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Hundred helium atoms, which roughly correspond to half of the liquid density in bulk spaces at 4 K, were arranged in the external nanopores of the CNTs.
Both quantities exhibited the best agreement with the calculations including high temperature electron distributions and the liquid density of state, albeit the ambient DOS could not be excluded.
We have calculated the electron-ion coupling parameter using the following relation from the ref. 21 with both the ambient and liquid density of states.
At very high pressure, the density of the fluid can be 90 percent or more of the liquid density.
However, inaccurate liquid density predictions remain a significant deficiency in these equations.
The saturated liquid density follows a decreasing trend with the solubility of methane and ethane.
Here, the filling factor in Fig. 7 is defined as the adsorbed helium densities in the internal nanopores of CNTs divided by the bulk liquid density (120 mg mL−1) at 4 K.
The experimental data of the bubble point pressure and the liquid density were agreed well with the literature.
The bubble point pressure and the liquid density were measured for CO2+PAG-1 at 344.3 K.
The calculation correlations of liquid density and interfacial area were updated by coding Fortran subroutines in Aspen Plus®.
The influences of confinement by pore walls, pore widths, liquid density, and temperature on the self-diffusion coefficient are investigated.
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