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dc.contributor.authorDoğan, Mehmet
dc.contributor.authorKalafat, Mehmet Yaşar
dc.contributor.authorKızılduman, Berna Koçer
dc.contributor.authorBicil, Zeynep
dc.contributor.authorTurhan, Yasemin
dc.contributor.authorYanmaz, Ersin
dc.contributor.authorDuman, Betül
dc.date.accessioned2025-05-12T11:05:04Z
dc.date.available2025-05-12T11:05:04Z
dc.date.issued2025en_US
dc.identifier.issn0016-2361 / 1873-7153
dc.identifier.urihttps://doi.org/10.1016/j.fuel.2025.134705
dc.identifier.urihttps://hdl.handle.net/20.500.12462/17228
dc.description.abstractIn this first experimental study, defective fullerenes were produced from fullerenes using a high-rate tungsten carbide mortar ball mill at different rates and times, characterized with different techniques, and their hydrogen storage capacities and kinetic properties were investigated. Structural characterizations showed that the structure, particle size and atomic mass composition of fullerene changed with increasing grinding rate and time, transforming into an amorphous carbonaceous structure. Fullerene decomposed in a single step, while defective fullerenes decomposed in two steps. Significant changes were observed in the morphology and topography of the samples with the formation of defective structures. No regular change was observed in the BET surface areas of the samples, and the sample with the highest BET and pore volume was determined as D-C60-1 h-500 rpm. Parallel to the BET surface area and pore volumes, the D-C60-1 h-500 rpm sample (2.17 wt% at 97 bar) has the highest hydrogen storage capacity. The hydrogen storage capacity of the samples increased with increasing pressure and decreasing temperature. The experimental data were consistent with Henry’s law at room temperature, while at cryogenic temperature, they exhibited a multilayer adsorption isotherm. Adsorptiondesorption isotherms exhibited hysteresis and were in good agreement with the Type IV isotherm. The experimental results showed that hydrogen was also stored in the inner parts of the defective fullerene, and the storage capacity of the defective fullerene was lower than the computational results. Moreover, the experimental data were analyzed by pseudo-first order, pseudo-second order and Elvoich equations, and were in good agreement with the second-order kinetic equation.en_US
dc.language.isoengen_US
dc.publisherElsevieren_US
dc.relation.isversionof10.1016/j.fuel.2025.134705en_US
dc.rightsinfo:eu-repo/semantics/openAccessen_US
dc.subjectDefective Fullereneen_US
dc.subjectGrindingen_US
dc.subjectCharacterizationen_US
dc.subjectHydrogen Storageen_US
dc.subjectKineticsen_US
dc.titleHydrogen storage analysis of fullerene and defective fullerenes: The first experimental studyen_US
dc.typearticleen_US
dc.relation.journalFuelen_US
dc.contributor.departmentFen Edebiyat Fakültesien_US
dc.contributor.authorID0000-0002-3707-0497en_US
dc.contributor.authorID0000-0001-7540-9730en_US
dc.contributor.authorID0000-0002-0826-3556en_US
dc.contributor.authorID0000-0002-5023-947Xen_US
dc.contributor.authorID0000-0002-1657-9366en_US
dc.contributor.authorID0000-0001-5490-9592en_US
dc.identifier.volume390en_US
dc.identifier.issue134705en_US
dc.identifier.startpage1en_US
dc.identifier.endpage23en_US
dc.relation.tubitak"info:eu-repo/grantAgreement/TUBITAK/123Z536"
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US


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