Hui
Xu
ab,
Yabing
He
b,
Zhangjing
Zhang
c,
Shengchang
Xiang
c,
Jianfeng
Cai
a,
Yuanjing
Cui
a,
Yu
Yang
a,
Guodong
Qian
*a and
Banglin
Chen
*ab
aState Key Laboratory of Silicon Materials, Cyrus Tang Center for Sensor Materials and Applications, Department of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China. E-mail: gdqian@zju.edu.cn
bDepartment of Chemistry, University of Texas at San Antonio, One UTSA Circle, San Antonio, Texas 78249-0698, USA. E-mail: banglin.chen@utsa.edu; Fax: +1 210-458-7428
cCollege of Chemistry and Materials, Fujian Normal University, 3 Shangsan Road, Cangshang Region, Fuzhou, China 350007
First published on 16th October 2012
To immobilize both open metal and Lewis basic pyridyl sites into a microporous metal–organic framework, Cu6(PDC)6·2.6H2O (UTSA-50) was solvothermally synthesized and characterized. The combination of open metal sites and Lewis basic pyridyl functional sites leads to a high acetylene adsorption enthalpy of 39.4 kJ mol−1. As a result, UTSA-50 is a very promising MOF material for the highly selective separation of C2H2/CH4 and C2H2/CO2 at room temperature with the highest C2H2/CH4 separation selectivity of 68 ever reported and moderately high acetylene uptake of 91 cm−1 g−1.
Recently we have paid much attention to porous MOFs for the storage and separation of hydrocarbons because of their very important industrial applications, particularly acetylene storage and separation.3,24–38 Acetylene is a very important raw material for the synthesis of various industrial chemicals and consumer products, and for oxy-acetylene cutting in metal fabrication;39–41 and the high-purity acetylene is highly in need.42–44 The traditional cryogenic distillation separation technology for the separation of C2H2 from CO2 and CH4 is very energy consuming; the realization of effective new separation materials by adsorptive separation will significantly reduce the cost to produce high purity acetylene. Although some progress has been made on porous MOFs for the separation of C2H2/CH4 and C2H2/CO2 at room temperature, the MOFs with both high separation capacities and selectivity for these gas molecules have not been revealed.1–37 Maximization of both separation capacities (mainly determined by the gas storage capacities) and separation selectivity (mainly determined by the specific functional sites and size exclusive effect) is very important while very challenging. For example, a few porous MOFs exhibiting high acetylene storage capacities have low C2H2/CH4 and C2H2/CO2 separation selectivity,34–,35 while the UTSA-15 (Cu(bdc-OH)(4,4′-bipy)) has the highest C2H2/CH4 separation selectivity of 56, but low acetylene uptake of only 34 cm−1 g−1 at room temperature and 1 atm.37 In these examined MOF materials, only one of the important factors (either open metal sites, optimized pore/cage sizes, size exclusive effects or specific binding sites) has been implemented into porous MOFs to reach their acetylene separation capacities and selectivity, limiting their power to optimize both separation capacities and selectivity.3,25–38 We speculate that if those of the above mentioned important factors can be simultaneously incorporated into porous MOFs and then collaboratively utilized to maximize their acetylene separation capacities and selectivity, we should be able to realize some more promising porous MOF materials for acetylene separation with both high separation capacities and selectivity at room temperature. Herein we report the first example of such porous MOFs Cu6(PDC)6·2.6H2O (UTSA-50, PDC = 3,5-pyridine-dicarboxylate) with both open Cu2+ and Lewis basic pyridyl sites and suitable pore sizes for highly selective separation of C2H2/CH4 and C2H2/CO2 at room temperature with the highest C2H2/CH4 separation selectivity of 68 and moderately high acetylene uptake of 91 cm−1 g−1.
In order to remove guest solvent molecules in the framework, a freshly prepared sample of UTSA-50 was exchanged with acetone 10 times and then activated at 373 K under high vacuum for 12 h until the outgas rate was <5 μm Hg min−1 prior to measurements to get the activated UTSA-50a for gas sorption studies. The sorption measurement was maintained at 77 K with liquid nitrogen and 273 K with an ice-water bath, respectively. As the center-controlled air condition was set up at 296 K, a water bath of 296 K was used for adsorption isotherms at 296 K.
Isotherm data were analysed using the virial equation:19
ln(n/p) = A0 + A1n + A2n2 + … |
As shown in the previous work,18 the 3D framework of UTSA-50 is composed of paddle wheel dinuclear Cu2 units which are connected with eight neighboring Cu2 units by PDC ligands (Fig. 1b). It is worth noting that Cu1 atoms show one open metal site by the removal of terminal waters after the thermal activation, while Cu2 atoms are coordinated with four O atoms and one N atom coming from PDCs to give a pyramid. PDCs show two different coordination modes as shown in Fig. 1a and b, in which PDC-1 has two carboxylate binding sites and one uncoordinated pyridine N site, highlighting the existence of Lewis basic pyridyl sites. Therefore, two types of pores extending along the c direction are formed, which are walled by PDC-1 and PDC-2 (Fig. 1c), respectively. The void space accounts for approximately 57.1% of the whole crystal volume (2402.0 Å3 out of the 4205.9 Å3 per unit cell volume) by PLATON analysis. The combined feature of the open metal sites, Lewis basic pyridyl sites and optimized pore size highlights the potential strong binding and high storage of gas molecules. The N2 sorption isotherm at 77 K showed that UTSA-50a displayed type-I sorption behaviour with a BET surface area of 604 m2 g−1 (Langmuir surface area, 933 m2 g−1) (Fig. 2a).
Fig. 1 Single crystal structure of UTSA-50 indicating (a) PDCs showing two different coordination modes; (b) one paddle-wheel dinuclear Cu2 unit linking with eight Cu2 units through two PDC-1 ligands and three PDC-2 ligands; and Cu1 with open metal sites; (c) two types of pores: a large pore walled by a PDC-1 ligand of about 4 × 4 Å2 and a small pore walled by PDC-2 of about 3.6 × 3.6 Å2 (Cu1, yellow; Cu2, light blue; N, blue; O, red; C, gray; H, white); and (d) a 3D topology with Schläfli symbol {384105862}. |
Fig. 2 (a) N2 sorption isotherm at 77 K and C2H2 (blue), CO2 (red) and CH4 (green) sorption isotherms of UTSA-50a at (b) 273 K and (c) 296 K. Solid symbols: adsorption, open symbols: desorption. |
The above structural feature of UTSA-50 encourages us to examine its potential application in gas storage. As shown in Fig. 2, UTSA-50a can take the amount of C2H2 (113.9 cm3 g−1), CO2 (100.1 cm3 g−1) and CH4 (29.2 cm3 g−1) at 1 atm and 273 K; and C2H2 (90.6 cm3 g−1), CO2 (64.4 cm3 g−1) and CH4 (18.8 cm3 g−1) at 1 atm and 296 K.
The amount of absorbed C2H2 in UTSA-50a at 296 K is lower than similar structured MOFs with high density open metal sites,25,26 such as HKUST (201 cm3 g−1), NOTT-101 (184 cm3 g−1) and UTSA-20 (150 cm3 g−1). This could mainly be attributed to the lower surface area in UTSA-50a than in HKUST (1401 m2 g−1), NOTT-101 (2930 m2 g−1) and UTSA-20 (1894 m2 g−1). However, this value is comparable with the ones with small pores such as Cu2(NDC)2(DABCO) (97 cm3 g−1) and Zn2(NDC)2(DABCO) (106 cm3 g−1), which represent the best C2H2 adsorption property among the MOFs with low surface areas and small pores;20,25 but it is significantly higher than the ones with large pores such as MOF-5 (26 cm3 g−1) and ZIF-8 (25 cm3 g−1) with large surface areas.25 It is worth noting that the storage density of adsorbed acetylene in UTSA-50a micropores is 0.30 g cm−3, which is comparable with HKUST and MOF-74-Fe,23,25 and is among the high end for MOF materials. This illustrates that the combined feature of open metal sites, Lewis basic pyridyl sites and optimized pore size do lead to the efficient adsorption of acetylene molecules in UTSA-50 micropores. The comparison of some microporous MOFs for acetylene storage is listed in Table 1.
Material | Surface area (BET) [m2 g−1] | Pore volume [cm3 g−1] | C2H2 uptake [cm3 g−1] | Density of adsorbed C2H2a [g cm−3] |
---|---|---|---|---|
a Calculated density of adsorbed acetylene in micropores. b H8L = tetrakis[(3,5-dicarboxyphenoxy)methyl]methane. | ||||
UTSA-50 | 604 | 0.35 | 91 | 0.30 |
Cu2(ndc)2(dabco)20 | — | 0.44 | 97 | 0.26 |
Cu2(adc)2(dabco)20 | — | 0.28 | 82 | 0.34 |
Zn2(ndc)2(dabco)20 | — | 0.52 | 106 | 0.24 |
Zn2(adc)2(dabco)20 | — | 0.31 | 101 | 0.38 |
HKUST25 | 1401 | 0.76 | 201 | 0.31 |
MOF-74-Fe23 | 1350 | 0.63 | 156 | 0.29 |
UMCM-150 (ref. 26) | 3330 | 1.21 | 129 | 0.12 |
PCN-16 (ref. 26) | 2810 | 1.00 | 176 | 0.20 |
MOF-5 (ref. 25) | 3610 | — | 26 | — |
ZIF-8 (ref. 25) | 1758 | — | 25 | — |
NOTT-101 (ref. 26) | 2930 | 1.05 | 184 | 0.20 |
NOTT-102 (ref. 26) | 3590 | 1.28 | 146 | 0.14 |
UTSA-20 (ref. 26) | 1894 | 0.67 | 150 | 0.26 |
UTSA-33a 27 | 660 | 0.37 | 84 | 0.26 |
UTSA-34b 28 | 991 | 0.54 | 121 | 0.26 |
UTSA-35a 29 | 743 | 0.31 | 65 | 0.24 |
UTSA-36a 30 | 495 | 0.33 | 57 | 0.20 |
UTSA-38a 33 | 1090 | 0.61 | 64 | 0.12 |
Cu2(ebtc)34 | 1852 | 1.00 | 160 | 0.19 |
Cu4Lb,35 | 1115 | 0.61 | 154 | 0.29 |
Zn4(OH)2(1,2,4-btc)2 (ref. 36) | 408 | 0.22 | 53 | 0.28 |
Cu(bdc-OH)(4,4′-bpy)37 | 553 | 0.28 | 35 | 0.14 |
The coverage-dependent adsorption enthalpies of UTSA-50a for the three gases were calculated based on the virial method, which is a well-established and reliable methodology fitting from their adsorption isotherms at 273 K and 296 K, as listed in Table 2 and Fig. S2–S7.† The enthalpies at zero coverage are 39.4, 27.8 and 18.6 kJ mol−1 for C2H2, CO2 and CH4, respectively. Note that the adsorption enthalpy for C2H2 is significantly higher than MOF-505 (24.7 kJ mol−1) and HKUST (30.4 kJ mol−1) with high density open metal sites.25 This indicates that the high density of Lewis basic pyridyl sites and optimized pore sizes do further enhance the affinity between the MOF surface and C2H2 molecules, presumably by the H–CC–H…N (PDC) hydrogen bonding. Moreover, the adsorption enthalpy for C2H2 is more than 10 kJ mol−1 and 20 kJ mol−1 larger than that for CO2 and CH4, respectively. The most remarkable feature of UTSA-50a is the significantly higher Henry's law selectivities of 68.0 and 13.3 for C2H2/CH4 and C2H2/CO2, respectively at 296 K. To the best of our knowledge, the C2H2/CH4 separation selectivity of 68.0 is the highest one ever reported.3,25–38 The highly selectivity sorption for C2H2/CH4 and C2H2/CO2 and moderately high acetylene storage capacities highlight the promise of UTSA-50 in the practical acetylene separation.
Adsorbate | T/K | A 0 (In(mol g−1 Pa−1) | A 1 (g mol−1) | R 2 | K H (mol g−1 Pa−1) | S i/CH4 | S i/CO2 | Q st,n=0 (kJ mol−1) |
---|---|---|---|---|---|---|---|---|
a The Henry's law selectivity for gas component i over CH4 at the speculated temperature is calculated based on the equation Sij = KH(i)/KH(j). b The Henry's law selectivity for gas component i over CO2 at the speculated temperature is calculated based on the equation Sij = KH(i)/KH(j). | ||||||||
C2H2 | 273 | −12.706 | −1007.788 | 0.993 | 3.033 × 10−6 | 139 | 19.8 | 39.4 |
296 | −14.054 | −675.568 | 0.987 | 7.878 × 10−7 | 68 | 13.3 | ||
CO2 | 273 | −15.691 | −357.548 | 0.996 | 1.533 × 10−7 | 7.0 | 1.0 | 27.8 |
296 | −16.641 | −314.583 | 0.998 | 5.928 × 10−8 | 5.0 | 1.0 | ||
CH4 | 273 | −17.642 | −455.174 | 0.996 | 2.179 × 10−8 | 1.0 | — | 18.6 |
296 | −18.278 | −408.011 | 0.999 | 1.153 × 10−8 | 1.0 | — |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c2ta00155a |
This journal is © The Royal Society of Chemistry 2013 |