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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Chem.</journal-id>
<journal-title>Frontiers in Chemistry</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Chem.</abbrev-journal-title>
<issn pub-type="epub">2296-2646</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">1038095</article-id>
<article-id pub-id-type="doi">10.3389/fchem.2022.1038095</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Chemistry</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>CO<sub>2</sub>-assisted fabrication of silica gel adsorbent in honeycomb rotary wheels for air dehumidification</article-title>
<alt-title alt-title-type="left-running-head">You 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/fchem.2022.1038095">10.3389/fchem.2022.1038095</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>You</surname>
<given-names>Junjie</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>Qin</surname>
<given-names>Junbo</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Du</surname>
<given-names>Chuanqing</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Fu</surname>
<given-names>Jianhua</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Cheng</surname>
<given-names>Siqing</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/1770717/overview"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Innovation Centre for Nanomaterials in Energy and Environment (ICNEE)</institution>, <institution>School of Chemical and Environmental Engineering</institution>, <institution>Wuhan Polytechnic University</institution>, <addr-line>Wuhan</addr-line>, <addr-line>Hubei</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Wuhan Coobase Facilities Company Limited</institution>, <addr-line>Wuhan</addr-line>, <addr-line>Hubei</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/1031267/overview">Zhenyu Sun</ext-link>, Beijing University of Chemical Technology, China</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/860486/overview">Jiehua Liu</ext-link>, Hefei University of Technology, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1858905/overview">Feng Han</ext-link>, Shandong Agricultural University, China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Siqing Cheng, <email>icnee@whpu.edu.cn</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Green and Sustainable Chemistry, a section of the journal Frontiers in Chemistry</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>04</day>
<month>10</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>10</volume>
<elocation-id>1038095</elocation-id>
<history>
<date date-type="received">
<day>06</day>
<month>09</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>16</day>
<month>09</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 You, Qin, Du, Fu and Cheng.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>You, Qin, Du, Fu and Cheng</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>A honeycomb rotary wheel fabricated from sheet adsorbent of silica gel is a competitive drying facility for air dehumidification in modern drying and air conditioning industries due to its large contacting area (3,000&#xa0;m<sup>2</sup>/m<sup>3</sup>) and the rapid diffusion of the adsorbate compared to silica gel pellets. The delicate preparation procedure of hygroscopic silica gel is paramount for improved adsorption capacity by optimizing the surface area, pore size, and pore volume of silica gel. In this article, silica gel adsorbent in a honeycomb rotary wheel was fabricated by neutralizing the impregnated water glass solution with a modulus of 3.3 on the glass fiber sheet of the honeycomb matrix using CO<sub>2</sub> at different pressure at room temperature instead of corrosive acids. The as-obtained silica gel absorbent was characterized by XRD, scanning electron microscopy (SEM), specific surface area and pore size analysis, and dynamic vapor/gas sorption analysis. The results showed that the as-obtained silica gel adsorbent is uniform in size and tunable in terms of specific surface area, pore size, pore volume, and adsorption capacity by CO<sub>2</sub> pressure. The typical silica gel fabricated by CO<sub>2</sub> of 0.25&#xa0;MPa with a specific surface area of 764.86&#xa0;m<sup>2</sup>/g, an average micropore size with a diameter of 2.94&#xa0;nm, and a pore volume of 0.45&#xa0;ml/g delivers a saturated adsorption capacity of as high as 287.24&#xa0;mg/g at RH 50%, which is the best in adsorption performance compared to the previously reported results. This provides a new strategy for environment-friendly manufacturing of silica gel adsorbent in honeycomb rotary wheels for air dehumidification.</p>
</abstract>
<kwd-group>
<kwd>honeycomb rotary wheel</kwd>
<kwd>dehumidification</kwd>
<kwd>CO<sub>2</sub>
</kwd>
<kwd>silica gel</kwd>
<kwd>absorbent</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>Air humidity has always been drawing a worldwide concern both in our daily life and in various conventional (food, cosmetics, papermaking, pharmaceuticals, etc.) and emerging industries (microelectronics, lithium-related batteries, etc.) due to its role with respect to air quality and its requirement for the manufacture, preservation, transportation, and further processing of products (<xref ref-type="bibr" rid="B1">Aristov et al., 2002</xref>; <xref ref-type="bibr" rid="B26">Wu et al., 2018</xref>). Thus, air dehumidification technology has been attracting extensive interest academically and industrially. The traditional direct dehumidification technologies mainly consist of condensing dehumidification, heating dehumidification, membrane dehumidification, and liquid desiccant dehumidification, in which the relevant environmental issues owing to the utilization of a non-environment-friendly refrigerant, the energy-intensive requirement, high-cost membrane fabrication, etc. impede their further development, especially in today&#x2019;s ever-increasing climate deterioration (<xref ref-type="bibr" rid="B4">Cha et al., 2007</xref>; <xref ref-type="bibr" rid="B7">Hwang et al., 2007</xref>; <xref ref-type="bibr" rid="B3">Bhagat et al., 2008</xref>; <xref ref-type="bibr" rid="B8">Iswar et al., 2017</xref>). In recent years, an adsorptive dehumidification technology by solid regenerable desiccant to selectively remove and separate the moisture from moist air under ambient conditions shows great promise for future air dehumidification (<xref ref-type="bibr" rid="B10">Kabeel, 2007</xref>; <xref ref-type="bibr" rid="B2">Bareschino et al., 2015</xref>).</p>
<p>Thus far, four types of solid desiccant dehumidifiers as adsorptive dehumidification technology have been proposed, namely, solid packed beds, rotating horizontal beds, multiple vertical beds, and honeycomb rotary wheels, among which only the honeycomb rotary wheels integrate the dehumidifier and desorption processes into one, demonstrating the lower pressure drop and large surface area for heat and mass transfer with respect to the desirable characteristics, such as high space efficiency, continuous adsorption&#x2013;desorption cycles, high dehumidification, and utilization of low-grade heat sources, such as solar energy and waste heat, for adsorbent regeneration (<xref ref-type="bibr" rid="B5">Chung et al., 2001</xref>; <xref ref-type="bibr" rid="B3">Bhagat et al., 2008</xref>; <xref ref-type="bibr" rid="B6">Hindersmann, 2019</xref>). As a state-of-the-art solid desiccant dehumidification technology, the honeycomb rotary wheel consists of numerous parallel airflow passageway constructed typically with alternating sinusoidal corrugated fibrous substrate sheets and flat fibrous substrate sheets on whose surface a solid desiccant material is impregnated. As such, the widely dispersed desiccants work based on the famous Kelvin formula which shows the vapor pressure difference between the air and the desiccant to attract the moisture from the air until its vapor pressure is in equilibrium with the air. (<xref ref-type="bibr" rid="B11">Kodama et al., 1993</xref>; <xref ref-type="bibr" rid="B9">Jia et al., 2006</xref>).</p>
<p>The performance of the solid desiccant honeycomb rotary wheel depends, to a large extent, upon the characteristics of the desiccant materials such as high dehumidification capacity, fast kinetics, high stability, and the ability to regenerate at a low temperature. Silica gel is the most popular solid desiccant usually used in the honeycomb rotary wheel due to its low cost, high porosity, and excellent stability although it has a limited dehumidification capacity of 20%&#x2013;30% of its initial weight and higher regeneration temperature of 60&#x2013;100&#xb0;C (<xref ref-type="bibr" rid="B12">Kuma and Hirose, 1996</xref>; <xref ref-type="bibr" rid="B13">La et al., 2010</xref>; <xref ref-type="bibr" rid="B14">Lee and Lee, 2012</xref>; <xref ref-type="bibr" rid="B15">Li et al., 2016</xref>). As we know, desiccant dehumidifies in that desiccants have open empty spaces between the molecules called capillaries. As such, the hygroscopic performance of the silica gel is determined by its intrinsic physical/chemical properties and the surface porous (capillary) structure including surface area, pore volume, average pore size, and pore size distribution, which are affected by the preparation procedures/variables of silica gel (<xref ref-type="bibr" rid="B11">Kodama et al., 1993</xref>; <xref ref-type="bibr" rid="B18">Neti and Wolfe, 2000</xref>; <xref ref-type="bibr" rid="B16">Liu, 2003</xref>; <xref ref-type="bibr" rid="B17">Manjunatha et al., 2013</xref>).</p>
<p>The general manufacturing variables of silica gel are quite complex including the type of starting materials, catalyst, solvent, reaction temperature, gelation schemes, drying temperature, etc. Many research works have investigated in detail the effects of the preparation procedure on the surface characteristics of silica gel. Especially for the silica gel used in the honeycomb rotary wheel with glass fibers as substrate, water glass is generally employed to act as the type of starting material due to its availability, low cost, and environment friendliness (<xref ref-type="bibr" rid="B21">Sarawade et al., 2010</xref>; <xref ref-type="bibr" rid="B19">O&#x2019;Connor et al., 2016</xref>; <xref ref-type="bibr" rid="B20">Prasad et al., 2019</xref>). The different preparation procedures of silica gel by neutralization using different acids such as HCl, H<sub>3</sub>PO<sub>4</sub>, H<sub>2</sub>SO<sub>4</sub>, HNO<sub>3,</sub> and HCOOH were investigated to obtain the different surface characteristics of silica gel and thus the different dehumidification properties, which are also adopted to manufacture industrially silica gel desiccant in the honeycomb rotary wheel (<xref ref-type="bibr" rid="B28">Zhang et al., 2003</xref>; <xref ref-type="bibr" rid="B25">White et al., 2011</xref>; <xref ref-type="bibr" rid="B26">Wu et al., 2018</xref>; <xref ref-type="bibr" rid="B27">Yang et al., 2020</xref>). However, the usages of strong acids are unfavorable to operation and the environment due to their corrosion or volatility (<xref ref-type="bibr" rid="B23">Wang et al., 2013</xref>; <xref ref-type="bibr" rid="B24">Wei et al., 2013</xref>; <xref ref-type="bibr" rid="B22">Su et al., 2021</xref>). Herein, to our knowledge, it is the first time in this work to report that CO<sub>2</sub> as nontoxic greenhouse gas was employed to neutralize the starting material water glass to prepare silica gel desiccant in the honeycomb rotary wheel and the preparation variables including CO<sub>2</sub> pressure and the reaction time were optimized, the resulting silica gel desiccant in the honeycomb rotary wheel exhibits excellent surface characteristics and thus good dehumidification characteristics.</p>
</sec>
<sec id="s2">
<title>Experimental</title>
<sec id="s2-1">
<title>Preparation of honeycomb silica gel</title>
<p>The flat glass fiber paper (Ahlstrom-Munksjo glassfibre Oy, Kotka, Finland) was cut to be 10 &#xd7; 10&#xa0;cm square and was rolled down to be corrugated glass fiber paper with colloidal silica (10&#xa0;wt%, Chemical Engineering Sci.and Tech. Ltd. Company, Henan, China). Then, the flat and the prepared corrugated glass fiber paper were stacked alternately with a thickness of 10&#xa0;cm to form a honeycomb monolith. The as-obtained honeycomb monolith was impregnated with water glass (ca. 3.3 modulus, 40&#xa0;wt%, Haobo Chemical Engineering Ltd. Company, Shandong, China) for 2&#xa0;hours and taken out to dry incompletely. The water glass-impregnated honeycomb monolith was placed in a high-pressure reactor and subjected to CO<sub>2</sub> at different pressure for 3&#x2013;5&#xa0;h. After the reaction was complete, the honeycomb monolith was washed to remove the carbonate until the solution is close to being neutral followed by the aging in the deionized water for 2&#xa0;h at 40&#xb0;C. Finally, the honeycomb monolith with silica gel was completed by drying and calcination.</p>
</sec>
<sec id="s2-2">
<title>Characterization of honeycomb silica gel</title>
<p>The powder X-ray diffraction (XRD) patterns were collected on a Japan Shimadzu DX-7000 advanced X-ray diffractometer using the Cu K&#x3b1; radiation with <italic>&#x3bb;</italic> &#x3d; 0.15418&#xa0;nm over 2&#x3b8; degree from 10&#xb0; to 70&#xb0; at a scan rate of 4&#xb0; min<sup>&#x2212;1</sup>. Scanning electron microscopy (SEM) images were performed on a JEOL JSM-6700M scanning electron microscopy. Nitrogen physisorption was carried out at &#x2212;196<inline-formula id="inf1">
<mml:math id="m1">
<mml:mrow>
<mml:mo>&#x2103;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> on a Micromeritics BeishiDe PS2-1529-B specific surface area and pore size analyzer. The Brunauer&#x2013;Emmett&#x2013;Teller (BET) surface area, pore volume, and pore size distribution were obtained. The samples were pretreated at 150<inline-formula id="inf2">
<mml:math id="m2">
<mml:mrow>
<mml:mo>&#x2103;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> under a high vacuum for 12&#xa0;h prior to the nitrogen adsorption-desorption test. The pore volume was calculated from the adsorbed nitrogen after complete pore condensation at the relative pressure of P/P<sub>0</sub> &#x3d; 0.995. The pore size was estimated from the desorption branch <italic>via</italic> the Barrett&#x2013;Joyner&#x2013;Halenda (BJH) method.</p>
</sec>
<sec id="s2-3">
<title>Adsorption/desorption kinetics and isotherms of water vapor</title>
<p>The adsorption/desorption kinetics and isotherms of the water vapor on the silica gel were measured on a gravity dynamic vapor system (BSD-VVS, BeiShiDe Instrument). Before the measurement of vapor adsorption, the samples were dried at 200<inline-formula id="inf3">
<mml:math id="m3">
<mml:mrow>
<mml:mo>&#x2103;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> for 2&#xa0;h. Nitrogen was used as the dry carrier gas and the concentration of vapor was precisely controlled with a mass flow controller and real-time vapor concentration monitor. The sample weight change during water vapor sorption/desorption can be measured by an ultra-microbalance module. With the mass change to &#x3c; 0.002 mass%/min, the samples were considered to reach the kinetic equilibrium. Based on the equilibrium moisture content at different relative humidity, water vapor isotherms can be plotted. The adsorption kinetics was obtained by measuring the weight change of the samples with time at 25<inline-formula id="inf4">
<mml:math id="m4">
<mml:mrow>
<mml:mo>&#x2103;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> at different relative humidity (RH). The adsorption isotherms were plotted based on the equilibrium adsorption capacity at various RHS. The desorption kinetics was obtained by measuring the weight change of the samples with time at 87<inline-formula id="inf5">
<mml:math id="m5">
<mml:mrow>
<mml:mo>&#x2103;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula>. Regeneration of silica gel in multiple adsorption-desorption cycles was also obtained in the system.</p>
</sec>
</sec>
<sec sec-type="results|discussion" id="s3">
<title>Results and discussion</title>
<p>Silica gel as a solid desiccant in a honeycomb rotary wheel is thought to be environmentally friendly and its desiccant capacity is dependent on its surface structure including specific surface area, pore volume, pore size, etc. As such, it is vital to choose a suitable and clean fabrication procedure to tune the surface structure of the silica gel solid desiccant in a honeycomb rotary wheel. Indeed, the surface structure of silica gel is affected by many preparation variables consisting of starting materials, catalyst, reaction temperature and time, aging temperature and time, etc. So, it is difficult to control elaborately the preparation procedure to obtain the desirable silica gel with excellent desiccant capacity (<xref ref-type="bibr" rid="B29">Zhang et al., 2006</xref>; <xref ref-type="bibr" rid="B30">Zheng et al., 2014</xref>). In this work, water glass was used as a green and low-cost raw material for the preparation of silica gel desiccant in a honeycomb rotary by the neutralization of acids. Although it is more difficult to result in the good surface structure of silica gel than organic silicon as a starting material because inorganic salt yielded during the neutralization in the solution impacts greatly the gelatinization of the silica sol, water glass could be used as an adhesive agent for the formation of honeycomb monolith without any other organic adhesive introduction. More importantly, CO<sub>2</sub> gas as the neutralized acid should be able to relieve the salt effect in the solution due to the usage of liquid acid on the gelation of silica sol. As demonstrated in <xref ref-type="fig" rid="F1">Figure 1</xref> for the monolith and the XRD pattern of the as-obtained honeycomb silica gel by the reaction of water glass and CO<sub>2</sub>, it can be seen that there is a weak broadening band at about 23<sup>o</sup> without any diffraction peaks of impurity, revealing the typical amorphous nature of SiO<sub>2</sub> and thus a feasible preparation approach.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>
<bold>(A)</bold> Typical photograph of the as-obtained honeycomb silica gel with CO<sub>2</sub> as the neutralized agent; <bold>(B)</bold> typical XRD pattern of silica gel powder detached from the honeycomb monolith.</p>
</caption>
<graphic xlink:href="fchem-10-1038095-g001.tif"/>
</fig>
<p>
<xref ref-type="fig" rid="F2">Figure 2</xref> shows the SEM images of the obtained honeycomb silica gel at a different state. From <xref ref-type="fig" rid="F2">Figures 2A&#x2013;C</xref>, it can be seen that the prepared silica gel is gelatinized well with a smooth and uniform surface, which could be further verified by the SEM images of the cross section of honeycomb silica gel monolith in <xref ref-type="fig" rid="F2">Figures 2D&#x2013;F</xref>, illustrating the complete reaction of water glass with CO<sub>2</sub> to implement the polymerization between SiO<sub>2</sub> molecules during gelatinization. From <xref ref-type="fig" rid="F2">Figures 2G&#x2013;I</xref>, it is indicated that the prepared silica gel is dispersed evenly between the networks of glass fiber paper, allowing the available maximal exposed surface, which is favorable to promote the adsorption capacity. Although it is not observed obviously the surface microstructure of the prepared silica gel by glass fiber paper as a substrate, the texture of the monolith is indicated to disperse widely the silica gel on fiber gel paper so that the pretty large contact area of the silica gel with vapor for desiccant is obtained, which shall be verified further by the following characterized surface structure including specific surface area, pore volume, pore diameters.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Typical SEM images of the as-obtained honeycomb silica gel with CO<sub>2</sub> as the neutralized agent. <bold>(A&#x2013;C)</bold> Silica gel powder detached from the honeycomb matrix; <bold>(D&#x2013;F)</bold> cross section of honeycomb matrix; and <bold>(G&#x2013;I)</bold> surface of the honeycomb matrix.</p>
</caption>
<graphic xlink:href="fchem-10-1038095-g002.tif"/>
</fig>
<p>To optimize the effect of CO<sub>2</sub> pressure on the surface structure, the preparation of the honeycomb silica gel using water glass as starting material was investigated at different CO<sub>2</sub> pressure at ambient temperature. The nitrogen adsorption and desorption isotherms of the as-obtained honeycomb silica gel are shown in <xref ref-type="fig" rid="F3">Figure 3</xref>. As indicated in <xref ref-type="fig" rid="F3">Figure 3</xref>, all isotherms are identified as the typical Type IV, which are the characteristic isotherms of mesoporous materials at any pressure of CO<sub>2</sub>, preferably used as a desiccant as well. Nonetheless, the different isotherms at different pressure of CO<sub>2</sub> demonstrate the different surface structures of the prepared honeycomb silica gel, displaying the regularity of CO<sub>2</sub> on the surface structure of silica gel with the exception of the acid effect for the neutralization of water glass. As shown in <xref ref-type="fig" rid="F4">Figure 4</xref> for the changed surface structure with CO<sub>2</sub> pressure including the pore size distribution, pore size, and pore volume, it could be seen that the most probable pore size between 2 and 10&#xa0;nm is further evidence of the above typical Type IV BET isotherms of mesoporous materials although the pore size difference with CO<sub>2</sub> pressure is markable, which should be embodied from the accumulative pore volume change with CO<sub>2</sub> pressure. As known generally, the reaction of CO<sub>2</sub> with water glass should be the neutralization of water glass by carbonic acid generated by CO<sub>2</sub> and H<sub>2</sub>O, thus, CO<sub>2</sub> pressure affects the reaction rate due to CO<sub>2</sub> pressure dependence of CO<sub>2</sub> concentration so that the surface structure of the generated silica gel is varied. All the detailed surface structure data of the prepared honeycomb silica gel at different CO<sub>2</sub> were compiled in <xref ref-type="table" rid="T1">Table 1</xref>. From <xref ref-type="table" rid="T1">Table 1</xref>, it is clear that the surface structure of the prepared honeycomb silica gel is varied greatly with CO<sub>2</sub> pressure, which could be explained by the famous Kelvin formula, as shown in the following equation:<disp-formula id="e1">
<mml:math id="m6">
<mml:mrow>
<mml:mi>R</mml:mi>
<mml:mi>T</mml:mi>
<mml:mi>l</mml:mi>
<mml:mi>n</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>P</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:mi>&#x3c3;</mml:mi>
<mml:mi>M</mml:mi>
</mml:mrow>
<mml:mi>&#x3c1;</mml:mi>
</mml:mfrac>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x2212;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>where <italic>R</italic> is the gas constant, <italic>T</italic> is the thermodynamic temperature of the system, <italic>P</italic>
<sub>
<italic>2</italic>
</sub> and <italic>P</italic>
<sub>
<italic>1</italic>
</sub> are the saturated vapor pressure at different curved diameters <italic>R</italic>
<sub>
<italic>2</italic>
</sub> and <italic>R</italic>
<sub>
<italic>1</italic>
</sub>, respectively, <italic>M</italic> is the molar mass of water, <italic>&#x3c1;</italic> is the density of water.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Nitrogen adsorption and desorption isotherms of the as-obtained honeycomb silica gel using water glass as the starting material at different CO<sub>2</sub> pressures.</p>
</caption>
<graphic xlink:href="fchem-10-1038095-g003.tif"/>
</fig>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>BJH (desorption) pore volume and pore size logarithm curves of the as-obtained honeycomb silica gel using water glass as the starting material at different CO<sub>2</sub> pressures.</p>
</caption>
<graphic xlink:href="fchem-10-1038095-g004.tif"/>
</fig>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Surface parameters of the prepared silica gel at different CO<sub>2</sub> pressures.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">CO<sub>2</sub> pressure (MPa)</th>
<th align="left">Specific area (m<sup>2</sup>/g)</th>
<th align="left">Pore volume (ml/g)</th>
<th align="left">Average pore diameter (nm)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">0.10</td>
<td align="left">224.260</td>
<td align="left">0.147</td>
<td align="left">2.817</td>
</tr>
<tr>
<td align="left">0.15</td>
<td align="left">431.483</td>
<td align="left">0.0644</td>
<td align="left">2.563</td>
</tr>
<tr>
<td align="left">0.20</td>
<td align="left">523.207</td>
<td align="left">0.292</td>
<td align="left">4.088</td>
</tr>
<tr>
<td align="left">0.25</td>
<td align="left">764.862</td>
<td align="left">0.447</td>
<td align="left">2.938</td>
</tr>
<tr>
<td align="left">0.30</td>
<td align="left">695.765</td>
<td align="left">0.303</td>
<td align="left">3.316</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>From <xref ref-type="disp-formula" rid="e1">Eq. 1</xref>, it is clear that the saturated vapor pressure at constant temperature is dependent on the pore diameter, and the larger the pore diameter, the larger the saturated vapor pressure. Thus, the adsorption capacity of desiccant is directly related to the pore volume and the specific surface area of desiccant with the average pore diameter of the mesopore (2&#x2013;50&#xa0;nm). Thus, the optimized CO<sub>2</sub> pressure for the preparation of the honeycomb silica gel is about 0.25&#xa0;MPa, which might be contributed to the unique gas acid effect with rapid diffusion.</p>
<p>To investigate the adsorptive characteristic of the prepared honeycomb silica gel, the adsorption/desorption kinetics was carried out at different humidity, as shown in <xref ref-type="fig" rid="F5">Figure 5</xref> for the typical adsorption/desorption kinetics at different humidity for the as-obtained honeycomb silica gel at CO<sub>2</sub> pressure of 0.25&#xa0;MPa. From <xref ref-type="fig" rid="F5">Figure 5</xref>, it can be seen that the prepared silica gel at CO<sub>2</sub> pressure of 0.25&#xa0;MPa exhibits adsorptive ability at different relative humidity, which is indispensable for desiccant dehumidification used in industry due to the hash requirement of products to air humidity. Moreover, it could be further desorpted after saturated adsorption, exhibiting the cycling adsorption/desorption characteristics. The comparative adsorption capacity and time for saturated adsorption of different silica gels prepared at different CO<sub>2</sub> pressure at a relative humidity of 50% were compiled in <xref ref-type="table" rid="T2">Table 2</xref>. In comparison, the silica gel prepared at CO<sub>2</sub> pressure of 0.25&#xa0;MPa shows the best high adsorption capacity and the suitable time for saturated adsorption at the relative humidity of 50%, which is attributed to the optimized surface structure, as shown above.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Typical adsorption/desorption kinetic curve at different humidities for the as-obtained honeycomb silica gel at a CO<sub>2</sub> pressure of 0.25&#xa0;MPa using water glass as the starting material.</p>
</caption>
<graphic xlink:href="fchem-10-1038095-g005.tif"/>
</fig>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Adsorption capacity and time for saturated adsorption of silica gel prepared at different CO<sub>2</sub> pressures at a relative humidity of 50%</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">CO<sub>2</sub> pressure (MPa)</th>
<th align="left">Adsorption capacity (mg/g)</th>
<th align="left">Time for saturated adsorption (min)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">0.10</td>
<td align="left">127.801</td>
<td align="left">517.20</td>
</tr>
<tr>
<td align="left">0.15</td>
<td align="left">194.121</td>
<td align="left">712.67</td>
</tr>
<tr>
<td align="left">0.20</td>
<td align="left">238.286</td>
<td align="left">722.03</td>
</tr>
<tr>
<td align="left">0.25</td>
<td align="left">287.244</td>
<td align="left">721.6</td>
</tr>
<tr>
<td align="left">0.30</td>
<td align="left">264.386</td>
<td align="left">721.25</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec sec-type="conclusion" id="s4">
<title>Conclusion</title>
<p>The honeycomb silica gel in a solid desiccant rotary wheel is fabricated environmentally friendly using water glass as starting material and CO<sub>2</sub> as neutralized acid. Water glass is used as an adhesive agent as well allowing the formation of the honeycomb monolith without any additional organic adhesive agent and guarantees a clean manufacturing procedure. CO<sub>2</sub> could tune the surface structure of silica gel including the specific surface area, pore volume, and pore size due to its rapid diffusion and pressure. The results indicate that the prepared honeycomb silica gel has a large specific surface area of as much as 760&#xa0;m<sup>2</sup>/g, a large pore volume of 0.45&#xa0;ml/g, and suitable mesoporous size of 2.94&#xa0;nm at a CO<sub>2</sub> pressure of 0.25&#xa0;MPa, which allows the excellent performance of the prepared honeycomb silica gel as a solid desiccant with an adsorption capacity of 287.24&#xa0;mg/g at a relative humidity of 50%. Therefore, the proposed green preparation procedure of the honeycomb silica gel as a solid desiccant is feasible and promising in the manufacturing of honeycomb rotary wheels for dehumidification.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="s5">
<title>Data availability statement</title>
<p>The original contributions presented in the study are included in the article/supplementary material; further inquiries can be directed to the corresponding author.</p>
</sec>
<sec id="s6">
<title>Author contributions</title>
<p>JY: writing and experiment design. JQ: experiment. JF: experiment design. CD: experiment. SC: writing and experiment.</p>
</sec>
<ack>
<p>The authors are pleased to acknowledge the funding support by the Wuhan Science and Technology Plan Project (No. 2020020602012123).</p>
</ack>
<sec sec-type="COI-statement" id="s7">
<title>Conflict of interest</title>
<p>JY, JF, and SC were employed by Wuhan Coobase Facilities Company Limited.</p>
<p>The remaining 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="disclaimer" id="s8">
<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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