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Volumn 153, Issue 1, 2010, Pages 72-78

Molecular dynamics simulations of water confined in graphene nanochannels: From ambient to supercritical environments

Author keywords

Graphene slab; High temperature; Hydrophobic confinement; Liquid; Molecular dynamics; Supercritical water

Indexed keywords

ATOMIC VIBRATION; CARBON ATOMS; FORCE FIELDS; HIGH TEMPERATURE; HYDROGEN BONDINGS; HYDROPHOBIC CONFINEMENT; INFRARED SPECTRUM; LENNARD JONES; MICROSCOPIC STRUCTURES; MOLECULAR DYNAMICS SIMULATIONS; NANO CHANNELS; POTENTIAL MODEL; RESIDENCE TIME; ROOM TEMPERATURE; SELF-DIFFUSION COEFFICIENTS; SPECTRAL SHIFT; STRUCTURAL WEAKENING; SUPER-CRITICAL; SUPERCRITICAL CONDITION; SUPERCRITICAL WATER;

EID: 77950019538     PISSN: 01677322     EISSN: None     Source Type: Journal    
DOI: 10.1016/j.molliq.2009.09.015     Document Type: Article
Times cited : (58)

References (58)
  • 25
    • 23944489961 scopus 로고    scopus 로고
    • M.C. Gordillo, G. Nagy, J. Martí, J. Chem. Phys. 123 (2005) 054707(1-9).
    • M.C. Gordillo, G. Nagy, J. Martí, J. Chem. Phys. 123 (2005) 054707(1-9).
  • 36
    • 77950020079 scopus 로고    scopus 로고
    • The thin region between 5 and 7.5 Å at room temperature was called an intermediate region in a previous work [8] and analyzed separately, although the main structural - molecular orientations, hydrogen-bond distributions - dielectric and dynamical properties of water in such a region were found to be qualitatively the same as those of water located in the central, bulk-like area. In addition, that third region quickly vanishes when temperature increases, having almost disappeared at 400 K (see Fig. 2).
    • The thin region between 5 and 7.5 Å at room temperature was called an intermediate region in a previous work [8] and analyzed separately, although the main structural - molecular orientations, hydrogen-bond distributions - dielectric and dynamical properties of water in such a region were found to be qualitatively the same as those of water located in the central, bulk-like area. In addition, that third region quickly vanishes when temperature increases, having almost disappeared at 400 K (see Fig. 2).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.