Atomic insights into combustion mechanism of nano‐aluminum hydride
Summary As an important hydrogen storage material, aluminum hydride is widely used in the combustion field. However, the oxidation behavior and potential mechanism of aluminum hydride nanoparticle (AHNP) in the combustion process are not clear. Molecular reactive dynamics was used to explore the oxi...
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Veröffentlicht in: | International journal of energy research 2022-06, Vol.46 (8), p.11079-11091 |
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creator | Zhao, Ying Ma, Deng‐Xue Mei, Zheng Zhao, Feng‐Qi Xu, Si‐Yu Ju, Xue‐Hai |
description | Summary
As an important hydrogen storage material, aluminum hydride is widely used in the combustion field. However, the oxidation behavior and potential mechanism of aluminum hydride nanoparticle (AHNP) in the combustion process are not clear. Molecular reactive dynamics was used to explore the oxidation behavior and mechanism of pure and core‐shell AHNP with different oxide layer thickness, particle size and oxygen concentration. The simulation results show that uneven oxidation of AHNP surface presents branched distribution, and the oxidation process is carried out by the interdiffusion of O and Al. The core Al diffusion coefficient of 40 ps (1.42 × 10−4 cm2/s) is much larger than that of shell O atoms (4.90 × 10−5 cm2/s), indicating that oxidation of core‐shell AHNP is dominated by the uneven diffusion of core Al into the oxide layer driven by an electrostatic force. This leads to the formation of hydrogen gas chamber of different sizes. Mean square displacement shows that core Al tends to diffuse into a thinner oxide layer. The oxide layer inhibits the diffusion of core Al and H, resulting in a slower oxidation rate. The smaller AHNP exhibits a micro‐explosion oxidation accompanied by the formation of small Al clusters, and the reaction process is dominated by aluminum diffusion. The initial reaction of the larger AHNP is mainly concentrated on the surface, the subsequent oxidation processes rely on heterogeneous reactions between the oxidation phase and AlH3. Under lower oxygen concentration, AHNP shows a lower oxidation rate and heat release, where core Al and environment O atoms diffuse toward each other to form a homogeneous OAl phase. Under higher oxygen concentration, the active Al atoms diffuse outward to form a hollow spherical structure. This work provides fundamental insight into the storage and application of AHNP that serve as a high energy density fuel.
The oxide phase on the surface of nano aluminum hydride presents a branched chain distribution.
The oxidation of core‐shell aluminum hydride is dominated by the diffusion of aluminum atoms into the oxide layer.
At low concentration of O2, the oxidation of nano‐aluminum hydride is dominated by bidirectional diffusion of aluminum and O, forming homogeneous oxidation phase during the oxidation process.
At high O2 concentration, the oxidation of nano‐aluminum hydride is mainly aluminum diffusion, and hollow structure is formed during the oxidation process.
Nano‐aluminum hydride with small par |
doi_str_mv | 10.1002/er.7910 |
format | Article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_journals_2676778702</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2676778702</sourcerecordid><originalsourceid>FETCH-LOGICAL-c2190-cb2f0f4a23fe17b7c110d9aba11a7a1d4a9c0d291624e43be563ddf6d619f3833</originalsourceid><addsrcrecordid>eNp10M1KAzEQB_AgCtYqvsKCBw-ydSZZN82x1PoBBUEUegvZfNiU7qYmu0hvPoLP6JO4tV49zcD8-A_8CTlHGCEAvbZxxAXCARkgCJEjFotDMgBWslwAXxyTk5RWAP0N-YDcTtpQe535Jvm3ZZv6pQ2ZDnXVpdaHJqutXqrGpzoLLmtUE74_v9S6q33T1dlya6I39pQcObVO9uxvDsnr3exl-pDPn-4fp5N5rikKyHVFHbhCUeYs8oprRDBCVQpRcYWmUEKDoQJLWtiCVfamZMa40pQoHBszNiQX-9xNDO-dTa1chS42_UtJS15yPuZAe3W5VzqGlKJ1chN9reJWIshdRdJGuauol1d7-eHXdvsfk7PnX_0DRrJn2A</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2676778702</pqid></control><display><type>article</type><title>Atomic insights into combustion mechanism of nano‐aluminum hydride</title><source>Wiley Online Library</source><creator>Zhao, Ying ; Ma, Deng‐Xue ; Mei, Zheng ; Zhao, Feng‐Qi ; Xu, Si‐Yu ; Ju, Xue‐Hai</creator><creatorcontrib>Zhao, Ying ; Ma, Deng‐Xue ; Mei, Zheng ; Zhao, Feng‐Qi ; Xu, Si‐Yu ; Ju, Xue‐Hai</creatorcontrib><description>Summary
As an important hydrogen storage material, aluminum hydride is widely used in the combustion field. However, the oxidation behavior and potential mechanism of aluminum hydride nanoparticle (AHNP) in the combustion process are not clear. Molecular reactive dynamics was used to explore the oxidation behavior and mechanism of pure and core‐shell AHNP with different oxide layer thickness, particle size and oxygen concentration. The simulation results show that uneven oxidation of AHNP surface presents branched distribution, and the oxidation process is carried out by the interdiffusion of O and Al. The core Al diffusion coefficient of 40 ps (1.42 × 10−4 cm2/s) is much larger than that of shell O atoms (4.90 × 10−5 cm2/s), indicating that oxidation of core‐shell AHNP is dominated by the uneven diffusion of core Al into the oxide layer driven by an electrostatic force. This leads to the formation of hydrogen gas chamber of different sizes. Mean square displacement shows that core Al tends to diffuse into a thinner oxide layer. The oxide layer inhibits the diffusion of core Al and H, resulting in a slower oxidation rate. The smaller AHNP exhibits a micro‐explosion oxidation accompanied by the formation of small Al clusters, and the reaction process is dominated by aluminum diffusion. The initial reaction of the larger AHNP is mainly concentrated on the surface, the subsequent oxidation processes rely on heterogeneous reactions between the oxidation phase and AlH3. Under lower oxygen concentration, AHNP shows a lower oxidation rate and heat release, where core Al and environment O atoms diffuse toward each other to form a homogeneous OAl phase. Under higher oxygen concentration, the active Al atoms diffuse outward to form a hollow spherical structure. This work provides fundamental insight into the storage and application of AHNP that serve as a high energy density fuel.
The oxide phase on the surface of nano aluminum hydride presents a branched chain distribution.
The oxidation of core‐shell aluminum hydride is dominated by the diffusion of aluminum atoms into the oxide layer.
At low concentration of O2, the oxidation of nano‐aluminum hydride is dominated by bidirectional diffusion of aluminum and O, forming homogeneous oxidation phase during the oxidation process.
At high O2 concentration, the oxidation of nano‐aluminum hydride is mainly aluminum diffusion, and hollow structure is formed during the oxidation process.
Nano‐aluminum hydride with small particle size exhibits micro‐explosion oxidation.</description><identifier>ISSN: 0363-907X</identifier><identifier>EISSN: 1099-114X</identifier><identifier>DOI: 10.1002/er.7910</identifier><language>eng</language><publisher>Chichester, UK: John Wiley & Sons, Inc</publisher><subject>Aluminium ; Aluminum ; Aluminum hydrides ; atomic diffusion ; Combustion ; Diffusion ; Diffusion coefficient ; Diffusion layers ; Diffusion rate ; Electrostatic properties ; Heat transfer ; Hydrogen storage ; Hydrogen storage materials ; Interdiffusion ; Nanoparticles ; nano‐aluminum hydride ; Oxidation ; oxidation mechanism ; Oxidation process ; Oxidation rate ; Oxygen ; particle size ; Thickness</subject><ispartof>International journal of energy research, 2022-06, Vol.46 (8), p.11079-11091</ispartof><rights>2022 John Wiley & Sons Ltd.</rights><rights>2022 John Wiley & Sons, Ltd.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c2190-cb2f0f4a23fe17b7c110d9aba11a7a1d4a9c0d291624e43be563ddf6d619f3833</citedby><cites>FETCH-LOGICAL-c2190-cb2f0f4a23fe17b7c110d9aba11a7a1d4a9c0d291624e43be563ddf6d619f3833</cites><orcidid>0000-0002-9668-3066</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fer.7910$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fer.7910$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,777,781,1412,27905,27906,45555,45556</link.rule.ids></links><search><creatorcontrib>Zhao, Ying</creatorcontrib><creatorcontrib>Ma, Deng‐Xue</creatorcontrib><creatorcontrib>Mei, Zheng</creatorcontrib><creatorcontrib>Zhao, Feng‐Qi</creatorcontrib><creatorcontrib>Xu, Si‐Yu</creatorcontrib><creatorcontrib>Ju, Xue‐Hai</creatorcontrib><title>Atomic insights into combustion mechanism of nano‐aluminum hydride</title><title>International journal of energy research</title><description>Summary
As an important hydrogen storage material, aluminum hydride is widely used in the combustion field. However, the oxidation behavior and potential mechanism of aluminum hydride nanoparticle (AHNP) in the combustion process are not clear. Molecular reactive dynamics was used to explore the oxidation behavior and mechanism of pure and core‐shell AHNP with different oxide layer thickness, particle size and oxygen concentration. The simulation results show that uneven oxidation of AHNP surface presents branched distribution, and the oxidation process is carried out by the interdiffusion of O and Al. The core Al diffusion coefficient of 40 ps (1.42 × 10−4 cm2/s) is much larger than that of shell O atoms (4.90 × 10−5 cm2/s), indicating that oxidation of core‐shell AHNP is dominated by the uneven diffusion of core Al into the oxide layer driven by an electrostatic force. This leads to the formation of hydrogen gas chamber of different sizes. Mean square displacement shows that core Al tends to diffuse into a thinner oxide layer. The oxide layer inhibits the diffusion of core Al and H, resulting in a slower oxidation rate. The smaller AHNP exhibits a micro‐explosion oxidation accompanied by the formation of small Al clusters, and the reaction process is dominated by aluminum diffusion. The initial reaction of the larger AHNP is mainly concentrated on the surface, the subsequent oxidation processes rely on heterogeneous reactions between the oxidation phase and AlH3. Under lower oxygen concentration, AHNP shows a lower oxidation rate and heat release, where core Al and environment O atoms diffuse toward each other to form a homogeneous OAl phase. Under higher oxygen concentration, the active Al atoms diffuse outward to form a hollow spherical structure. This work provides fundamental insight into the storage and application of AHNP that serve as a high energy density fuel.
The oxide phase on the surface of nano aluminum hydride presents a branched chain distribution.
The oxidation of core‐shell aluminum hydride is dominated by the diffusion of aluminum atoms into the oxide layer.
At low concentration of O2, the oxidation of nano‐aluminum hydride is dominated by bidirectional diffusion of aluminum and O, forming homogeneous oxidation phase during the oxidation process.
At high O2 concentration, the oxidation of nano‐aluminum hydride is mainly aluminum diffusion, and hollow structure is formed during the oxidation process.
Nano‐aluminum hydride with small particle size exhibits micro‐explosion oxidation.</description><subject>Aluminium</subject><subject>Aluminum</subject><subject>Aluminum hydrides</subject><subject>atomic diffusion</subject><subject>Combustion</subject><subject>Diffusion</subject><subject>Diffusion coefficient</subject><subject>Diffusion layers</subject><subject>Diffusion rate</subject><subject>Electrostatic properties</subject><subject>Heat transfer</subject><subject>Hydrogen storage</subject><subject>Hydrogen storage materials</subject><subject>Interdiffusion</subject><subject>Nanoparticles</subject><subject>nano‐aluminum hydride</subject><subject>Oxidation</subject><subject>oxidation mechanism</subject><subject>Oxidation process</subject><subject>Oxidation rate</subject><subject>Oxygen</subject><subject>particle size</subject><subject>Thickness</subject><issn>0363-907X</issn><issn>1099-114X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNp10M1KAzEQB_AgCtYqvsKCBw-ydSZZN82x1PoBBUEUegvZfNiU7qYmu0hvPoLP6JO4tV49zcD8-A_8CTlHGCEAvbZxxAXCARkgCJEjFotDMgBWslwAXxyTk5RWAP0N-YDcTtpQe535Jvm3ZZv6pQ2ZDnXVpdaHJqutXqrGpzoLLmtUE74_v9S6q33T1dlya6I39pQcObVO9uxvDsnr3exl-pDPn-4fp5N5rikKyHVFHbhCUeYs8oprRDBCVQpRcYWmUEKDoQJLWtiCVfamZMa40pQoHBszNiQX-9xNDO-dTa1chS42_UtJS15yPuZAe3W5VzqGlKJ1chN9reJWIshdRdJGuauol1d7-eHXdvsfk7PnX_0DRrJn2A</recordid><startdate>20220625</startdate><enddate>20220625</enddate><creator>Zhao, Ying</creator><creator>Ma, Deng‐Xue</creator><creator>Mei, Zheng</creator><creator>Zhao, Feng‐Qi</creator><creator>Xu, Si‐Yu</creator><creator>Ju, Xue‐Hai</creator><general>John Wiley & Sons, Inc</general><general>Hindawi Limited</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7ST</scope><scope>7TB</scope><scope>7TN</scope><scope>8FD</scope><scope>C1K</scope><scope>F1W</scope><scope>F28</scope><scope>FR3</scope><scope>H96</scope><scope>KR7</scope><scope>L.G</scope><scope>L7M</scope><scope>SOI</scope><orcidid>https://orcid.org/0000-0002-9668-3066</orcidid></search><sort><creationdate>20220625</creationdate><title>Atomic insights into combustion mechanism of nano‐aluminum hydride</title><author>Zhao, Ying ; Ma, Deng‐Xue ; Mei, Zheng ; Zhao, Feng‐Qi ; Xu, Si‐Yu ; Ju, Xue‐Hai</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2190-cb2f0f4a23fe17b7c110d9aba11a7a1d4a9c0d291624e43be563ddf6d619f3833</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Aluminium</topic><topic>Aluminum</topic><topic>Aluminum hydrides</topic><topic>atomic diffusion</topic><topic>Combustion</topic><topic>Diffusion</topic><topic>Diffusion coefficient</topic><topic>Diffusion layers</topic><topic>Diffusion rate</topic><topic>Electrostatic properties</topic><topic>Heat transfer</topic><topic>Hydrogen storage</topic><topic>Hydrogen storage materials</topic><topic>Interdiffusion</topic><topic>Nanoparticles</topic><topic>nano‐aluminum hydride</topic><topic>Oxidation</topic><topic>oxidation mechanism</topic><topic>Oxidation process</topic><topic>Oxidation rate</topic><topic>Oxygen</topic><topic>particle size</topic><topic>Thickness</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Zhao, Ying</creatorcontrib><creatorcontrib>Ma, Deng‐Xue</creatorcontrib><creatorcontrib>Mei, Zheng</creatorcontrib><creatorcontrib>Zhao, Feng‐Qi</creatorcontrib><creatorcontrib>Xu, Si‐Yu</creatorcontrib><creatorcontrib>Ju, Xue‐Hai</creatorcontrib><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Environment Abstracts</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Oceanic Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>Civil Engineering Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Environment Abstracts</collection><jtitle>International journal of energy research</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zhao, Ying</au><au>Ma, Deng‐Xue</au><au>Mei, Zheng</au><au>Zhao, Feng‐Qi</au><au>Xu, Si‐Yu</au><au>Ju, Xue‐Hai</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Atomic insights into combustion mechanism of nano‐aluminum hydride</atitle><jtitle>International journal of energy research</jtitle><date>2022-06-25</date><risdate>2022</risdate><volume>46</volume><issue>8</issue><spage>11079</spage><epage>11091</epage><pages>11079-11091</pages><issn>0363-907X</issn><eissn>1099-114X</eissn><abstract>Summary
As an important hydrogen storage material, aluminum hydride is widely used in the combustion field. However, the oxidation behavior and potential mechanism of aluminum hydride nanoparticle (AHNP) in the combustion process are not clear. Molecular reactive dynamics was used to explore the oxidation behavior and mechanism of pure and core‐shell AHNP with different oxide layer thickness, particle size and oxygen concentration. The simulation results show that uneven oxidation of AHNP surface presents branched distribution, and the oxidation process is carried out by the interdiffusion of O and Al. The core Al diffusion coefficient of 40 ps (1.42 × 10−4 cm2/s) is much larger than that of shell O atoms (4.90 × 10−5 cm2/s), indicating that oxidation of core‐shell AHNP is dominated by the uneven diffusion of core Al into the oxide layer driven by an electrostatic force. This leads to the formation of hydrogen gas chamber of different sizes. Mean square displacement shows that core Al tends to diffuse into a thinner oxide layer. The oxide layer inhibits the diffusion of core Al and H, resulting in a slower oxidation rate. The smaller AHNP exhibits a micro‐explosion oxidation accompanied by the formation of small Al clusters, and the reaction process is dominated by aluminum diffusion. The initial reaction of the larger AHNP is mainly concentrated on the surface, the subsequent oxidation processes rely on heterogeneous reactions between the oxidation phase and AlH3. Under lower oxygen concentration, AHNP shows a lower oxidation rate and heat release, where core Al and environment O atoms diffuse toward each other to form a homogeneous OAl phase. Under higher oxygen concentration, the active Al atoms diffuse outward to form a hollow spherical structure. This work provides fundamental insight into the storage and application of AHNP that serve as a high energy density fuel.
The oxide phase on the surface of nano aluminum hydride presents a branched chain distribution.
The oxidation of core‐shell aluminum hydride is dominated by the diffusion of aluminum atoms into the oxide layer.
At low concentration of O2, the oxidation of nano‐aluminum hydride is dominated by bidirectional diffusion of aluminum and O, forming homogeneous oxidation phase during the oxidation process.
At high O2 concentration, the oxidation of nano‐aluminum hydride is mainly aluminum diffusion, and hollow structure is formed during the oxidation process.
Nano‐aluminum hydride with small particle size exhibits micro‐explosion oxidation.</abstract><cop>Chichester, UK</cop><pub>John Wiley & Sons, Inc</pub><doi>10.1002/er.7910</doi><tpages>13</tpages><orcidid>https://orcid.org/0000-0002-9668-3066</orcidid></addata></record> |
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subjects | Aluminium Aluminum Aluminum hydrides atomic diffusion Combustion Diffusion Diffusion coefficient Diffusion layers Diffusion rate Electrostatic properties Heat transfer Hydrogen storage Hydrogen storage materials Interdiffusion Nanoparticles nano‐aluminum hydride Oxidation oxidation mechanism Oxidation process Oxidation rate Oxygen particle size Thickness |
title | Atomic insights into combustion mechanism of nano‐aluminum hydride |
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