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1.
This paper investigates the decoration of superalkali NLi4 on graphene and the hydrogen storage properties by using first principles calculations. The results show that the NLi4 units can be stably anchored on graphene while the Li atoms are strongly bound together in the superalkali clusters. Decoration using the superalkali clusters not only solve the aggregation of metal atoms, it also provide more adsorption sites for hydrogen. Each NLi4 unit can adsorb up to 10 H2 molecules, and the NLi4 decorated graphene can reach a hydrogen storage capacity 10.75 wt% with an average adsorption energy ?0.21 eV/H2. We also compute the zero-point energies and the entropy change upon adsorption based on the harmonic frequencies. After considering the entropy effect, the adsorption strengths fall in the ideal window for reversible hydrogen storage at ambient temperatures. So NLi4 decorated graphene can be promising hydrogen storage material with high reversible storage capacities.  相似文献   

2.
Two-dimensional (2D) B2O monolayer is considered as a potential hydrogen storage material owing to its lower mass density and high surface-to-volume ratio. The binding between H2 molecules and B2O monolayer proceeds through physisorption and the interaction is very weak, it is important to improve it through appropriate materials design. In this work, based on density functional theory (DFT) calculations, we have investigated the hydrogen storage properties of Lithium (Li) functionalized B2O monolayer. The B2O monolayer decorated by Li atoms can effectively improve the hydrogen storage capacity. It is found that each Li atom on B2O monolayer can adsorb up to four H2 molecules with a desirable average adsorption energy (Eave) of 0.18 eV/H2. In the case of fully loaded, forming B32O16Li9H72 compound, the hydrogen storage density is up to 9.8 wt%. Additionally, ab initio molecular dynamics (AIMD) calculations results show that Li-decorated B2O monolayer has good reversible adsorption performance for H2 molecules. Furthermore, the Bader charge and density of states (DOS) analysis demonstrate H2 molecules are physically absorbed on the Li atoms via the electrostatic interactions. This study suggests that Li-decorated B2O monolayer can be a promising hydrogen storage material.  相似文献   

3.
In this study, we proposed that homo superalkali NM4 clusters with high tetrahedral geometry, can be applied to develop high-performance hydrogen storage materials. Moreover, their special bonding structures and chemical stability make them ideal units for decoration of different kinds of pristine monolayers. We made a trial to decorate the NLi4 clusters onto the 1D graphene nanoribbon, and employed density functional theory (DFT) computational studies to solve its electronic structure, and further evaluate its applicability in hydrogen storage. We found that the electronic charges on Li atoms were successfully transferred to the pristine monolayer, thus a partial electronic field around each Li atom was formed. This subsequently leads to the polarization of the adsorbed hydrogen molecules, and further enhances the electrostatic interactions between the Li atoms and hydrogen. Each NLi4 cluster can adsorb at most 16 hydrogen molecules. For this novel material, its total capacity of hydrogen storage can reach to 11.2 wt %, surpassing the target value of 5.5 wt %, set by the U.S department of energy (DOE) [1], making itself an ideal unit for advanced energy materials design.  相似文献   

4.
The hydrogen storage properties of superalkali NLi4 decorated β12-borophene have been comprehensively investigated based on first-principles density functional calculations (DFT). It is found that the NLi4 cluster can be stably anchored on the surface of β12-borophene because of its large binding energy. The calculated Bader charge population indicates that the charges are transferred from Li atoms to the original monolayer and causes the NLi4 steady adsorbs onto the surface of β12-borophene. For H2 storage, two sides of NLi4 decorated β12-borophene can adsorb up to 24H2 molecules with an ideal H2 adsorption energy of ?0.176 eV/H2. Meanwhile, the hydrogen uptake density achieves 7.66 wt% and surpasses the target of 6.5 wt% from U.S. Department of Energy (DOE). In addition, the adsorption reasons of H2 molecules include the orbital hybridization between H2 and β12-borophene from the calculated projected density of states (PDOS) and the polarization effect of electrostatic field from the calculated charge density difference. We hope this theoretical study can encourage the experimental fabrication for hydrogen storage applications in the near future.  相似文献   

5.
In this article, we have explored the hydrogen (H2) storage capacity of the Li doped B clusters LinB14(n = 1–5) using density functional theory (DFT). The geometrical and Bader's topological parameters indicate that the clusters adsorb H2 in the molecular form. The Li atom polarises the H2 molecules for their effective adsorption on the clusters. The LinB14 (n = 1–5) clusters are found to be stable even after H2 adsorption at room temperature. The average adsorption energy is found to be in the range of 0.12–0.14 eV/H2. Among the various clusters, the Li5B14 shows maximum H2 storage capacity (13.89 wt%) at room temperature. The ADMP simulation reveals that within few femtoseconds (fs), the H2 molecules begin to move away from the clusters and within 400 fs most of the H2 molecules moved away from the clusters.  相似文献   

6.
In this work, we report on the study of the hydrogen storage capability of titanium (Ti) decorated B36 nanosheets using density functional theory (DFT) calculations with van der Waals corrections. Ti atoms are strongly bonded to the surface of B36 with a binding energy of 6.23 eV, which exceeds the bulk cohesive energy of crystalline Ti. Ti-decorated B36 (2Ti@B36) can reversibly adsorb up to 12 H2 molecules with a hydrogen storage capacity of 4.75 wt % and average adsorption energy between 0.361 and 0.674 eV/H2. The values of desorption temperature and the results of molecular dynamics simulations enable to conclude that 2Ti@B36 is a perspective reversible material for hydrogen storage under real conditions.  相似文献   

7.
Based on the first-principles density functional theory, we proposed a stable icosahedral B12-containing core-shell structure of B12@Mg20Al12. The vibrational frequency analysis and the molecular dynamics (MD) simulations indicate the good stability of B12@Mg20Al12 structure. Analysis of the chemical bonding characters shows that there are multi-center two-electron σ bonds formed by p electrons of B and Al atoms and s electrons of Mg atoms, which can form strong connections in the whole B12@Mg20Al12. This can be the powerful evidence of the structural stability. The potential application of B12@Mg20Al12 in hydrogen storage has also been investigated. Calculation results show that about 146 hydrogen molecules, which present a double-shell distribution, can be absorbed at most, corresponding to a high hydrogen capacity of 23.7 wt%, which means the B12@Mg20Al12 can be a promising candidate of high-capacity hydrogen storage materials.  相似文献   

8.
The H2 storage properties of isoreticular metal-organic framework materials (IRMOFs), MOF-5 and IRMOF-10, impregnated with different numbers and types of heterogeneous C48B12 molecules were investigated using density functional theory and grand canonical Monte Carlo (GCMC) calculations. The excess hydrogen adsorption isotherms of IRMOFs at 77 K within 20 bar indicate that suitable number and type of C48B12 molecules play a crucial role in improving the H2 storage properties of IRMOFs. Among the studied pure and nC48B12 (n = 1, 2, 4, 8) in Ci symmetry impregnating into MOF-5, at 77 K under 6 bar, MOF-5-4C48B12 with a 3.5 wt% and 29.9 g/L hydrogen storage density, and at 77 K under 12 bar, the pure MOF-5 with a 4.9 wt% and 31.0 g/L hydrogen storage density has the best hydrogen storage properties. Whereas, among the studied pure and nC48B12 (n = 1, 2, 4, 8) in S6 symmetry impregnating into IRMOF-10, IRMOF-10-8C48B12 always shows the best hydrogen storage properties among the pure and C48B12-impregnated IRMOF-10 at 77 K within 20 bar. IRMOF-10-8C48B12 has a 6.0 wt% and 34.6 g/L hydrogen storage density at 77 K under 6 bar, and has a 7.1 wt% and 41.4 g/L hydrogen storage density at 77 K under 12 bar. The confinement effect of IRMOFs on C48B12 molecules, and steric hindrance effect of C48B12 molecules on IRMOFs mainly affects the H2 uptake capacity by comparing the absolute H2 molecules in individual IRMOFs units, C48B12 molecules, and IRMOFs-nC48B12 compounds. The absolute hydrogen adsorption profiles show that eight C48B12 molecules impregnating into MOF-5 can exert obvious steric effects for H2 adsorption. The saturated gravimetric and volumetric H2 densities of IRMOF-10-8C48B12 higher than those of MOF-5-8C48B12 due to with larger free volume.  相似文献   

9.
In this study, we studied defect-engineering and lithium decoration of 2D phosphorene for effective hydrogen storage using density functional theory. Contrary to graphene, it is found that the presence of point-defects is not preferable for anchoring of H2 molecules over defective phosphorene. According to previous research, strategies such as defect engineering, metal decoration, and doping enhance the hydrogen storage capacity of several 2D materials. Our DFT simulations show that point defects in phosphorene do not improve the hydrogen storage capacity compared to pristine phosphorene. However, selective lithium decoration over the defective site significantly improves the hydrogen adsorption capacity yielding a binding energy of as high as ?0.48 eV/H2 in Li-decorated single vacancy phosphorene. Differential charge densities and projected density of states have been computed to understand the interactions and charge transfer among the constituent atoms. Strong polarization of the H2 molecule is evidenced by the charge accumulation and depletion. The PDOS shows that the presence of Li leads to enhanced charge transfer. The maximum gravimetric density was investigated by sequentially adding H2 molecules to the Li-decorated single vacancy defective phosphorene. The Li-decorated single vacancy phosphorene is found to possess a gravimetric density of around 5.3% for hydrogen storage.  相似文献   

10.
The demand for clean renewable energy is urgent in current. The hydrogen application is difficult mainly due to the ratively low capacity in the storage medium. In this work, the adsorption and desorption of the hydrogen molecules by the Li atoms decorated B38 cage are studied by the density functional theory. The calculated largest binding energy of one Li atom (2.68 eV and 2.58 eV) is upon the hexagonal hole of the B38 cage, which is much larger than the experimental cohesive energy of bulk Li (1.63 eV). Each Li atom in the outside of the B38 cage can adsorb up to four H2 molecules. The Ead of B38(Li-nH2)4 decreases from the 0.22 eV for n = 1 to the 0.11 eV for n = 4. The B38(Li–4H2)4 structure achieves the 6.85 wt% hydrogen gravimetric density, which is higher than the goal of 5.5 wt% before 2017 set by the United States Department of Energy. The almost the same partial density of states for the fifth H2 molecule as that of the isolated H2 molecule, the longer 4.5 Å distance between the fifth H2 molecule and the Li atom, together with the small NBO charges all reveal the weak electronic field around the Li+, which can interpret the weak H2 adsorption mechanism. Finally, the B38Li4 structure can easily release 9H2 molecules at 373 K known from the molecular dynamic simulation and practically trap about 1.08H2 molecules at 373 K/3 atom condition calculated by the grand partition function. Thus, its reversible practical HGD of B38Li4-14.34H2 is 6.18 wt%, which is almost the same value as the theoretical 6.85 wt% for B38(Li–4H2)4. Our studies will be the strong theory basis for the future application in hydrogen storage material development.  相似文献   

11.
The B6Be2 and B8Be2 clusters, adopting fascinating inverse sandwich-like geometries, were recently predicted with quantum chemical calculations. Both systems exhibit the high stability and double aromaticity with 4σ/6π or 6σ/6π delocalized electrons. The hydrogen storage of two systems is studied in the present paper. Our calculations show that B6Be2 and B8Be2 clusters have the ultra-high capacity hydrogen storage, each Be site can bound up with seven H2 molecules, corresponding to a gravimetric density of 25.3 wt percentage (wt%) for B6Be2 and 21.1 wt% for B8Be2, respectively, which far exceeds the target (5.5 wt%) proposed by the US department of energy (DOE) in 2017. The average absorption energies of 0.10–0.45 eV/H2 for B6Be2 and 0.11–0.50 eV/H2 for B8Be2 at the wB97XD level suggest that both systems are ideal for reversible hydrogen storage and release. The reversibility of H2 molecules on B6Be2 and B8Be2 complexes are faithfully demonstrated with the Born-Oppenheimer molecular dynamics (BOMD) simulations. The Be-doped boron nanostructure is a promising candidate for ultra-high hydrogen storage materials.  相似文献   

12.
We have applied ab initio random structure searching to study the structure, stability and hydrogen storage properties of monolayer TiS2 coated with Li and small Li2O clusters. For the low Li covered system we found a complex adsorption mechanism: some hydrogen molecules were adsorbed due to polarization with Li, others due to polarization with S near the surface of TiS2. The peculiarities of the interaction of the H2 molecules with each other and the preferred adsorption sites allowed us to formulate a series of recommendations that can be useful when selecting the material for the most effective support. Moreover, the findings also show that the storage capacity of this system can reach up to 9.63 wt%, presenting a good potential as hydrogen storage material. As for the Li2O clusters supported on TiS2, we found that the polarization of the Li–O bond increases upon the adsorption of the Li2O nanocluster. Moreover, the polarized Li–S bonds appear in addition to the already existing Li–O bonds. All this is possible due to the extraction of 1.46 electrons from the S atom of the substrate by O atom of the cluster, and should contribute to an increase in both the adsorption energy and the maximum capacity. The adsorption energies of H2 for the systems studied here are within 0.11–0.16 eV/H2 which is a recommended range for reversible hydrogen physisorption under standard test conditions. This study may stimulate experimental efforts to check the claims of high-capacity, stable and reversible hydrogen adsorption reported here.  相似文献   

13.
In this work, adsorption of H2 molecules on heteroborospherene C2v C4B32 decorated by alkali atoms (Li) is studied by density functional theory calculations. The interaction between Li atoms and C4B32 is found to be strong, so that it prevents agglomeration of the former. An introduced hydrogen molecule tilts toward the Li atoms and is stably adsorbed on C4B32. It is obtained that Li4C4B32 can store up to 12H2 molecules with hydrogen uptake capacity of 5.425 wt% and average adsorption energy of ?0.240 eV per H2. Dynamics simulation results show that 6H2 molecules can be successfully released at 300 K. Obtained results demonstrate that Li decorated C4B32 is a promising material for reversible hydrogen storage.  相似文献   

14.
The use of hydrogen as a sustainable clean energy source has several benefits, such as reduction in dependency on petroleum fuel and emission of green house gases, and enhanced energy security. The H2 storage properties of Sc grafted calix[4]arene (CX) and octamethylcalix[4]arene (MCX) are investigated by using density functional theory with M06/6-311G(d,p) level of theory. It is observed that Sc strongly binds with benzene rings of CX and MCX through Dewar coordination with average Sc binding energy of 1.09 and 1.25 eV, respectively for CXSc4 and MCXSc4. Each Sc atom adsorbs 4 H2 molecules on both the Sc grafted systems and H2 molecules are bound by Kubas interaction with H2 interaction energy in the range of 0.2–0.5 eV. The calculated conceptual reactivity index shows the stability of the systems increases with number of hydrogen molecules. Hirshfeld charge analysis shows the charge transfer mechanism during H2 adsorption. Born-Oppenheimer molecular dynamics simulations of CXSc4-16H2 and MCXSc4-16H2 systems, show that these systems are stable up to 273 K and all the adsorbed H2 releases at 373 K. The hydrogen storage capacity of Sc grafted CX system is found to be 8.9 wt % and for MCX system is 9.7 wt %. The energy and storage capacity meets the US Department of Energy target, which makes them a propitious hydrogen storage material.  相似文献   

15.
Doping heteroatoms and producing defects are perfect methods to improve the hydrogen storage property of TM-decorated carbon materials. In this view, four novel Sc/Ti-decorated and B- substituted defective C60 fullerenes (B24C24) are explored. The special stability, large specific surface, uniform distribution of the metal and positively charged states make these four fullerenes have high hydrogen storage capacities. Especially, each Sc atom in Sc6B24C24(B4) can adsorb up to five H2 molecules with a storage capacity of 6.80 wt %. The adsorbed H2 molecules in Sc6B24C24(B4)–30H2 begin to relax at 190 K and are 100% released at 290 K. Moreover, a comparative study is carried out for hydrogen storage properties of Sc-decorated B4, C4, or N4 coordination environments. These results provide a new focus on the nature of B-, and N-substituted defective carbon nanomaterials.  相似文献   

16.
Based on the density functional theory, we investigate the electronic properties of the clusters M2B7 (M = Be, Mg, Ca) and their hydrogen storage properties systematically in this paper. Extensive global search results show that the global minimal structures of the three systems (Be2B7, Mg2B7 and Ca2B7) are heptagonal biconical structure, and the two alkaline earth metals are located at the top of the biconical. Chemical bonding analyses show that M2B7 clusters have 6σ and 6π delocalized electrons, which are doubly aromatic. At the wB97XD level, the three systems have good hydrogen storage capabilities. The hydrogen storage density of Be2B7 is as high as 23.03 wt%, while Mg2B7 and Ca2B7 also far exceed the hydrogen storage target set by the U.S. Department of Energy in 2017. Their average adsorption energies of H2 molecules all ranged from 0.1 eV/H2 to 0.48 eV/H2, which is fall in between physisorption and chemisorption. Extensive Born Oppenheimer molecular dynamics (BOMD) simulations show that the H2 molecules of the three systems can be completely released at a certain temperature. Therefore, M2B7 systems can achieve reversible adsorption of H2 molecules at normal temperature and pressure. It can be seen that the B7 clusters modified by alkaline earth metals may become a promising new nano-hydrogen storage material.  相似文献   

17.
Hydrogen storage properties of Li-decorated graphene oxides containing epoxy and hydroxyl groups are studied by using density functional theory. The Li atoms form Li4O/Li3OH clusters and are anchored strongly on the graphene surface with binding energies of −3.20 and −2.84 eV. The clusters transfer electrons to the graphene substrate, and the Li atoms exist as Li+ cations with strong adsorption ability for H2 molecules. Each Li atom can adsorb at least 2H2 molecules with adsorption energies greater than −0.20 eV/H2. The hydrogen storage properties of Li-decorated graphene at different oxidation degrees are studied. The computations show that the adsorption energy of H2 is −0.22 eV/H2 and the hydrogen storage capacity is 6.04 wt% at the oxidation ratio O/C = 1/16. When the O/C ratio is 1:8, the storage capacity reaches 10.26 wt% and the adsorption energy is −0.15 eV/H2. These results suggest that reversible hydrogen storage with high recycling capacities at ambient temperature can be realized through light-metal decoration on reduced graphene oxides.  相似文献   

18.
Combined density functional theory and grand canonical monte Carlo (GCMC) calculations were performed to study the electronic structures and hydrogen adsorption properties of the Zn-based metal-organic framework MOF-650. The benzene azulenedicarboxylate linkers of MOF-650 were substituted by B atoms, N atoms, and boronic acid B(OH)2 linkers, and the Zn atoms were substituted by Mg and Ca atoms. The calculated electronic densities of states (DOSs) of MOF-650 showed that introduction of B atoms reduces the band gap but damages the structure of MOF-650. Introduction of single N bonds cannot provide active electrons to attract H2 molecules. Thus, substitutions of B and N into MOF-650 are not suggested. B(OH)2 substitute in MOF-650 decreased its band gap, slightly improved its hydrogen storage ability and made H2 molecules more intensively distributed besides organic linkers. GCMC calculations were carried out by estimating the H2 storage amount of the pure and modified MOFs at 77 and 298 K and from 1 bar to 20 bar. B(OH)2 linker and Mg/Ca co-doped MOF-650 showed increased H2 adsorption by approximately 20 wt%. The adsorption of H2 around different bonds showed the order N–C < C = C < B–C < C–O < B–O.  相似文献   

19.
The hydrogen adsorption and storage of Cu3Bx (X = 1–4) compounds have been computationally investigated at B3LYP-D3/6-311G (3df, 3pd) level. The most stable compounds of Cu3Bx (X = 1–4) can adsorb 16, 11, 15, and 9 hydrogen molecules with H2 gravimetric densities of 13.80, 9.46, 11.94, 7.20 wt%, respective. Their average adsorption energies are in the range of 0.26–0.43 eV/H2. The Gibbs free energy corrected adsorption energies indicate that the maximum adsorption of Cu3Bx (X = 1–4) are energetically favorable under ambient conditions. Atom-centered density matrix propagation (ADMP) molecular dynamics simulations are used to analyzed the real time dynamics of H2 and Cu3Bx (X = 1–4). We can find that Cu3Bx (X = 1–4) can bind with 4–5 H2 within 1000 fs at 200 K.  相似文献   

20.
A three dimensional (3D) dumbbell-like nanostructure composed by interconnected fullerenes and nanotubes with Lithium decoration and boron-doping (37Li@C139B31) has been proposed in virtue of density functional theory (DFT) and first-principles molecular dynamics (MD) simulations which shows excellent geometric and thermal stability. First-principles calculations are performed to investigate the hydrogen adsorption onto the 37Li@C139B31. The results indicate that B substitution can improve the metal binding and the average binding energy of 37 adsorbed Li atoms on the C139B31 (2.79 eV) is higher than the cohesive energy of bulk Li (1.63 eV) suppressing the clustering. Meanwhile, the H2 storage gravimetric density of 178H2@37Li@C139B31 reaches up to 15.9 wt% higher than the year 2020 target from the US department of energy (DOE). The average adsorption energy of H2 molecules falls in a desirable range of 0.18–0.27 eV. Moreover, grand canonical ensemble Monte Carlo (GCMC) simulations reveal that at room temperature the hydrogen gravimetric density (HGD) adsorbed on 37Li@C139B31 reaches up to 11.6 wt% at 100 bars higher than the DOE 2020 target. Our multiscale simulations indicate that our proposed nanostructure provides a promising medium for hydrogen storage.  相似文献   

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