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Inorganic Chemistry
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crystal structure. The total pore volume calculated from the maximum
amount of N2 adsorbed is 0.50 cm3·g−1. The C1 and C2 hydrocarbons
and CO2 adsorption isotherms of PCP-33 at 273 and 298 K have been
collected and fitted (Figure 3). The Langmuir−Freundlich parameters
potential for separation. The predicted CO2/CH4 selectivity, as well as
the C2H2/CO2 selectivity, is around 6−10. In addition, we note that
the equimolar C2H2/C2H4, C2H2/C2H6, and C2H6/C2H4 selectivities
are all close to unity, showing the separation of individual components
of C2 hydrocarbons is difficult. Thus, the IAST calculations in Figure 4
demonstrate high potential for natural gas purification, as well as the
possibility for selective removal of CO2 from C2 hydrocarbons and
separation of C2H2/CO2 mixtures at room temperature.
Isosteric Heat of Adsorption. To understand such high
separation ability better, the adsorption enthalpies were calculated.
The binding energies of C2H2, C2H4, C2H6, and CO2 in PCP-33 are
reflected in the isosteric heat of adsorption, Qst. These values were
determined using the pure component isotherm fits. Figure 5 presents
Figure 3. Comparison of absolute component loadings for CH4, C2
hydrocarbons, and CO2 at 298 K in PCP-33 with the isotherm fits.
for each pure component isotherms in PCP-33 are provided in Table
S1, Supporting Information. The adsorption hierarchies of these five
gases are very distinct, indicating good separability. The total uptake of
C2H2, C2H6, C2H4, CO2, and CH4 in PCP-33 reached 121.8, 102.4,
86.8, 58.6, and 6.9 cm3·g−1, respectively, at 1 bar and 298 K. In
addition, all of the isotherms are completely reversible, and no
hysteresis is observed. Thus, these results motivated us to examine the
potential application of PCP-33 for C1 and C2 hydrocarbon and CO2
separation, given the fact that these five molecules have comparable
molecular sizes (Table S2, Supporting Information).
Figure 5. Isosteric heats of adsorption for C2H2, C2H4, C2H6, and CO2
in PCP-33. The determination of the Qst is based on the Clausius−
Clapeyron equation.
data on the loading dependence of Qst for C2H2, C2H4, C2H6, and CO2
in PCP-33. We note that the binding energies are in the narrow range
of 22−27 kJ mol−1. It is particularly note worthy that the Qst for C2H2
in PCP-33 is about half the value reported for other MOFs with open
metal sites such FeMOF-74, MgMOF-74, CoMOF-74, and CuBTC,42
implying the significantly lower energy consumption during
regeneration of adsorbed C2 hydrocarbons in fixed bed absorbers of
PCP-33. This is because the large pore size (9−22 Å) and organic
counterions of PCP-33 somewhat reduced the heat of adsorption.43
Transient Breakthroughs. We also performed transient break-
through simulations in a fixed bed adsorber to investigate the
separation potential of PCP-33. Such simulations reflect the combined
influences of adsorption selectivity and uptake capacity. The
breakthroughs of an equimolar component mixture including CH4,
C2H2, C2H4, C2H6, and CO2, using the methodology described in
earlier works,44,45 were explored at 298 K. The relative concentrations
of outflowing gas are shown in Figure 6. The simulation results for
transient breakthrough are presented in terms of a dimensionless time τ,
defined by dividing the actual time, t, by the characteristic time (Lε/u).
The breakthrough hierarchy is dictated by the adsorption strengths;
the weaker the adsorption, the earlier the breakthrough.
Adsorption Selectivity. The ideal adsorbed solution theory
(IAST) of Myers and Prausnitz41 was employed to predict
multicomponent adsorption behaviors from the experimental pure-
gas isotherms. Figure 4 presents IAST calculations of the component
Natural gas usually contains CO2 and C2 hydrocarbons that require
removal by selective adsorption. Figure 6a presents simulation results
for equimolar five-component CH4/C2H2/C2H4/C2H6/CO2 mixtures.
The partial pressures of these five gases were set as 20 kPa. It is clear
that pure CH4 can be recovered because it is the least strongly
adsorbed component and elutes first. In addition, the result shown in
Figure 6b demonstrates that after recovery of CH4, the remaining
C2H2/C2H4/C2H6/CO2 mixture can be separated to yield two
fractions: CO2 and C2 hydrocarbons. Thus, we further simulate the
separation behavior of C2H2/CO2, since it is particularly challenging in
view of their similarity molecular dimensions and also boiling point.3
In view of the high selectivity for adsorption of C2H2, it is possible to
recover pure CO2 during the adsorption phase in a fixed bed adsorber
(Figure 6c). In addition, the significant time interval between the
Figure 4. IAST calculations of CH4, C2H2, C2H4, C2H6, and CO2
adsorption selectivities in PCP-33 at 298 K.
loadings for CH4, C2H2, C2H4, C2H6, and CO2 for adsorption of a five-
component equimolar mixture in PCP-33 at 298 K. The IAST
calculations show the following loading hierarchies at 100 kPa. On the
basis of the component loadings, we calculate the selectivities of
separation of the six constituent binary pairs: C2H2/CH4, C2H2/C2H4,
C2H2/C2H6, C2H2/CO2, C2H6/C2H4, and CO2/CH4. The C2H2/CH4
selectivity is the highest and falls in the range of 40−65, indicating the
C
DOI: 10.1021/ic5030058
Inorg. Chem. XXXX, XXX, XXX−XXX