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Hydrogen Storage Property Study Of H2Molecule Adsorption On LaFeO3(100) Surfaces

Posted on:2013-12-24Degree:MasterType:Thesis
Country:ChinaCandidate:X X LvFull Text:PDF
GTID:2231330374455909Subject:Condensed matter physics
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Alkaline solution of ABO3oxide as electrode materials not only with the higherelectrochemical reaction activity and the discharge capacity, but also the electrochemicalstorage hydrogen phenomenon has certain catholicity. So use the ABO3oxides asnickel-metal hydride batteries anode material has the feasibility, with low cost, easyactivation, high discharge capacity and good chemical stability, ABO3oxides can be appliedin the high energy nickel-metal hydride battery in the future.As Ni-M-H battery cathode material, people have different issues on hydrogen with aproton or atomic state form absorb on the rare earth perovskite-type complex oxides LaFeO3,and after absorption of hydrogen element valence variation problem. So the adsorption of H2on LaFeO3(100) crystal surface and LaFeO3(100) crystal surface with O vacant defect werestudied by first-principles based on the density functional theory (DFT).In chapter3, the adsorption of H2on two kinds of LaFeO3(100) crystal surface arestudied by first principles. Preferred adsorption sites, adsorption energy, dissociation energyand electronic structure of the LaFeO3(100)/H2systems are calculated separately. It is foundthat H2is adsorbed on the hollow site of LaFeO3(100) surface which contains Fe atoms and Oatoms more favorably than on the other sites, while two—OH are formed on the LaFeO3(100) crystal surface. The adsorption energy on the hollow site is2.139eV, belonging tostrong chemical adsorption; The interaction between H2and LaFeO3(100) surface is mainlydue the overlapping among H1s, O2s and O2p states, through which covalent bonds areformed between O and H atoms, the bond length is0.971. H2O is formed after theoptimization of H2adsorbed on the O top sites on two kinds of LaFeO3(100) crystal surfaces,The adsorption energy on the Model Ⅰ O top site is negative. In other words, this adsorptionis unstable, it is easy to form a O vacant site after evaporation of H2O molecule.In chapter4, the adsorption of H2on two kinds of LaFeO3(100) crystal surface with Ovacant defect are studied by first principles. Preferred adsorption sites, adsorption energy,dissociation energy and electronic structure of the LaFeO3(100)/H2systems are calculatedseparately. It is found that H2is adsorbed on the hollow site of LaFeO3(100) surface whichcontains Fe atoms and O atoms more favorably than on the other sites, while two—OH are formed on the LaFeO3(100) crystal surface. The adsorption energy on the hollow site is2.206eV, belonging to strong chemical adsorption; The interaction between H2and LaFeO3(100)surface is mainly due the overlapping among H1s, O2s and O2p states, through whichcovalent bonds are formed between O and H atoms, the bond length is0.971. H2O isformed after the optimization of H2adsorbed on the O top sites on two kinds of LaFeO3(100)crystal surfaces, The adsorption energy on the Model Ⅰ O top site is negative. In other words,this adsorption is unstable, it is easy to form a O vacant site after evaporation of H2Omolecule. Compared with no O vacancy adsorption results, adsorption energy on the moststable structure is increased, it is easy to adsorb on the hollow site; adsorption energy on theO top sites on two kinds of LaFeO3(100) crystal surfaces is decreased, so H2is easy to adsorbon the O vacancy defect LaFeO3(100) and formed–OH with O atomic from crystal surface.
Keywords/Search Tags:first principle, LaFeO3(100), O vacant, H2, adsorption
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