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dc.contributor.authorZhang, T
dc.contributor.authorZhang, K
dc.contributor.authorLiu, F
dc.contributor.authorZhao, M
dc.contributor.authorZhang, DZ
dc.date.accessioned2024-02-19T14:00:50Z
dc.date.issued2024-01-14
dc.date.updated2024-02-19T13:16:40Z
dc.description.abstractPhase change materials (PCMs) exhibit considerable potential for utilization in energy storage and temperature regulation applications, primarily attributed to their notable latent heat capacity. Nevertheless, the intrinsically limited thermal conductivity of PCMs necessitates the use of thermal conductivity enhancers (TCEs) that possess adjustable features to compensate for greater heat storage efficiency. Porous structures with flexible design freedom have garnered growing interest in contrast to traditional random foams, owing to their significantly larger surface areas and fully interconnected pore networks. This study fabricated three polar form-designed triply periodic minimal surfaces (TPMS) porous structures using selective laser melting (SLM) based on various radial density gradients, namely the uniform density, the linear gradient, and the Boltzmann gradient. The TPMS porous structures were incorporated as TCEs within a paraffin matrix to form composite TPMS-PCMs. The melting behavior of composite TPMS-PCMs during the charging process was investigated by employing both visual experiments and numerical methods. A thorough analysis was undertaken regarding the progression of solid-liquid phase interfaces, temperature distribution, convection distribution, and heat storage rate to elucidate the mechanisms that contribute to enhanced heat transfer. The findings indicate that the configuration of the density gradient has a notable impact on the melting behavior of composite TPMS-PCMs by tuning heat transfer paths. The heat storage rate of the linear gradient case is the highest among the three, reaching 12.1 W, 1.6 times that of the uniform density case, and twice that of the Boltzmann gradient case. Although the Boltzmann gradient case has the lowest heat storage rate, it demonstrates exceptional performance in terms of temperature uniformity. The average temperature gradient along the radius during melting is 348.6 °C/m, which is only 59% observed in the linear gradient case and 56% in the uniform density case. These findings substantiate the effectiveness of the radial gradient density design in the control of the thermal storage process of composite TPMS-PCMs. They serve as a reference for optimizing thermal storage and temperature control systems that rely on latent heat storage in the future.en_GB
dc.description.sponsorshipNational Natural Science Foundation of Chinaen_GB
dc.description.sponsorshipNatural Science Foundation of Chongqing, Chinaen_GB
dc.identifier.citationVol. 358, article 122630en_GB
dc.identifier.doihttps://doi.org/10.1016/j.apenergy.2024.122630
dc.identifier.grantnumber52305247en_GB
dc.identifier.grantnumber52205250en_GB
dc.identifier.grantnumbercstc2020jcyj-zdxmX0021en_GB
dc.identifier.urihttp://hdl.handle.net/10871/135345
dc.identifierORCID: 0000-0002-1561-0923 (Zhang, David Z)
dc.language.isoenen_GB
dc.publisherElsevieren_GB
dc.rights.embargoreasonUnder embargo until 14 January 2025 in compliance with publisher policyen_GB
dc.rights© 2024 Elsevier Ltd. This version is made available under the CC-BY-NC-ND 4.0 license: https://creativecommons.org/licenses/by-nc-nd/4.0/  en_GB
dc.subjectTriply periodic minimal surfaces (TPMS)en_GB
dc.subjectGradient designen_GB
dc.subjectThermal conductivity enhancer (TCE)en_GB
dc.subjectPhase change material (PCM)en_GB
dc.titleAnalysis of thermal storage behavior of composite phase change materials embedded with gradient-designed TPMS thermal conductivity enhancers: A numerical and experimental studyen_GB
dc.typeArticleen_GB
dc.date.available2024-02-19T14:00:50Z
dc.identifier.issn0306-2619
exeter.article-number122630
dc.descriptionThis is the author accepted manuscript. The final version is available from Elsevier via the DOI in this recorden_GB
dc.descriptionData availability: No data was used for the research described in the article.en_GB
dc.identifier.journalApplied Energyen_GB
dc.rights.urihttps://creativecommons.org/licenses/by-nc-nd/4.0/  en_GB
dcterms.dateAccepted2024-01-04
rioxxterms.versionAMen_GB
rioxxterms.licenseref.startdate2024-01-14
rioxxterms.typeJournal Article/Reviewen_GB
refterms.dateFCD2024-02-19T13:51:42Z
refterms.versionFCDAM
refterms.panelBen_GB


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© 2024 Elsevier Ltd. This version is made available under the CC-BY-NC-ND 4.0 license: https://creativecommons.org/licenses/by-nc-nd/4.0/  
Except where otherwise noted, this item's licence is described as © 2024 Elsevier Ltd. This version is made available under the CC-BY-NC-ND 4.0 license: https://creativecommons.org/licenses/by-nc-nd/4.0/