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The excess adsorption isotherms of methane for different temperatures (pore size of 4 nm) are listed in Fig. 7.
The excess adsorption isotherms of methane for different mole fractions of nitrogen are shown in Fig. 13.
Open image in new window Fig. 7 Excess adsorption isotherms of methane for different temperatures (pore size of 4 nm).
Excess adsorption isotherms of methane for different mole fractions of carbon dioxide are shown in Fig. 16.
Open image in new window Fig. 11 Excess adsorption isotherms of methane for different water contents Open image in new window Fig. 12 Potential energy distribution curves of methane and chlorite for different water contents.
Open image in new window Fig. 8 Average isosteric heats of methane for different temperatures (pore size of 4 nm) Open image in new window Fig. 9 Potential energy distribution curves of methane and chlorite at different temperatures (pore size of 4 nm).
Similar(54)
In this study, grand canonical Monte Carlo (GCMC) simulation was used to investigate temperature effect on methane adsorption capacity and adsorbed methane density for different sized pores.
The potential energy distribution curves of methane and chlorite for different water contents are shown in Fig. 12.
Open image in new window Fig. 13 Excess adsorption isotherms of methane on chlorite for different mole fractions of nitrogen.
Open image in new window Fig. 6 Potential energy distribution curves of methane and chlorite for different pressures (pore size of 4 nm) (a) and different pore sizes (pressure of 20 MPa) (b).
It can be seen that the most probable potential energy of methane and chlorite for different carbon dioxide mole fractions was higher than that of carbon dioxide, suggesting that the potential energy distribution between methane and chlorite was different from that between carbon dioxide and chlorite.
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