• Acta Physica Sinica
  • Vol. 69, Issue 6, 068802-1 (2020)
Li-Hua Yuan1、*, Ji-Jun Gong1, Dao-Bin Wang1, Cai-Rong Zhang1, Mei-Ling Zhang1、3, Jun-Yan Su1, and Long Kang2
Author Affiliations
  • 1School of Sciences, Lanzhou University of Technology, Lanzhou 730050, China
  • 2School of Material Science and Engineering, Lanzhou University of Technology, Lanzhou 730050, China
  • 3School of Nuclear Science and Technology, Lanzhou University, Lanzhou 730000, China
  • show less
    DOI: 10.7498/aps.69.20190694 Cite this Article
    Li-Hua Yuan, Ji-Jun Gong, Dao-Bin Wang, Cai-Rong Zhang, Mei-Ling Zhang, Jun-Yan Su, Long Kang. Hydrogen storage capacity of alkali metal atoms decorated porous graphene[J]. Acta Physica Sinica, 2020, 69(6): 068802-1 Copy Citation Text show less
    Optimized geometry structure of a alkaline metal atom decorated PG: (a) Li-PG; (b) Na-PG; (c) K-PG.
    Fig. 1. Optimized geometry structure of a alkaline metal atom decorated PG: (a) Li-PG; (b) Na-PG; (c) K-PG.
    Optimized geometry structure of the Li-PG with H2 molecules adsorption. Red digits represent the corresponding bond length of H—H.
    Fig. 2. Optimized geometry structure of the Li-PG with H2 molecules adsorption. Red digits represent the corresponding bond length of H—H.
    Optimized geometry structure of the Na-PG with H2 molecules adsorption. Red digits represent the corresponding bond length of H—H
    Fig. 3. Optimized geometry structure of the Na-PG with H2 molecules adsorption. Red digits represent the corresponding bond length of H—H
    Optimized geometry structure of the K-PG with H2 molecules. Red digits represent the corresponding bond length of H—H
    Fig. 4. Optimized geometry structure of the K-PG with H2 molecules. Red digits represent the corresponding bond length of H—H
    Partial density of states (PDOS) of a H2 molecule on (a) Li-PG and (b) Na-PG.
    Fig. 5. Partial density of states (PDOS) of a H2 molecule on (a) Li-PG and (b) Na-PG.
    Charge density differences of n H2 adsorbed on Li-PG system for (a) n = 1 and (b) n = 4. The isovalue is taken to be 0.01 e/Å3
    Fig. 6. Charge density differences of n H2 adsorbed on Li-PG system for (a) n = 1 and (b) n = 4. The isovalue is taken to be 0.01 e/Å3
    Charge density differences of a H2 adsorbed on Na-PG (a) and K-PG (b) system. The isovalue is taken to be 0.01 e/Å3.
    Fig. 7. Charge density differences of a H2 adsorbed on Na-PG (a) and K-PG (b) system. The isovalue is taken to be 0.01 e/Å3.
    Optimized geometry structure of the Li-decorated PG with 12 H2 adsorption.
    Fig. 8. Optimized geometry structure of the Li-decorated PG with 12 H2 adsorption.
    Equilibrated structure of the 12 H2-Li-PG (a) and fluctuations of total energy as a function of simulation time (b) in AIMD simulations at 300 K.
    Fig. 9. Equilibrated structure of the 12 H2-Li-PG (a) and fluctuations of total energy as a function of simulation time (b) in AIMD simulations at 300 K.
    n(H2)
    1234
    ΔEad /eV –0.308–0.239–0.249–0.044
    $\Delta {\bar E_{{\rm{ad}}}}$/eV·H2–1–0.308–0.274–0.266–0.225
    q /e 1.231.401.561.56
    Table 1. Adsorption energies (ΔEad) and average adsorption energies ( )of H2 molecules, and the charge of Li (q).
    n(H2)
    123
    ΔEh1/eV –0.202–0.262–0.215
    ΔEh2/eV –0.234–0.117–0.166
    Table 2. [in Chinese]
    Li-Hua Yuan, Ji-Jun Gong, Dao-Bin Wang, Cai-Rong Zhang, Mei-Ling Zhang, Jun-Yan Su, Long Kang. Hydrogen storage capacity of alkali metal atoms decorated porous graphene[J]. Acta Physica Sinica, 2020, 69(6): 068802-1
    Download Citation