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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">733257</article-id>
<article-id pub-id-type="doi">10.3389/fmats.2021.733257</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>The Effect of Pyrolysis Conditions on the Preparation of Fe<sub>2</sub>O<sub>3</sub> Particles Using Simulated Pickling Liquor in a Venturi Reactor</article-title>
<alt-title alt-title-type="left-running-head">Lv et&#x20;al.</alt-title>
<alt-title alt-title-type="right-running-head">Effect of Pyrolysis Conditions on Particle</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Lv</surname>
<given-names>Chao</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1390514/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Sun</surname>
<given-names>Ming-He</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Yin</surname>
<given-names>Hong-Xin</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
</contrib-group>
<aff id="aff1">
<label>
<sup>1</sup>
</label>School of Control Engineering, Northeastern University, <addr-line>Qinhuangdao</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<label>
<sup>2</sup>
</label>Key Laboratory for Ferrous Metallurgy and Resources Utilization of Ministry of Education, Wuhan University of Science and Technology, <addr-line>Wuhan</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/1147504/overview">Wangzhong Mu</ext-link>, Royal Institute of Technology, Sweden</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/1391383/overview">Yuming Wen</ext-link>, Royal Institute of Technology, Sweden</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1391443/overview">Fengqin Liu</ext-link>, University of Science and Technology Beijing, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1392174/overview">Zongliang Zhang</ext-link>, Central South University, China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Chao Lv, <email>lvchao@neuq.edu.cn</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Colloidal Materials and Interfaces, a section of the journal Frontiers in Materials</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>13</day>
<month>08</month>
<year>2021</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>8</volume>
<elocation-id>733257</elocation-id>
<history>
<date date-type="received">
<day>30</day>
<month>06</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>03</day>
<month>08</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2021 Lv, Sun and Yin.</copyright-statement>
<copyright-year>2021</copyright-year>
<copyright-holder>Lv, Sun and Yin</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&#x20;terms.</p>
</license>
</permissions>
<abstract>
<p>Large amounts of pickling liquor are produced during the pickling of iron and steel. The Venturi reactor is used during the pyrolysis of pickling liquor to prepare high-purity Fe<sub>2</sub>O<sub>3</sub> particles. Changing the pyrolysis conditions will affect the purity and concentration of Fe<sub>2</sub>O<sub>3</sub> particles. In this paper, physical experiments and numerical simulations were carried out to study the effect of pyrolysis conditions on the Fe<sub>2</sub>O<sub>3</sub> particles, including the pyrolysis temperature, the FeCl<sub>2</sub>/FeCl<sub>3</sub> ratio in the pickling liquor, and the citric acid ratio. The results showed that a product with a higher purity, better crystallinity, and greater concentration was obtained at 923&#xa0;K. Further increasing the temperature did not change the concentration of Fe<sub>2</sub>O<sub>3</sub> particles. When the ratio of FeCl<sub>2</sub>/FeCl<sub>3</sub> in the pickling liquor was 1:1.5, the maximum concentration of Fe<sub>2</sub>O<sub>3</sub> particles at the outlet was obtained. When the added proportion of citric acid was 1:1, the particle size distribution was more uniform, and when the added proportion was 1:2.5, the maximum concentration of Fe<sub>2</sub>O<sub>3</sub> particles at the outlet was achieved.</p>
</abstract>
<kwd-group>
<kwd>pickling liquor</kwd>
<kwd>pyrolysis</kwd>
<kwd>Fe<sub>2</sub>O<sub>3</sub>
</kwd>
<kwd>particles</kwd>
<kwd>numerical simulation</kwd>
</kwd-group>
<contract-num rid="cn001">51904069</contract-num>
<contract-num rid="cn002">E2019501085</contract-num>
<contract-sponsor id="cn001">National Natural Science Foundation of China<named-content content-type="fundref-id">10.13039/501100001809</named-content>
</contract-sponsor>
<contract-sponsor id="cn002">Natural Science Foundation of Hebei Province<named-content content-type="fundref-id">10.13039/501100003787</named-content>
</contract-sponsor>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>The dense Fe<sub>2</sub>O<sub>3</sub> formed on the surface of steel products during their production requires pickling, which produces 1.2&#x2013;2 tons of pickling liquor per ton of steel (<xref ref-type="bibr" rid="B17">Zhang et&#x20;al., 2014</xref>; <xref ref-type="bibr" rid="B13">Wang and Ma, 2017</xref>; <xref ref-type="bibr" rid="B14">Wang et&#x20;al., 2020</xref>). HCl pickling liquor contains 1&#x2013;5% HCl and 5&#x2013;20% FeCl<sub>2</sub>/FeCl<sub>3</sub>, which causes severe environmental issues if discharged directly, as well as resource waste (<xref ref-type="bibr" rid="B3">Fang et&#x20;al., 2010</xref>; <xref ref-type="bibr" rid="B4">Gao et&#x20;al., 2021</xref>). In large iron and steel enterprises, the Ruthner spray pyrolysis method (<xref ref-type="bibr" rid="B11">Qi, 2006</xref>; <xref ref-type="bibr" rid="B2">Deng et&#x20;al., 2007</xref>; <xref ref-type="bibr" rid="B1">Bian et&#x20;al., 2015</xref>) is primarily used to process waste acid, in which FeCl<sub>2</sub> and FeCl<sub>3</sub> react with H<sub>2</sub>O and O<sub>2</sub> to produce HCl and Fe<sub>2</sub>O<sub>3</sub> particles. Nevertheless, this process has technical barriers and high investment costs. To decrease costs and increase the value of by-products, an in-depth study of the pyrolysis technique is needed. <xref ref-type="bibr" rid="B12">Sun et&#x20;al. (2021)</xref> prepared the nanometer ferric oxide (Fe<sub>2</sub>O<sub>3</sub> nanorod) by the hydrothermal method, the ferric nitrate nonahydrate (Fe(NO<sub>3</sub>)<sub>3</sub>&#xb7;9H<sub>2</sub>O) was the source of ferric and the ethanol absolute and ethylenediamine were used as the surfactant. Effects of the reaction temperature and the mass fraction of Fe(NO<sub>3</sub>)<sub>3</sub>&#xb7;9H<sub>2</sub>O on the particle size of the Fe<sub>2</sub>O<sub>3</sub> nanorod were investigated. <xref ref-type="bibr" rid="B18">Zhang et&#x20;al. (2020)</xref> prepared the &#x3b1;-nanometer Fe<sub>2</sub>O<sub>3</sub> by microwave hydrolysis, FeCl<sub>3</sub> was the raw material and the triethylenetetramine (TETA) was used as the coordination agent. Taniguchi (<xref ref-type="bibr" rid="B5">Izumi et&#x20;al., 2007</xref>) synthesized LiMn<sub>2</sub>O<sub>4</sub> particles with a hollow sphere morphology from a precursor solution using spray pyrolysis from a slurry solution and prepared spherical LiMn<sub>2</sub>O<sub>4</sub> nanoparticles. <xref ref-type="bibr" rid="B6">Liu et&#x20;al. (2018)</xref> designed a spray pyrolysis reactor using SiC and prepared MgO with an average particle size of 90&#xa0;&#x3bc;m. They also studied parameters such as the pyrolysis temperature and feed quantity. Moreover, computational fluid dynamics (CFD) was used to simulate the spray pressure and temperature distribution in a pyrolysis furnace. Lv et&#x20;al. produced a mixture of gases and solids with the Venturi reactor, which improved the pyrolysis efficiency and prepared spherical CeCl<sub>3</sub> and Fe<sub>2</sub>O<sub>3</sub> micro/nanoparticles (<xref ref-type="bibr" rid="B8">Lv et&#x20;al., 2019a</xref>; <xref ref-type="bibr" rid="B9">Lv et&#x20;al., 2019b</xref>; <xref ref-type="bibr" rid="B10">Lv et&#x20;al., 2019c</xref>; <xref ref-type="bibr" rid="B7">Lv, 2019</xref>). Venturi reactor can enhance the mix of the gas and liquid, and solve the problem of Ruthner spray pyrolysis method that the nozzle needs to be replaced periodically. The simple structure and low investment of the Venturi reactor have resulted in its broad usage, but it is necessary to study it further. At present, there is a problem that the product particles are easy to accumulate and jam at the Venturi tube when the Venturi reactor is used for the pyrolysis reaction. Adding citric acid can well solve this problem. The carbon dioxide and water vapor are produced in the chemical reaction by citric acid. The gas-phase pressure can push the particles to flow to outlet, which prevents the jam at Venturi tube, increases the reaction efficiency and changes the morphology of the product particles.</p>
<p>This paper used a combination of experiments and numerical simulations to study the effects of temperature, pickling liquor composition, and citric acid ratio on the composition and morphology of Fe<sub>2</sub>O<sub>3</sub> particles obtained at the outlet of a Venturi reactor. The effect on the Fe<sub>2</sub>O<sub>3</sub> particle distribution in the reactor was also investigated. The results can be used to optimize the operating conditions of pyrolysis, as well as the pickling liquor, to provide a reference for the optimal design of Venturi reactors.</p>
</sec>
<sec id="s2">
<title>Experimental</title>
<sec id="s2-1">
<title>Physical Experiments</title>
<p>A diagram of the equipment used in the jet pyrolysis experiments is shown in <xref ref-type="fig" rid="F1">Figure&#x20;1</xref>. Oxygen was added by a high-speed air pump 1 into the Venturi reactor 4. The waste acid 2 mixed with citric acid, and then the mixed liquor dripped into the heating furnace 3. Pyrolysis occurred in the Venturi reactor 4. Next, the pyrolysis product Fe<sub>2</sub>O<sub>3</sub> was collected by a particle collector, and tail gas was recovered by the alkali liquor in the recovery device 6. Venturi reactor is a place for evaporation, phase change and pyrolysis reaction. The reaction mechanism is not clear now, so the investigation of it should be focused on. Because of the mature separation technology of the gas and solid phase, we did not lay emphasis on it in this study. Employing the pyrolysis conditions summarized in <xref ref-type="table" rid="T1">Table&#x20;1</xref> and O<sub>2</sub>, CO<sub>2</sub>, HCl(g), H<sub>2</sub>O(g), HCl(l), H<sub>2</sub>O(l), FeCl<sub>2</sub>, FeCl<sub>3</sub>, and Fe<sub>2</sub>O<sub>3</sub> as the chemical&#x20;species involved in the reactions. Physical parameters of the substances were obtained from the handbook of practical inorganic thermodynamic data (<xref ref-type="bibr" rid="B16">Ye and Hu, 2002</xref>).</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Diagram of equipment. 1 oxygen bottle; 2 waste acid solution; 3 heating furnace; 4 Venturi reactor; 5 Solid product collector; 6 alkali liquor.</p>
</caption>
<graphic xlink:href="fmats-08-733257-g001.tif"/>
</fig>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Pyrolysis conditions.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Condition</th>
<th align="center">Value</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Temperature (K)</td>
<td align="center">773&#x3001;873&#x3001;923&#x3001;973&#x3001;1023&#x3001;1123</td>
</tr>
<tr>
<td align="left">FeCl<sub>2</sub>/FeCl<sub>3</sub>
</td>
<td align="center">1:0.5; 1:0.75; 1:1; 1:1.25; 1:1.5</td>
</tr>
<tr>
<td align="left">FeCl<sub>2</sub>/C<sub>6</sub>H<sub>8</sub>O<sub>7</sub>
</td>
<td align="center">1:0.5; 1:1; 1:1.5; 1:2; 1:2.5</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s2-2">
<title>Numerical Simulations</title>
<p>According to the Venturi reactor dimensions, a geometric model with identical proportions was created in SolidWorks 2016, and ICEM 19.0 was used to divide the geometric model into a structured grid with a quantity of 410&#x2032;000 (<xref ref-type="fig" rid="F2">Figure&#x20;2</xref>).</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Geometric models and mesh generation.</p>
</caption>
<graphic xlink:href="fmats-08-733257-g002.tif"/>
</fig>
<p>Eulerian multiphase model, standard k-&#x3b5; turbulence model and SIMPLE algorithm were selected in Fluent 19.0, the control equations were differentially treated using the second-order upwind scheme, and all items were converged to 10<sup>&#x2013;4</sup> except for energy (to 10<sup>&#x2013;6</sup>). The time step was set to 0.001&#xa0;s, the computing time was 60&#xa0;s and the simulation results were steady at the moment. The main reactions involved include:<disp-formula id="e1">
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</mml:math>
<label>(5)</label>
</disp-formula>Besides the mass conservation equation, momentum conservation equation and energy conservation equation, it also involved the chemical reaction equation:<disp-formula id="e6">
<mml:math id="m6">
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:mo>&#x2202;</mml:mo>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mi>&#x3c1;</mml:mi>
<mml:msub>
<mml:mi>Y</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2202;</mml:mo>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x2b;</mml:mo>
<mml:mo>&#x2207;</mml:mo>
<mml:mo>&#x22c5;</mml:mo>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mi>&#x3c1;</mml:mi>
<mml:mrow>
<mml:mover accent="true">
<mml:mi>&#x3bd;</mml:mi>
<mml:mo stretchy="true">&#xaf;</mml:mo>
</mml:mover>
</mml:mrow>
<mml:msub>
<mml:mi>Y</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mo>&#x3d;</mml:mo>
<mml:mo>&#x2212;</mml:mo>
<mml:mo>&#x2207;</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mover accent="true">
<mml:mi>J</mml:mi>
<mml:mo stretchy="true">&#xaf;</mml:mo>
</mml:mover>
</mml:mrow>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>&#x2b;</mml:mo>
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>&#x2b;</mml:mo>
<mml:msub>
<mml:mi>S</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
<label>(6)</label>
</disp-formula>where Y<sub>i</sub> is the mass fraction of the ith substance, R<sub>i</sub> is the net produce rate of chemical reaction of the ith substance, S<sub>i</sub> is the discrete phase of the ith substance and it is also the extra produce rate caused by the user-defined source item, J<sub>i</sub> is the diffusive flux of the ith substance produced by the concentration gradient.</p>
<p>As shown in <xref ref-type="fig" rid="F2">Figure&#x20;2</xref>, the section on the left side in the horizontal direction of the jet reactor was set as the O<sub>2</sub> inlet, the section on the right was the free outlet, and the section directly below the reactor in the vertical direction was the waste acid solution&#x20;inlet.</p>
</sec>
<sec id="s2-3">
<title>Procedures</title>
<p>FeCl<sub>2</sub> and FeCl<sub>3</sub> solutions, each with a mass ratio of 10%, were prepared using deionized water, HCl, FeCl<sub>2</sub> and FeCl<sub>3</sub> solution (FeCl<sub>2</sub>10%FeCl<sub>3</sub>5%, FeCl<sub>2</sub>10%FeCl<sub>3</sub>7.5%, FeCl<sub>2</sub>10%FeCl<sub>3</sub>10%, FeCl<sub>2</sub>10%FeCl<sub>3</sub>12.5%, FeCl<sub>2</sub>10%FeCl<sub>3</sub>15%, the mass ratio of the two was 1:0.5, 1:0.75, 1:1, 1:1.25, and 1:1.5). Based on the prepared FeCl<sub>2</sub>10%FeCl<sub>3</sub>10% waste acid solution, a certain amount of citric acid was added to prepare a precursor solution with FeCl<sub>2</sub>: C<sub>6</sub>H<sub>8</sub>O<sub>7</sub> mass ratios of 1:0.5, 1:1, 1:1.5, 1:2, and 1:2.5. FeCl<sub>2</sub>, FeCl<sub>3</sub>, HCl, and C<sub>6</sub>H<sub>8</sub>O<sub>7</sub> were provided by Tianjin Fengchuan Chemical Reagent Technologies Co., Ltd. The real-time monitoring of the pyrolysis temperature was performed by the pyrolysis furnace. When the furnace reached the set temperature, the oxygen entered the Venturi reactor from the left inlet at a speed of 21.15&#xa0;m/s under the carrier gas pressure, and the waste acid solution entered the Venturi reactor from the material inlet. The furnace temperature was set to 773, 873, 923, 973, 1023, and 1123&#xa0;K, and the pyrolysis products Fe<sub>2</sub>O<sub>3</sub> were collected at the cyclone separating&#x20;unit.</p>
</sec>
</sec>
<sec sec-type="results|discussion" id="s3">
<title>Results and Discussion</title>
<sec id="s3-1">
<title>Verification of Simulation Result</title>
<p>The boundary conditions are shown in <xref ref-type="table" rid="T2">Table&#x20;2</xref>. The basic standard conditions of the research are 10%FeCl<sub>2</sub>, 10%FeCl<sub>3</sub>, 5%HCl, 0%C<sub>6</sub>H<sub>8</sub>O<sub>7</sub>.</p>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Boundary conditions.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left"/>
<th align="center">Inlet1-O<sub>2</sub>
</th>
<th align="center">Inlet2-FeCl<sub>2</sub>\FeCl<sub>3</sub>
</th>
<th align="center">Outlet</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Condition</td>
<td align="center">Velocity-inlet</td>
<td align="center">Velocity-inlet</td>
<td align="center">Outflow</td>
</tr>
<tr>
<td align="left">Value (m/s)</td>
<td align="center">21.15</td>
<td align="center">0.015 (10%FeCl<sub>2</sub>, 5%-15%FeCl<sub>3</sub>, 5%HCl, 0%-25%C<sub>6</sub>H<sub>8</sub>O<sub>7</sub>)</td>
<td align="center">&#x2014;</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>As shown in <xref ref-type="table" rid="T3">Table&#x20;3</xref>, the data results of Fe<sub>2</sub>O<sub>3</sub> and CO<sub>2</sub> at outlet of the two representative conditions: adding no citric acid and adding 10% citric acid were compared. The errors between the experimental results of the collected Fe<sub>2</sub>O<sub>3</sub> and CO<sub>2</sub> at the outlet and the numerical simulations was within 10%, which indicated the validity of the chosen model and the boundary conditions of the simulation. As shown in <xref ref-type="fig" rid="F3">Figure&#x20;3</xref>, to further study the distribution of Fe<sub>2</sub>O<sub>3</sub> in the reactor, five sections in the Venturi reactor were monitored.</p>
<table-wrap id="T3" position="float">
<label>TABLE 3</label>
<caption>
<p>Content comparison at outlet.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left"/>
<th align="center">Experimental result</th>
<th align="center">Simulation results</th>
<th align="center">Errors</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Fe<sub>2</sub>O<sub>3</sub>(0%C<sub>6</sub>H<sub>8</sub>O<sub>7</sub>)</td>
<td align="char" char=".">2997.03&#xa0;g/h</td>
<td align="char" char=".">3211.24&#xa0;g/h</td>
<td align="char" char=".">6.67%</td>
</tr>
<tr>
<td align="left">CO<sub>2</sub>(0%C<sub>6</sub>H<sub>8</sub>O<sub>7</sub>)</td>
<td align="center">0&#xa0;g/h</td>
<td align="center">0&#xa0;g/h</td>
<td align="center">0%</td>
</tr>
<tr>
<td align="left">Fe<sub>2</sub>O<sub>3</sub>(10%C<sub>6</sub>H<sub>8</sub>O<sub>7</sub>)</td>
<td align="char" char=".">3018.61&#xa0;g/h</td>
<td align="char" char=".">3289.25&#xa0;g/h</td>
<td align="char" char=".">8.23%</td>
</tr>
<tr>
<td align="left">CO<sub>2</sub>(10%C<sub>6</sub>H<sub>8</sub>O<sub>7</sub>)</td>
<td align="char" char=".">3382.76&#xa0;g/h</td>
<td align="char" char=".">3519.42&#xa0;g/h</td>
<td align="char" char=".">3.88%</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Determination of monitoring surface.</p>
</caption>
<graphic xlink:href="fmats-08-733257-g003.tif"/>
</fig>
</sec>
<sec id="s3-2">
<title>Effects of Pyrolysis Temperature on the Pyrolysis Performance</title>
<p>The XRD phase analysis of products prepared under different pyrolysis temperatures was carried out from 10 to 80&#xb0; at a scan rate of 7&#xa0;&#xb0;/min. As shown in <xref ref-type="fig" rid="F4">Figure&#x20;4</xref>, the products prepared by jet pyrolysis under different temperatures all consisted of Fe<sub>2</sub>O<sub>3</sub>. Upon increasing the pyrolysis temperature, the intensity of the diffraction peak of (B-L) Fe<sub>2</sub>O<sub>3</sub> first decreased and then gradually increased. The intensity of the diffraction peak of F &#x2212;923&#xa0;K was the smallest without an obvious peak of impurity phases, different crystal forms of Fe<sub>2</sub>O<sub>3</sub> were possibly produced at 923&#xa0;K.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>XRD patterns of the pyrolysis products obtained at different temperatures. B-773, D-873K, F-923K, H-973K, J-1023K, L-1123K.</p>
</caption>
<graphic xlink:href="fmats-08-733257-g004.tif"/>
</fig>
<p>According to the numerical simulation results (<xref ref-type="fig" rid="F5">Figure&#x20;5</xref>), the average Fe<sub>2</sub>O<sub>3</sub> concentration on various monitored surfaces in the reactor increased significantly upon increasing the pyrolysis temperature. When the pyrolysis temperature reached 923&#xa0;K, further increasing the pyrolysis temperature did not affect the average concentration of Fe<sub>2</sub>O<sub>3</sub> particles significantly. This indicates that 923&#xa0;K is the optimal pyrolysis temperature.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>The average Fe<sub>2</sub>O<sub>3</sub> concentration on monitored surfaces at different temperatures.</p>
</caption>
<graphic xlink:href="fmats-08-733257-g005.tif"/>
</fig>
</sec>
<sec id="s3-3">
<title>Effects of Pickling Liquor Composition on Pyrolysis</title>
<p>When the pyrolysis temperature reached 923&#xa0;K, the XRD phase analysis of products prepared using different FeCl<sub>2</sub>/FeCl<sub>3</sub> ratios in the pickling liquor was conducted, and the results are shown in <xref ref-type="fig" rid="F6">Figure&#x20;6</xref>. The products prepared by jet pyrolysis under different FeCl<sub>2</sub>/FeCl<sub>3</sub> ratios all consisted of Fe<sub>2</sub>O<sub>3</sub>. The height of the crystal face 104 and 110 changed. As the FeCl<sub>2</sub>/FeCl<sub>3</sub> ratio increased, (B-J) Fe<sub>2</sub>O<sub>3</sub> grew along different crystal faces. When FeCl<sub>2</sub>:FeCl<sub>3</sub> &#x3d; 1:1, the Fe<sub>2</sub>O<sub>3</sub> with the least impurities among all the cases was obtained, with the strongest diffraction peak intensity.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>XRD patterns of the pyrolysis products obtained at different FeCl<sub>2</sub>/FeCl<sub>3</sub> ratios. B-1:0.5, D-1:0.75, F-1:1, H-1:1.25, J-1:1.5.</p>
</caption>
<graphic xlink:href="fmats-08-733257-g006.tif"/>
</fig>
<p>As shown in <xref ref-type="fig" rid="F7">Figure&#x20;7</xref>, the Fe<sub>2</sub>O<sub>3</sub> concentration in the reactor increased upon increasing the concentration of FeCl<sub>3</sub> in the pickling liquor. When FeCl<sub>2</sub>:FeCl<sub>3</sub> &#x3d; 1:1.5, the maximum average Fe<sub>2</sub>O<sub>3</sub> particle concentration on various monitored surfaces in the reactor was obtained. This was because upon increasing the FeCl<sub>3</sub> concentration, the Fe ion content at the material inlet increased; thus, according to the law of conservation, the concentration of Fe<sub>2</sub>O<sub>3</sub> particles at the outlet&#x20;also increased.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Fe<sub>2</sub>O<sub>3</sub> concentration on the monitored surfaces at different FeCl<sub>2</sub>/FeCl<sub>3</sub> ratios.</p>
</caption>
<graphic xlink:href="fmats-08-733257-g007.tif"/>
</fig>
</sec>
<sec id="s3-4">
<title>Effects of the Citric Acid Ratio During Pyrolysis</title>
<p>When the pyrolysis temperature reached 923&#xa0;K, FeCl<sub>2</sub>:FeCl<sub>3</sub> &#x3d; 1:1, the XRD phase analysis of products prepared with different proportions of citric acid was carried out, and the results are shown in <xref ref-type="fig" rid="F8">Figure&#x20;8</xref>. Adding citric acid contributed to a sufficient pyrolysis reaction and a disappearing of impurity peak. The products prepared by jet pyrolysis using different citric acid ratios all consisted of Fe<sub>2</sub>O<sub>3</sub>. Upon changing the pickling liquor ratio, there was no obvious change in the intensity of the diffraction peak of (B-J) Fe<sub>2</sub>O<sub>3</sub>, and the addition of more citric acid had no obvious effect on the product purity.</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>XRD patterns of the pyrolysis products obtained using different citric acid ratios. B-1:0.5, D-1:1, F-1:1.5, H-1:2, J-1:2.5.</p>
</caption>
<graphic xlink:href="fmats-08-733257-g008.tif"/>
</fig>
<p>
<xref ref-type="fig" rid="F9">Figure&#x20;9</xref> shows the SEM images of pyrolysis products using solutions with different citric acid ratios. As the citric acid ratio increased, the Fe<sub>2</sub>O<sub>3</sub> particles aggregated and finally evolved into irregular sheets. This was because upon increasing the citric acid ratio, a great amount of gas was produced during the pyrolysis of citric acid under a high temperature, and the aggregated products exploded into fragments due to the gas pressure (<xref ref-type="bibr" rid="B15">Yang et&#x20;al., 2017</xref>).</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>SEM images of the pyrolysis products <bold>(A)</bold> 1:0.5&#x20;<bold>(B)</bold> 1:1&#x20;<bold>(C)</bold> 1:1.5&#x20;<bold>(D)</bold> 1:2&#x20;<bold>(E)</bold> 1:2.5.</p>
</caption>
<graphic xlink:href="fmats-08-733257-g009.tif"/>
</fig>
<p>The integral area of each curve in <xref ref-type="fig" rid="F10">Figure&#x20;10</xref> is shown in <xref ref-type="table" rid="T4">Table&#x20;4</xref>. When the concentration of the citric acid changed, increasing the citric acid ratio did not obviously affect the total amount of Fe<sub>2</sub>O<sub>3</sub> particles in the reactor because the addition of citric acid did not change the total amount of Fe ions at the material inlet. The added citric acid changed the Fe<sub>2</sub>O<sub>3</sub> particle distribution in the reactor&#x2014;at a higher citric acid ratio, less Fe<sub>2</sub>O<sub>3</sub> appeared on the first half of the monitored surface, and a higher Fe<sub>2</sub>O<sub>3</sub> content appeared on the second half. This was because a large amount of gas (CO<sub>2</sub> and H<sub>2</sub>O) was produced during the pyrolysis of citric acid. The flow of this gas changed the distribution of particle products in the Venturi reactor, which caused the particle product content to decrease in the first half of the reactor, while the particle product content increased in the second&#x20;half.</p>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>Average Fe<sub>2</sub>O<sub>3</sub> concentrations on monitored surfaces in the reactor at different citric acid ratios.</p>
</caption>
<graphic xlink:href="fmats-08-733257-g010.tif"/>
</fig>
<table-wrap id="T4" position="float">
<label>TABLE 4</label>
<caption>
<p>Integral areas of different curves.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Curve</th>
<th align="center">1:0</th>
<th align="center">1:0.5</th>
<th align="center">1:1</th>
<th align="center">1:1.5</th>
<th align="center">1:2</th>
<th align="center">1:2.5</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Area</td>
<td align="char" char=".">0.0813</td>
<td align="char" char=".">0.0812</td>
<td align="char" char=".">0.0810</td>
<td align="char" char=".">0.0813</td>
<td align="char" char=".">0.0812</td>
<td align="char" char=".">0.0811</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</sec>
<sec sec-type="conclusion" id="s4">
<title>Conclusion</title>
<p>As the pyrolysis temperature increased, the concentration of Fe<sub>2</sub>O<sub>3</sub> particles in the reactor increased. At 923&#xa0;K, the purity and concentration of Fe<sub>2</sub>O<sub>3</sub> were maximized, and further increasing the pyrolysis temperature had negligible effects on the concentration of Fe<sub>2</sub>O<sub>3</sub> particles at the outlet. When FeCl2:FeCl3 &#x3d; 1:1, the Fe2O3 with the least impurities among all the cases was obtained. When FeCl<sub>2</sub>/FeCl<sub>3</sub> &#x3d; 1:1.5, the concentration of Fe<sub>2</sub>O<sub>3</sub> particles at the outlet was maximized. The ratio of citric acid possibly changed size distribution of Fe<sub>2</sub>O<sub>3</sub> particles and their distribution in the reactor. When the ratio of FeCl<sub>2</sub>/C<sub>6</sub>H<sub>8</sub>O<sub>7</sub> was1:1, the size distribution of Fe<sub>2</sub>O<sub>3</sub> particles was homogeneous, and when the ratio of FeCl<sub>2</sub>/C<sub>6</sub>H<sub>8</sub>O<sub>7</sub> was1:2.5, the concentration of Fe<sub>2</sub>O<sub>3</sub> particles at the outlet was maximized.</p>
</sec>
</body>
<back>
<sec id="s5">
<title>Data Availability Statement</title>
<p>The raw data supporting the conclusion of this article will be made available by the authors, without undue reservation.</p>
</sec>
<sec id="s6">
<title>Author Contributions</title>
<p>CL: Conceptualization, Funding acquisition, Project administration; M-HS: Data curation, Writing&#x2014;original, draft; H-XY: Software.</p>
</sec>
<sec id="s7">
<title>Funding</title>
<p>This research was supported by the National Natural Science Foundation of China (51904069), the open fund of the Key Laboratory of iron and steel metallurgy and resource utilization of Wuhan University of science and technology (FMRU19-1), the Scientific Research Fund project of Northeastern University at Qinhuangdao (XNY201808), the Natural Science Foundation of Hebei Province of China (E2019501085).</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 id="s9" sec-type="disclaimer">
<title>Publisher&#x2019;s Note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
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