Inorganic Chemistry
Article
Figure 4. (a) CO2, CH4, and N2 sorption isotherms of Cu-1 at 273 and 298 K. (b) C2H2, C2H4, and C2H6 sorption isotherms of Cu-1 at 273 and
298 K.
irregular channels with an approximate size of 7.9 × 3.8 Å2
along the [110] direction (Figure 1b,c). With the help of
PLATON, the solvent-accessible void space of Cu-1 was
calculated as 53.7%, which was occupied by free methanol
molecules. From the perspective of topology, the TIA2− ligands
can be regarded as 3-connected nodes, and the paddle wheel
can be simplified as 6-connected nodes (Figure 1d). Therefore,
the structure of Cu-1 can be described as a new 3,6-connected
apo framework.
It is worth noting that the channel wall of Cu-1 is modified
by polar triazole rings that can be regarded as active sites,
which can strengthen the interactions between the framework
and the polar gases of small molecules such as CO2 and C2H2.
Thus, the adsorption capacity and selectivity of these gases can
be enhanced.
Stabilities of Cu-1. Powder X-ray diffraction (PXRD) and
thermogravimetric analysis (TGA) experiments were con-
ducted to confirm the stability of the MOF Cu-1. As can be
seen from Figure 2a, the framework of Cu-1 has outstanding
acid−base stability, which can remain invariant in a wide range
of pH = 2−13. In addition, the temperature-dependent PXRD
pattern (Figure 2b) and TGA curve (Figure S2) confirm that
the framework also has excellent thermal stability, which can
withstand high temperature up to 260 °C, and the structure of
Cu-1 starts to collapse when the temperature is above 300 °C.
Therefore, Cu-1 has excellent thermal and chemical stability,
which is the basis for the following adsorption and separation
experiments.
excellent CO2 uptake capacity of 128.77 cm3·g−1 at 298 K and
1 bar, which is higher than the reported recorded value of bio-
MOF-11 (92 cm3·g−1).56 In addition, the CO2 loading at 273
K and 1 bar of Cu-1 is 180.05 cm3·g−1; it also set a very
excellernt value for CO2 adsorption compared with the
reported highest uptake of NOTT-101 (164 cm3·g−1).57,58
The excellent adsorption properties of Cu-1 for CO2 can be
ascribed to its higher surface area, multiple pores, the matching
effect of micropoles, the size of the CO2 molecule, and the
introduction of 1H-triazole rings in H2TIA, which can
strengthen the affinity between the framework and CO2.
Furthermore, Cu-1 exhibits a low adsorption capacity for CH4
(41.37 cm3·g−1 at 273 K and 26.07 cm3·g−1 at 298 K) and N2
(11.46 cm3·g−1 at 273 K and 9.81 cm3·g−1 at 298 K) under the
condition of 1 bar. For the sake of detecting the interaction
between gases and the framework of the MOF Cu-1, the
isoteric heat of adsorption (Qst) of CO2, N2, and CH4 was
obtained based on the adsorption isotherms at 273 and 298 K
with the help of a virial equation. As exhibited in Figure 5, the
Gas Sorption Properties. N2 sorption−desorption
isotherms of the activated Cu-1 were obtained to verify the
permanent porosity. The results are exhibited in Figure 3, a
typical reversible type I isotherm behavior with a breakthrough
uptake at P/P0 < 0.01, explaining the characteristics of the
micropores. At 77 K, the maximum uptake of N2 reached 270
cm3·g−1, and the corresponding Brunauer−Emmett−Teller
(BET) and Langmuir surface areas were calculated as 766 and
1117 m2·g−1, respectively. In addition, it can be seen in Figure
3b that there exist two kinds of pore systems. The large BET
surface areas and various pore sizes inspire us to study the Cu-
1 adsorption performance for small-molecule gases, such as
CO2, N2, CH4, and C2 hydrocarbons (C2H2, C2H4, and C2H6).
The single-component sorption isotherms of CO2, CH4, and
N2 for Cu-1 at 273 and 298 K up to 1 bar (Figure 4) were
collected to explore the abilities for adsorption and separation
for these gases. As presented in Figure 4a, Cu-1 has a very
Figure 5. Qst relationship of CO2, C2H2, C2H4, C2H6, CH4, and N2
adsorption for Cu-1 estimated from virial expression fits at 273 and
298 K.
Qst value of CO2 near zero loading is 27.6 kJ·mol−1; it slowly
rises to 32 kJ·mol−1 following and increase of the adsorption
capacity. For CH4 and N2, the zero-loading Qst values are 16.4
and 16.3 kJ·mol−1, respectively (Figure 5).
It is well-known that the selective adsorption and separation
of light hydrocarbons play a vital role in the development of
petrochemical enterprises. Considering the microporous
characteristics of the MOF Cu-1, single components of C2
hydrocarbons (C2H2, C2H4, and C2H6) were also carried out at
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Inorg. Chem. 2021, 60, 6550−6558