TY - JOUR
T1 - Hydrogen storage properties of C6S6Li6
T2 - A density functional theory study
AU - Tang, Yupeng
AU - Yang, Haiying
AU - Jin, Fan
AU - Li, Nan
N1 - Publisher Copyright:
© 2025, Chinese Chemical Society. All rights reserved.
PY - 2025
Y1 - 2025
N2 - In this paper, the hydrogen storage properties of C6S6Li6 were studied by two density functional methods. C6S6Li6 was dynamically stable and could adsorb up to 38 H2 molecules with a hydrogen storage density of 20.213%. The average adsorption energy of C6S6Li6(H2)38 was very close to the energy range (0.1-⁃0.8 eV) for reversible hydro-⁃ gen storage at near ambient conditions. Various wave function analysis methods revealed that the 2s→2p electron transition of Li in C6S6Li6 and the electric field of each charged atom jointly dominated Van der Waals attractions between C6S6Li6 and hydrogen molecules. Thermo-⁃chemistry calculations indicated that 6, 32, and 38 H2 molecules in C6S6Li6(H2)38 could be readily adsorbed at 77 K and desorbed at 298.15 K under 0.1, 2.5, and 5.0 MPa, respectively. This process corresponds to the reversible hydrogen storage densities of 3.846%, 17.582%, and 20.213%. Atom den-⁃ sity matrix propagation (ADMP) molecular dynamic simulations indicated that most of the hydrogen molecules in C6S6Li6(H2)38 got efficiently released at room temperature. The (C6S6Li6)2 dimer could also adsorb 53 H2 molecules with a gravimetric density of 15.014%. The average adsorption energy for C12S12Li12(H2)53 could approach the revers-⁃ ible energy range for hydrogen storage.
AB - In this paper, the hydrogen storage properties of C6S6Li6 were studied by two density functional methods. C6S6Li6 was dynamically stable and could adsorb up to 38 H2 molecules with a hydrogen storage density of 20.213%. The average adsorption energy of C6S6Li6(H2)38 was very close to the energy range (0.1-⁃0.8 eV) for reversible hydro-⁃ gen storage at near ambient conditions. Various wave function analysis methods revealed that the 2s→2p electron transition of Li in C6S6Li6 and the electric field of each charged atom jointly dominated Van der Waals attractions between C6S6Li6 and hydrogen molecules. Thermo-⁃chemistry calculations indicated that 6, 32, and 38 H2 molecules in C6S6Li6(H2)38 could be readily adsorbed at 77 K and desorbed at 298.15 K under 0.1, 2.5, and 5.0 MPa, respectively. This process corresponds to the reversible hydrogen storage densities of 3.846%, 17.582%, and 20.213%. Atom den-⁃ sity matrix propagation (ADMP) molecular dynamic simulations indicated that most of the hydrogen molecules in C6S6Li6(H2)38 got efficiently released at room temperature. The (C6S6Li6)2 dimer could also adsorb 53 H2 molecules with a gravimetric density of 15.014%. The average adsorption energy for C12S12Li12(H2)53 could approach the revers-⁃ ible energy range for hydrogen storage.
KW - Li cluster
KW - adsorption energy
KW - atom density matrix propagation
KW - density functional theory
KW - hydrogen storage
UR - https://www.scopus.com/pages/publications/105016215640
U2 - 10.11862/CJIC.20240460
DO - 10.11862/CJIC.20240460
M3 - Article
AN - SCOPUS:105016215640
SN - 1001-4861
VL - 41
SP - 1827
EP - 1839
JO - Chinese Journal of Inorganic Chemistry
JF - Chinese Journal of Inorganic Chemistry
IS - 9
ER -