</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:mi mathvariant="normal">&#x03BB;</mml:mi></mml:mrow><mml:mi>n</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mstyle></mml:mstyle></mml:mstyle></mml:math>
</disp-formula></p>
<p>The coefficients of exposure time and position effect, <italic>&#x03BB;</italic> and <italic>v</italic>, can be regressed by <xref ref-type="disp-formula" rid="eqn-4">Eq. (4)</xref> according to the relative dynamic elastic modulus after frost attack which can be measured in experiment.</p>
</sec>
<sec id="s2_2">
<label>2.2</label>
<title>Model of Chloride Transportation in Damaged Concrete</title>
<p>For one-dimensional diffusion in a semi-infinite medium, the Fick&#x2019;s second law is commonly used to represent the pure diffusion process. The governing equation can be written as:<disp-formula id="eqn-5"><label>(5)</label>
<mml:math id="mml-eqn-5" display="block"><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mrow><mml:mi mathvariant="normal">&#x2202;</mml:mi><mml:mi>C</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mtext>&#x00A0;</mml:mtext><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2202;</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mrow><mml:mo>=</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mi mathvariant="normal">&#x2202;</mml:mi><mml:mrow><mml:mi mathvariant="normal">&#x2202;</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi>D</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mtext>&#x00A0;</mml:mtext><mml:mi>n</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mrow><mml:mi mathvariant="normal">&#x2202;</mml:mi><mml:mi>C</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mtext>&#x00A0;</mml:mtext><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2202;</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mrow></mml:mstyle><mml:mo>)</mml:mo></mml:mrow></mml:mstyle></mml:mstyle></mml:math>
</disp-formula>where <italic>C</italic>(<italic>x</italic>, <italic>t</italic>) is the chloride concentration at depth <italic>x</italic> and exposure time <italic>t</italic>; and <italic>D</italic>(<italic>x</italic>, <italic>n</italic>) is the chloride ion diffusion coefficient at a depth <italic>x</italic> after <italic>n</italic> cycles of freeze-thaw, which is related to the concrete damage. <italic>D</italic>(<italic>x</italic>, <italic>n</italic>) can be expressed as <xref ref-type="disp-formula" rid="eqn-6">Eq. (6)</xref>:<disp-formula id="eqn-6"><label>(6)</label>
<mml:math id="mml-eqn-6" display="block"><mml:mi>D</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mtext>&#x00A0;</mml:mtext><mml:mi>n</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mi>f</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>d</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:msub><mml:mi>D</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:math>
</disp-formula>where <italic>D</italic><sub>0</sub> is the initial chloride diffusion coefficient of sound concrete, <italic>f</italic>(<italic>d</italic>) is the damage coefficient induced by frost attack, which can be expressed as an s-type function [<xref ref-type="bibr" rid="ref-23">23</xref>]:<disp-formula id="eqn-7"><label>(7)</label>
<mml:math id="mml-eqn-7" display="block"><mml:mi>f</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>d</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mrow><mml:mo movablelimits="true" form="prefix">max</mml:mo></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:mrow></mml:mfrac></mml:mrow><mml:mrow><mml:mo>{</mml:mo><mml:mrow><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:msup><mml:mrow><mml:mo stretchy="false">[</mml:mo><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>d</mml:mi><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mrow><mml:mi mathvariant="normal">c</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:mrow></mml:mrow></mml:msub><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mi>m</mml:mi></mml:msup><mml:mo stretchy="false">]</mml:mo></mml:mrow><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>}</mml:mo></mml:mrow></mml:mstyle></mml:math>
</disp-formula>where <italic>D</italic><sub>max</sub> is chloride diffusion coefficient for a completely cracked material, <italic>m</italic> and <italic>d</italic><sub>cr</sub> are model parameters (<italic>m&#x2009;</italic>&#x003D;&#x2009;5, <italic>d</italic><sub>cr&#x2009;</sub>&#x003D;&#x2009;0.4). <xref ref-type="disp-formula" rid="eqn-7">Eq. (7)</xref> proceeds from the assumption that the chloride diffusion coefficient should be affected by damage, within the bounds of the coefficients for undamaged concrete and of totally cracked concrete, where the diffusion of free water is expected to be recovered on macro crack faces. Hence, <italic>D</italic><sub>max</sub> cannot exceed the diffusion coefficient in free water which is about 1.0&#x2009;&#x00D7;&#x2009;10<sup>&#x2212;9</sup> m<sup>2</sup>/s.</p>
</sec>
</sec>
<sec id="s3">
<label>3</label>
<title>Experiment</title>
<sec id="s3_1">
<label>3.1</label>
<title>Materials</title>
<p>Three different types of concrete materials, including OPC (ordinary Portland concrete), PFC (polypropylene fiber concrete), and SFC (steel fiber concrete), were tested in the experiment. The ordinary Portland cement (P.O 42.5) of Jiangsu Helin brand was adopted, and its properties met the standard [<xref ref-type="bibr" rid="ref-24">24</xref>]. The natural coarse aggregate used was 5&#x223C;25&#x2005;mm continuous graded crushed stone. The fine aggregate was river sand, with a fineness modulus of 2.7. The tap water was adopted, and the water reducing agent was used to improve the workability of the concrete. The two types of fiber used in PFC and SFC are usually added into the concrete mix to prevent crack damage. All tested specimens have the same dimension of 100&#x2005;mm &#x00D7;&#x2009;100&#x2005;mm&#x2009;&#x00D7;&#x2009;400&#x2005;mm, which were conformed to the standard dimensions of freeze-thaw cycle specimens [<xref ref-type="bibr" rid="ref-25">25</xref>]. The proportions of concrete mix are shown in <xref ref-type="table" rid="table-1">Table 1</xref>. The volume fractions of polypropylene and steel fibers in PFC and SFC concrete are 0.1&#x0025; and 1&#x0025;, respectively. Fibers used here were shown in <xref ref-type="fig" rid="fig-1">Fig. 1</xref> and their properties are given in <xref ref-type="table" rid="table-2">Table 2</xref>.</p>
<table-wrap id="table-1"><label>Table 1</label>
<caption>
<title>Proportion of concrete mix</title></caption>
<table><colgroup><col align="left"/><col align="left"/><col align="left"/><col align="left"/><col align="left"/><col align="left"/><col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">ID</th>
<th align="left">w/c ratio</th>
<th align="left">Water (kg/m<sup>3</sup>)</th>
<th align="left">Cement (kg/m<sup>3</sup>)</th>
<th align="left">Fine aggregate (kg/m<sup>3</sup>)</th>
<th align="left">Coarse aggregate (kg/m<sup>3</sup>)</th>
<th align="left">Fibre (kg/m<sup>3</sup>)</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">OPC</td>
<td align="left">0.55</td>
<td align="left">198</td>
<td align="left">360</td>
<td align="left">647</td>
<td align="left">1202</td>
<td align="left">-</td>
</tr>
<tr>
<td align="left">PFC</td>
<td align="left">0.55</td>
<td align="left">198</td>
<td align="left">360</td>
<td align="left">647</td>
<td align="left">1202</td>
<td align="left">0.9</td>
</tr>
<tr>
<td align="left">SFC</td>
<td align="left">0.55</td>
<td align="left">198</td>
<td align="left">360</td>
<td align="left">647</td>
<td align="left">1202</td>
<td align="left">40</td>
</tr>
</tbody>
</table>
</table-wrap><fig id="fig-1">
<label>Figure 1</label>
<caption>
<title>Fibers used in the experiment</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-1.tif"/>
</fig><table-wrap id="table-2"><label>Table 2</label>
<caption>
<title>Properties of PPF and SF</title></caption>
<table><colgroup><col align="left"/><col align="left"/><col align="left"/><col align="left"/><col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">Fibre name</th>
<th align="left">Density (g/cm<sup>3</sup>)</th>
<th align="left">Length (mm)</th>
<th align="left">Tensile strength (MPa)</th>
<th align="left">Elastic modulus (GPa)</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">Polypropylene fibre</td>
<td align="left">0.91</td>
<td align="left">10</td>
<td align="left">&#x003E;450</td>
<td align="left">&#x003E;3.9</td>
</tr>
<tr>
<td align="left">Steel fibre</td>
<td align="left">7.8</td>
<td align="left">20</td>
<td align="left">&#x003E;600</td>
<td align="left">200</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s3_2">
<label>3.2</label>
<title>Experimental Methodology</title>
<p>12 prism specimens for each mix were cast and then cured in water for 28 days. Subsequently, 9 specimens of OPC, PFC, and SFC withstood 10, 25, and 50 cycles of freeze-thaw activity according to the standard test method. Rapid freeze&#x2013;thaw cycle test was performed by using the NELD-FC810 concrete rapid freeze&#x2013;thaw test apparatus. In this test, the temperature at the center of the control specimens ranged from &#x2212;17&#x00B0;C&#x223C;5&#x00B0;C, and each cycle was about 3.5&#x2005;h. Detailed requirements and operation steps were conducted following the specifications in the GB/T 50082-2009. The dynamic modulus of elasticity of the concrete specimen was obtained by measuring the longitudinal pulse velocity of the specimen (ZBL-U520 non-metal pulse velocity test apparatus) after every 5 cycle&#x2019;s frost according to the standard test method, which was shown in <xref ref-type="fig" rid="fig-2">Fig. 2</xref>.</p>
<fig id="fig-2">
<label>Figure 2</label>
<caption>
<title>Photograph of concrete dynamic elastic modulus measurement</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-2.tif"/>
</fig>
<p>Then, considering one mold contact surface (100&#x2005;mm&#x2009;&#x00D7;&#x2009;400&#x2005;mm) as the exposure surface, seal the other five surfaces of the specimen with epoxy resin using a brush. After that, harden the epoxy resin through air exposure for 24&#x2005;h. Then immersed the specimen in NaCl solution with a concentration of 8&#x0025; for 120 days accelerated test. Took out the specimens from the chloride solution after exposure and drilled three holes in each specimen using a 14&#x2005;mm diameter rotary impact drill. Sufficient powdered concrete sample was taken out from each hole at a depth of every 5 mm and was mixed to provide the average chloride content in the measured location. Powdered concrete samples with particle size less than 0.63&#x2005;mm were then selected with a sieve and dried to anhydrous state. After that, 1.5&#x2005;g samples from each group were dissolved in 10&#x2005;ml distilled water, vibrated for nearly 1 min, and then stewed for 24 h to completely dissolve the free chloride ion in the sample [<xref ref-type="bibr" rid="ref-26">26</xref>,<xref ref-type="bibr" rid="ref-27">27</xref>]. Mohr titration [<xref ref-type="bibr" rid="ref-28">28</xref>] was finally used to determine the potential of the concentration with chloride ions. According to the calibration test results from the standard chloride concentration and its potential value, the free chloride concentration of every solution containing concrete powder sample can be obtained from the tested potential (<xref ref-type="fig" rid="fig-3">Fig. 3</xref>).</p>
<fig id="fig-3">
<label>Figure 3</label>
<caption>
<title>Photograph of chloride ion concentration measurement for concrete powder</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-3.tif"/>
</fig>
</sec>
<sec id="s3_3">
<label>3.3</label>
<title>Results and Discussion</title>
<p>The scaling of the concrete surface after 50 freeze-thaw cycles were shown in <xref ref-type="fig" rid="fig-4">Fig. 4</xref>, which indicated that the damages of OPC and PFC were more serious than those of SFC. The dynamic elastic modulus of each specimen was measured after every 5 cycle&#x2019;s frost. The results are presented in <xref ref-type="fig" rid="fig-5">Fig. 5</xref>. The relative dynamic elastic modulus (RDEM) decreased with the increasing of freeze-thaw cycle. However, the descent rate of concrete with steel and polypropylene fibers were smaller than that of ordinary concrete. The reason for this was that the integrity of concrete was improved by the addition of fiber, and the hydrostatic pressure or osmotic pressure could be reduced during the freeze-thaw cycles, then finally reduced the degree of freeze-thaw damage [<xref ref-type="bibr" rid="ref-29">29</xref>,<xref ref-type="bibr" rid="ref-30">30</xref>]. As a result, it can be concluded from the results that the fibers can improve the ability of concrete to resist frost damage from variations of concrete surface and modulus.</p>
<fig id="fig-4">
<label>Figure 4</label>
<caption>
<title>Surface scaling of concrete specimens resulted from 50 freeze-thaw cycles</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-4.tif"/>
</fig><fig id="fig-5">
<label>Figure 5</label>
<caption>
<title>Relative dynamic elastic modulus <italic>vs.</italic> freeze-thaw cycle</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-5.tif"/>
</fig>
<p>The distribution of free chloride ions in OPC, PFC, SFC specimens after different time freeze-thaw cycles were shown in <xref ref-type="fig" rid="fig-6 fig-7 fig-8">Figs. 6&#x2013;8</xref>. The concentration of chloride ions in the shallow layer of concrete increases with the increase of freeze-thaw cycles. The change of chloride ion concentration in the deep layer of concrete is a little different between OPC, PFC, and SFC. The concentration of chloride ion in ordinary concrete within depth greater than 27&#x2005;mm decreases after 10 cycles of freeze-thaw, but increases a little after 25 cycles, and then increases obviously after 50 cycles. After 10 cycles of freeze-thaw, the concentration of chloride ion in concrete mixed with polypropylene fiber within depth greater than 25&#x2005;mm decreased slightly, while that in steel fiber concrete did not change significantly within depth greater than 32&#x2005;mm after 10 and 25 cycles of freeze-thaw. This shows that the damage of concrete in the shallow layer within about 30&#x2005;mm depth is damaged more obviously than that in the deep depth of concrete during freeze-thaw cycles, which results in more chloride ions invading into the concrete, because of the continuous hydration and ice crystal blocking, only when the number of freeze-thaw cycles is more, the internal damage is slightly aggravated, resulting in chloride ion erosion speed up. The free chloride concentration in all of the three types concrete after 50 cycles of freeze-thaw increased more clearly which demonstrated that the damages become more significantly than that after 10 and 25 freeze-thaw cycles.</p>
<fig id="fig-6">
<label>Figure 6</label>
<caption>
<title>Free chloride ion concentrations of OPC specimens subject to different freeze-thawing cycles</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-6.tif"/>
</fig><fig id="fig-7">
<label>Figure 7</label>
<caption>
<title>Free chloride ion concentrations of PFC specimens subject to different freeze-thawing cycles</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-7.tif"/>
</fig><fig id="fig-8">
<label>Figure 8</label>
<caption>
<title>Free chloride ion concentrations of SFC specimens subject to different freeze-thawing cycles</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-8.tif"/>
</fig>
</sec>
</sec>
<sec id="s4">
<label>4</label>
<title>Chloride Prediction</title>
<sec id="s4_1">
<label>4.1</label>
<title>Damage Calculation</title>
<p>The coefficients <italic>&#x03BB;</italic> and <italic>v</italic> in <xref ref-type="disp-formula" rid="eqn-2">Eq. (2)</xref> can be regressed from <xref ref-type="disp-formula" rid="eqn-4">Eq. (4)</xref> with the dynamic elastic modulus obtained at every 5 freeze-thaw cycle based on the least square method. The regressing results are shown in <xref ref-type="table" rid="table-3">Table 3</xref>. It shows that the time correlation coefficient <italic>&#x03BB;</italic> of OPC is larger than those of PFC and SFC, where the law of position correlation coefficient <italic>v</italic> is inversed. This result indicates that the damage caused by frost attack in OPC is larger than those in PFC and SFC.</p>
<table-wrap id="table-3"><label>Table 3</label>
<caption>
<title>Regression coefficients and accuracy of three types concrete</title></caption>
<table><colgroup><col align="left"/><col align="left"/><col align="left"/><col align="left"/>
</colgroup>
<thead>
<tr>
<th>Coefficient</th>
<th align="left" colspan="3">Concrete</th>
</tr>
<tr>
<th align="left"></th>
<th align="left">OPC</th>
<th align="left">PFC</th>
<th align="left">SFC</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left"><italic>&#x03BB;</italic></td>
<td align="left">1.59&#x2009;&#x00D7;&#x2009;10<sup>&#x2212;2</sup></td>
<td align="left">1.21&#x2009;&#x00D7;&#x2009;10<sup>&#x2212;2</sup></td>
<td align="left">1.06&#x2009;&#x00D7;&#x2009;10<sup>&#x2212;2</sup></td>
</tr>
<tr>
<td align="left"><italic>v</italic></td>
<td align="left">9.60&#x2009;&#x00D7;&#x2009;10<sup>&#x2212;4</sup></td>
<td align="left">9.65&#x2009;&#x00D7;&#x2009;10<sup>&#x2212;4</sup></td>
<td align="left">9.92&#x2009;&#x00D7;&#x2009;10<sup>&#x2212;4</sup></td>
</tr>
<tr>
<td align="left"><italic>R</italic></td>
<td align="left">0.99</td>
<td align="left">0.99</td>
<td align="left">0.99</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The calculated damage of concrete after 50 freeze-thaw cycles is plotted in <xref ref-type="fig" rid="fig-9">Fig. 9</xref>. The values slightly decrease with the depth. For example, the damage in OPC is 0.54 at the surface and becomes 0.52 at the depth of 50 mm. The values in PFC and SFC are both smaller than those in OPC and decrease with concrete depth.</p>
<fig id="fig-9">
<label>Figure 9</label>
<caption>
<title>Distribution of damage after 50 freeze-thaw cycles in concretes</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-9.tif"/>
</fig>
<p>As the RDEMs of most concrete prisms started to steadily decline from 10 cycles and reached an allowable value at about 50 cycles, the damages at these two states and a medium value of 25 cycle were representatively selected to analysis.</p>
<p>The damage coefficient calculated by <xref ref-type="disp-formula" rid="eqn-7">Eq. (7)</xref>, which is related to concrete depth and freeze-thaw cycles, is shown in <xref ref-type="fig" rid="fig-10 fig-11 fig-12">Figs. 10&#x2013;12</xref> for OPC, PFC, and SFC, respectively. The damage coefficients of each type of concrete slightly decrease with the depth but increase significantly with freeze-thaw cycle.</p>
<fig id="fig-10">
<label>Figure 10</label>
<caption>
<title>Distribution of damage coefficient in OPC after different times freeze-thaw cycle</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-10.tif"/>
</fig><fig id="fig-11">
<label>Figure 11</label>
<caption>
<title>Distribution of damage coefficient in PFC after different times freeze-thaw cycle</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-11.tif"/>
</fig><fig id="fig-12">
<label>Figure 12</label>
<caption>
<title>Distribution of damage coefficient in SFC after different times freeze-thaw cycle</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-12.tif"/>
</fig>
<p>For some coastal concrete structures in north area, they always sustain an action of freeze-thaw cycle in sea water, which will make the damage of concrete be more serious than that in fresh water. The damage coefficient will also be greater than that in <xref ref-type="fig" rid="fig-10 fig-11 fig-12">Figs. 10&#x2013;12</xref>.</p>
</sec>
<sec id="s4_2">
<label>4.2</label>
<title>Prediction of Chloride Content</title>
<p>During the experiment, surface chloride concentrations for each type of concrete were obtained after exposed to chloride solution for 120 days (<xref ref-type="table" rid="table-4">Table 4</xref>).</p>
<table-wrap id="table-4"><label>Table 4</label>
<caption>
<title>Surface chloride concentration (&#x0025;)</title></caption>
<table><colgroup><col align="left"/><col align="left"/><col align="left"/><col align="left"/>
</colgroup>
<thead>
<tr>
<th>Freeze-thaw cycle</th>
<th align="left" colspan="3">Concrete types</th>
</tr>
<tr>
<th align="left"></th>
<th align="left">OPC</th>
<th align="left">PFC</th>
<th align="left">SFC</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">0</td>
<td align="left">0.2740</td>
<td align="left">0.3138</td>
<td align="left">0.2497</td>
</tr>
<tr>
<td align="left">10</td>
<td align="left">0.3197</td>
<td align="left">0.3625</td>
<td align="left">0.3156</td>
</tr>
<tr>
<td align="left">25</td>
<td align="left">0.3062</td>
<td align="left">0.3460</td>
<td align="left">0.3504</td>
</tr>
<tr>
<td align="left">50</td>
<td align="left">0.3696</td>
<td align="left">0.3927</td>
<td align="left">0.3692</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The distribution of chloride ion at different depths of concrete under different exposure time can be obtained from Fick&#x2019;s second law of diffusion. The apparent diffusion coefficients of sound and damaged concrete were regressed by <xref ref-type="disp-formula" rid="eqn-8">Eq. (8)</xref> [<xref ref-type="bibr" rid="ref-31">31</xref>]:<disp-formula id="eqn-8"><label>(8)</label>
<mml:math id="mml-eqn-8" display="block"><mml:mi>C</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mtext>&#x00A0;</mml:mtext><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn>0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mi>s</mml:mi></mml:msub><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn>0</mml:mn></mml:msub><mml:mo stretchy="false">)</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>f</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mi>x</mml:mi><mml:mrow><mml:mn>2</mml:mn><mml:msqrt><mml:msub><mml:mi>D</mml:mi><mml:mrow><mml:mi mathvariant="normal">a</mml:mi></mml:mrow></mml:msub><mml:mi>t</mml:mi></mml:msqrt></mml:mrow></mml:mfrac></mml:mrow></mml:mstyle><mml:mo>)</mml:mo></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:math>
</disp-formula>where <italic>C</italic><sub>0</sub> is initial chloride concentration, <italic>C</italic><sub>s</sub> is the surface chloride concentration, <italic>D</italic><sub>a</sub> is the apparent chloride diffusion coefficient, <italic>t</italic> is the exposure time and <italic>erf</italic> is the error function.</p>
<p>As the chloride in the surface layer mainly transports by convection instead of diffusion [<xref ref-type="bibr" rid="ref-32">32</xref>,<xref ref-type="bibr" rid="ref-33">33</xref>], the first data at a depth of 0&#x223C;5&#x2005;mm was not considered in the regression [<xref ref-type="bibr" rid="ref-34">34</xref>]. The apparent chloride diffusion coefficients of frost-damaged concrete specimens developed from this equation were shown in <xref ref-type="fig" rid="fig-13">Fig. 13</xref>, which revealed that the values of chloride diffusion coefficient of these three mixes first decrease before 10 cycles&#x2019; freeze-thaw and then increase with freeze-thaw cycles. This attributed to the effect of continuous cement hydration was larger than the frost damage under small amount of cyclic freeze-thaw conditions. As the fibers can alleviate its damage under frost, concrete with steel and polypropylene fibers displays a lower value than the OPC.</p>
<fig id="fig-13">
<label>Figure 13</label>
<caption>
<title>Apparent chloride diffusion coefficients of OPC(O), PFC(P), and SFC(S) specimens subject to different freeze-thaw cycles</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-13.tif"/>
</fig>
<p>The chloride contents in the three types of concrete predicted by <xref ref-type="disp-formula" rid="eqn-8">Eq. (8)</xref> were given in <xref ref-type="fig" rid="fig-14 fig-15 fig-16">Figs. 14&#x2013;16</xref> and compared with the corresponding experimental results. It can be obtained that the predicted chloride contents agree well with the experimental data within the depth of 10&#x2013;30&#x2005;mm which were shown in the figures as accurate region. In this region, the relative errors between predicted and experimental data were ranged from 0.8&#x0025; to 14&#x0025;, and most of them were lower than 10&#x0025;. However, due to the convection effect, the experimental chloride contents were larger than the predicted chloride contents at the concrete surface within the depth of 0&#x223C;10 mm, and most of the relative errors between the predicted and experimental data were in the range of 4&#x0025;&#x2013;20&#x0025;. On the other hand, the test results were inaccurate at deep depths (larger than 30&#x2005;mm) because of the small values which would be influenced more significantly by the test error, and then made the relative errors be in the range of 20&#x0025;&#x2013;50&#x0025;. It can also be found that most of them are larger than the predicted values.</p>
<fig id="fig-14">
<label>Figure 14</label>
<caption>
<title>Distribution of chloride concentration after 10, 25, and 50 freeze-thaw cycles in OPC (&#x0025;)</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-14.tif"/>
</fig><fig id="fig-15">
<label>Figure 15</label>
<caption>
<title>Distribution of chloride concentration after 10, 25, and 50 freeze-thaw cycles in PFC (&#x0025;)</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-15.tif"/>
</fig><fig id="fig-16">
<label>Figure 16</label>
<caption>
<title>Distribution of chloride concentration after 10, 25, and 50 freeze-thaw cycles in SFC (&#x0025;)</title></caption>
<graphic mimetype="image" mime-subtype="tif" xlink:href="SDHM_22629-fig-16.tif"/>
</fig>
</sec>
</sec>
<sec id="s5">
<label>5</label>
<title>Conclusions</title>
<p>Based on the experimental results and the analysis model of the damage distribution induced by freeze-thaw cycle, the following conclusions can be drawn:<list list-type="simple"><list-item><label>(1) </label>
<p>Concrete exhibited non-uniform damage under freeze-thaw cycles. The surface spalling of OPC and PFC were more serious than those of SFC after 50 freeze-thaw cycles which indicated that the damage degree at the concrete surface is larger than that at a deep depth. The relative dynamic elastic modulus (RDEM) decreased with the increasing of freeze-thaw cycle numbers. The decline speed of RDEM for different types of concrete was in an order as OPC&#x2009;&#x003E;&#x2009;PFC&#x2009;&#x003E;&#x2009;SFC, which indicated that PPF and SF can both improve the ability of concrete to resist frost damage.</p></list-item><list-item><label>(2) </label>
<p>For the concrete after 10 and 25 freeze-thaw cycles, the chloride ion concentration in the shallow layer (within about 30&#x2005;mm depth) increased with the increasing of freeze-thaw cycle numbers. This phenomenon indicated that the frost damage of concrete in the shallow layer within about 30&#x2005;mm depth is more obviously than that in the deeper depth after few times of freeze-thaw cycle. The free chloride concentration at any position of OPC, PSC and SFC increased more obviously after 50 cycles of freeze-thaw which demonstrated that the damages become more significantly than those after 10 and 25 freeze-thaw cycles.</p></list-item><list-item><label>(3) </label>
<p>A model considering the freeze-thaw cycle and concrete depth was proposed in this study to express the non-uniform damage of concrete under freeze-thaw cycles. According to this model, the calculated damage values in PFC and SFC were both smaller than those in OPC and decreased with concrete depth. Non-uniform distributed chloride diffusion coefficient was found to increase with the increasing of the freeze-thaw cycle numbers and decrease slightly with the concrete depth. Based on this model, the chloride concentrations in frost damaged concrete were predicted and obtained to agreed well with the test result within the depth of 10 to 30&#x2005;mm. The relative errors of most data in this region were lower than 10&#x0025;.</p></list-item></list></p>
</sec>
</body>
<back>
<sec>
<title>Funding Statement</title>
<p>The work described in this paper was supported by the Graduate Research Innovation Program of Jiangsu University (Si Y. D., SJCX21_1689), and the Foundation from the National Natural Science Foundation of China (Yan Y. D., 51608233).</p>
</sec>
<sec sec-type="COI-statement">
<title>Conflicts of Interest</title>
<p>The authors declare that they have no conflicts of interest to report regarding the present study.</p>
</sec>
<ref-list content-type="authoryear">
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