Jing-Hong
Li
,
Jun-Xian
Chen
,
Rui-Biao
Lin
* and
Xiao-Ming
Chen
*
Key Laboratory of Bioinorganic and Synthetic Chemistry of Ministry of Education, School of Chemistry, IGCME, Sun Yat-Sen University, Guangzhou 510275, China. E-mail: linruibiao@mail.sysu.edu.cn; cxm@mail.sysu.edu.cn
First published on 25th August 2023
The separation of gaseous hydrocarbons is involved in many important industrial processes for manufacturing chemicals, polymers, plastics, and fuels, and is performed through cryogenic distillation, which is heavily energy-intensive. Adsorption-based gas separation technology by using adsorbent materials can potentially fulfill a much energy-efficient gas separation. As a new generation of adsorbent materials, metal–organic frameworks (MOFs) have been demonstrated to have great potential in addressing important gas separations of hydrocarbons. In this review, we outline the uniqueness of MOF adsorbents for their separation application for gaseous hydrocarbons. A variety of microporous MOFs have been developed for separating gaseous hydrocarbons, which have been achieved by fine-tuning their pore sizes for high molecular sieving effects and/or immobilizing binding sites on their pore surfaces for their specific recognition of small molecules. Herein, we highlight recent important progress in this very important topic, focusing on the purification of ethylene, propylene, and butadiene.
Metal–organic frameworks (MOFs, also known as porous coordination polymers) are an emerging type of crystalline porous solids, which are assembled by metal-containing nodes and organic linkers or struts through coordination bonds to have pore space. MOFs are unique owing to their exceptional porosity, diverse structures, tunable pore size, and ease of functionality.3–6 After two decades of intensive practices, MOF materials are well demonstrated for their exceptional capability for pore adjustment and interior modification. Today, about 100000 of MOFs have been synthesized. MOFs can show ultrahigh porosity with the largest pore surface area of over 7000 m2 g−1, or with pore sizes ranging from 3 to 100 Å, the highest thermal stability of over 600 °C, or exceptional chemical stability in concentrated acidic/basic solutions.3,7,8 The high modularity of MOFs enables us to construct their isostructural analogues of different pore sizes/shapes and surfaces (such as functional organic groups, metal open sites, etc.) with the same coordination networks. The key design element for MOFs is thus to functionalize their pore surface with binding sites and/or adjust their pore size/shape for molecular separation. In this context, MOFs have shown great promise that is superior to conventional porous materials (activated carbon and zeolites) in addressing important separations of gaseous hydrocarbons.9–19
For separation processes in physical adsorbents, their separation mechanism can be roughly categorized into either equilibrium or non-equilibrium adsorption. Equilibrium adsorption processes are thermodynamic and are mainly driven by binding affinity differences dominated by those functional sites (i.e., binding sites) through supramolecular interactions. Pore functionalization with strong binding sites can significantly boost such type of separation performance. For non-equilibrium adsorption processes,20 including kinetic separation and molecular sieving, the separation is achieved by differing the diffusivity, which is highly affected by the pore sizes and flexibility of adsorbents. The kinetic separation can be amplified after narrowing the pores of adsorbents. There are also cases that the separation is achieved by a combination of both thermodynamic and kinetic processes. In addition, there are gas separation processes that are usually performed with the collaboration of framework flexibility and structural transformation, namely, gate-opening or pore opening. Considering all aspects, it is very important to systematically control the pore size, pore surface and even the flexibility of adsorbents.
On the other hand, hydrocarbons are composed of the same elements with different carbon bonds and carbon/hydrogen ratios. Their physical properties and even chemical properties can be very similar (Table 1). The adsorptive separation by differing their molecular shapes or adsorption affinities in physical adsorbents is thus required to perform with high accuracy, which can be achieved by MOFs.13 For example, compared with the mixture counterpart propane, propylene, as one major petrochemical product, differs by just two hydrogen atoms, and there is around a 5 K difference in their boiling points. It has been demonstrated that MOFs with embedded binding sites (ranging from open metal sites to polar functional groups, such as anionic fluoride, hydroxyl and amino) can effectively separate olefins/paraffins owing to the difference in thermodynamic affinity. Another applicable approach is to adjust the pore sizes of MOFs for size-matching of gas molecules, which is expected to enhance kinetic separation or sieving effect and finally achieve high selectivity. If the pore aperture size of adsorbents is right between the molecular sizes of different gas components, an adsorption cut-off happens along with the inaccessibility of internal pore space to certain gas components, thus leading to molecular sieving. For some MOFs, the adjustment of pore size in MOFs can be done up to a precision level of 0.1 Å.13 Given that most hydrocarbon gases have their molecular sizes or kinetic diameters between 3 and 5 Å, microporous MOFs with comparable pore sizes have been intensively investigated for separating hydrocarbon mixtures. Usually, MOFs with large pores can show high sorption capacity but low separation selectivity for gas, whereas the ultramicroporous ones can exhibit high selectivity but low sorption capacity (termed sorption capacity versus selectivity trade off). By simultaneously tuning the pore size and incorporating binding sites, the internal pore space of MOFs can integrate molecular shape matching and preferential binding toward the targeted gas molecules, which is expected to address the trade-off for exceptional separation performance. The complicated effects of MOF flexibility for separation of hydrocarbons have also been noted.21
Adsorbate | Normal boiling point/K | Density/g L−1 (101.325 kPa, 273.15 K) | Kinetic diameter/Å | Polarizability × 1025/cm3 | Dipole moment × 1018/esu cm | Quadruple moment × 1026/esu cm2 |
---|---|---|---|---|---|---|
a Density at 298.15 K. | ||||||
CH4 | 111.66 | 0.717 | 3.758 | 25.93 | 0 | 0 |
C2H4 | 169.42 | 1.261 | 4.163 | 42.52 | 0 | 1.50 |
C2H6 | 184.55 | 1.355 | 4.443 | 44.3–44.7 | 0 | 0.65 |
C2H2 | 188.40 | — | 3.3 | 33.3–39.3 | 0 | — |
C3H6 | 225.46 | 1.914 | 4.678 | 62.6 | 0.366 | — |
C3H8 | 231.02 | 2.011 | 4.3–5.118 | 62.9–63.7 | 0.084 | — |
c-C3H6 | 240.34 | 1.920 | 4.23–4.807 | 56.6 | 0 | — |
i-C4H10 | 261.34 | 2.689 | 5.278 | 81.4–82.9 | 0.132 | — |
i-Butene | 266.25 | — | 4.84 | 8.14–8.29 | — | — |
1-Butene | 266.92 | — | 4.5 | 79.7–85.2 | 0.359–0.438 | — |
1,3-Butadiene | 268.62 | — | 5.2 | 86.4 | 0 | — |
n-C4H10 | 272.66 | 2.704 | 4.687 | 82.0 | 0.05 | — |
trans-2-Butene | 274.03 | — | — | 84.9 | 0 | — |
cis-2-Butene | 276.87 | — | 4.23 | — | 0.253 | — |
neo-C5H12 (2,2-dimethylpropane) | 282.65 | 2.334 (70.922 kPa) | 6.2–6.464 | 102.0 | 0 | — |
i-C5H12 | 300.99 | 1.120 (34.543 kPa) | 5.0 | — | 0.13 | — |
n-C5H12 | 309.22 | 0.789 (24.455 kPa) | 4.5 | 99.9 | 0 | — |
neo-C6H14 (2,2-dimethylbutane) | 322.87 | — | 6.2 | — | — | — |
i-C6H14 (2-methylpentane) | 333.40 | 0.343 (8.960 kPa) | 5.5 | — | 0.1 | — |
3-Methylpentane | 336.40 | — | 5.5 | — | — | — |
n-C6H14 | 341.88 | 0.231 (6.041 kPa) | 4.3 | 119 | 0 | — |
C6H6 | 353.24 | 0.403a (12.695 kPa) | 5.349–5.85 | 100–107.4 | 0 | — |
c-C6H12 (cyclohexane) | 353.93 | 0.446a (13.019 kPa) | 6.0–6.182 | 108.7–110 | 0 | — |
n-C7H16 | 371.57 | 0.067 (15.250 kPa) | 4.3 | 136.1 | 0 | — |
i-C8H18 (2,2,4-trimethylpentane) | 372.39 | — | 6.2 | 154.4 | 0 | — |
Toluene | 383.79 | 0.037 (0.906 kPa) | 5.25 | 118–123 | 0.375 | — |
Ethylbenzene | 409.36 | — | 5.8 | 142 | 0.59 | — |
p-Xylene | 411.53 | — | 5.8 | 137–149 | 0.1 | — |
m-Xylene | 412.34 | — | 6.8 | 142 | 0.37 | — |
o-Xylene | 417.59 | — | 6.8 | 141–149 | 0.640 | — |
By virtue of pore structural and chemical control of MOF materials, namely, tuning pore size, incorporating functional sites, or their combination, significant progress has been made for gaseous hydrocarbon separation. This review focuses on the research progress of MOF materials for separation of gaseous hydrocarbons in about recent five years. In particular, we summarize representative MOF materials with unique pores and functional sites for C2H2 and CO2 separation, C2H2/C2H4 separation, C2H4 and C2H6 separation, C3H4/C3H6 separation, C3H6/C3H8 separation, and purification of butadiene, xylenes and other volatile gaseous hydrocarbons.
Materials | Gas separation | Strategies | Uptakea (mmol g−1) | Selectivityb | Ref. |
---|---|---|---|---|---|
a Uptake amount at 1 bar and room temperature. b Calculated by IAST at ambient temperature and 1 bar. c Kinetic selectivity at ambient temperature. d Equilibrium-kinetic combined selectivity at ambient temperature. e Uptake amount at 1.05 bar and 333 K. f Uptake amount at 1.05 bar and 393 K. g Uptake amount at 7.1 mbar and 333 K. | |||||
ATC-Cu | CH4/N2 | Incorporating adjacent open copper sites | 2.9/0.75 | 9.7 | 23 |
Ni(ina)2 | Optimizing pore sizes (5.0 × 4.8 Å2) | 1.82/0.53 | 15.8 | 24 | |
DMOF-A2 | Optimizing pore sizes (5.3 Å) and incorporating parallel aromatic rings | 1.65/0.39 | 7.2 | 25 | |
MAF-92 | CO2/CH4 | Optimizing pore sizes (5.0 × 4.8 Å2) | 2.06/0.06 | 1.3 × 107 | 27 |
CuI@UiO-66-(COOH)2 | C2H4/C2H6 | Optimizing pore sizes (4.1 Å) and incorporating copper(I) ions onto the pore surfaces | 1.9/0.9 | 80.8 | 41 |
UTSA-280 | Optimizing pore rigidity and pore size (3.8 Å) | 2.5/0.098 | >10000 | 35 | |
Co-gallate | Optimizing pore size (5.2 Å) | 3.37/0.31 | 52 | 36 | |
ZnAtzPO4 | Optimizing pore structure (3.8 Å) and incorporating electronegative functional groups | 1.92/1.04 | 36.6c/12.4d | 39 | |
ZU-901 | Optimizing pore size (3.4 × 4.2 Å2) | 1.55/0.26 | — | 40 | |
MAF-49 | C2H6/C2H4 | Incorporating multiple hydrogen-bonding acceptors and dipole repulsion groups | 1.7/1.69 | 2.7 | 59 |
Cu(Qc)2 | Optimizing pore size (3.3 Å) | 1.85/0.78 | 3.4 | 60 | |
[Fe2(O2)(dobdc)] | Incorporating Fe-peroxo sites | 3.29/2.6 | 4.4 | 61 | |
SIFSIX-2-Cu-i | C2H2/C2H4 | Optimizing pore size (4.4 Å) and incorporating SiF62− sites | 4.02/2.19 | 44.8 | 70 |
UTSA-200a | Optimizing pore size (3.4 Å) and incorporating SiF62− sites | 3.65/0.63 | 6320 | 71 | |
UTSA-300a | Optimizing pore size (1.3 × 2.8 Å2) and incorporating SiF62− sites | 3.08/0.04 | 27 | 72 | |
NCU-100a | Optimizing pore size (1.4 × 3.0 Å2) and incorporating SiF62− sites | 4.57/0.32 | 7291 | 76 | |
UTSA-74 | C2H2/CO2 | Incorporating open Zn sites | 4.82/3.03 | 9 | 101 |
CuI@UiO-66-(COOH)2 | Incorporating copper(I) ions onto the pore surfaces | 2.44/0.85 | 185 | 107 | |
JNU-4 | Incorporating open Cu sites | 9.82/7.1 | 8.2 | 108 | |
CPL-1-NH2 | Incorporating amine sites | 1.84/0.21 | 119 | 114 | |
CAU-10-H | Suitable pore sizes (4.7 Å) | 4.01/2.68 | 4 | 115 | |
CAU-10-NH2 | Suitable pore sizes (3.8 Å) and incorporating amine sites | 3.57/2.08 | 10.8 | 116 | |
FJU-90 | Pore space partition | 8.04/4.6 | 4.3 | 122 | |
UTSA-300a | Optimizing pore size (1.3 × 2.8 Å2) and incorporating SiF62− sites | 3.08/0.18 | 860 | 72 | |
NCU-100a | Optimizing pore size (1.4 × 3.0 Å2) and incorporating SiF62− sites | 4.57/0.49 | 1787 | 125 | |
FJI-H36 | Suitable pore sizes (12.9 × 12.9 Å2 and 8.4 × 10.2 Å2), flexible pore structure, incorporating Ni and free N atoms sites | 6.46/4.20 | 3.5 | 127 | |
SOFOUR-TEPE-Zn | Incorporating electronegative pore surfaces | 3.98/0.63 | 16833 | 97 | |
ZUL-330 | Optimizing pore size (3.3 × 3.7 Å2) and incorporating SiF62− sites | 7.33/1.1 | 10086 | 98 | |
Cu-F-pymo | CO2/C2H2 | Incorporating residual guest molecules blocking the priority site for C2H2 | 2.09/0.1 | >105 | 143 |
Cd-NP | Suitable pore space (6.1 × 4.5 × 4.5 Å3), window size (3.2 Å) and incorporating complementary electrostatic potentials on the pore surface | 2.59/0.43 | 85 | 144 | |
Y-bptc | Incorporating large pore cage space (pore diameter: 9.46 Å), suitable pore window (4.2 Å) and μ3-OH− anions sites | 2.48/1.17 | 4.1/114c | 136 | |
MUF-4 | Suitable pore window size (2.2 Å) | 3.17/— | 3363c | 139 | |
ALF | Incorporating electropositive surface and the hydrogen-confined pore cavities with appropriate dimensional size (4.1 × 5.3 Å2) | 3.85/0.15 | 6.5 × 105 | 148 | |
MAF-23-O | C3H6/C3H8 | Incorporating carbonyl oxygen atoms sites | 1.34/1 | 8.8/71c | 149 |
UTSA-400 | Optimizing pore sizes (3.0 Å) and incorporating WO2F42− sites | 1.84/0.05 | >107 | 151 | |
Y-abtc | Optimizing pore sizes (4.7 Å) | 2/0.07 | — | 152 | |
HIAM-301 | Optimizing pore sizes (4.6 Å) | 3.16/0.27 | 150 | 153 | |
Co-gallate | Optimizing pore sizes (4.2 × 5.1 Å2) | 1.79/0.14 | 333 | 154 | |
JNU-3a | Incorporating orthogonally arrayed dynamic apertures | 2.62/2.14 | 513 | 155 | |
NTU-85 | Optimizing pore sizes (4.5 Å) | 0.45/0.003 | 1570 | 156 | |
ZJU-75a | Suitable pore sizes (4.1 × 4.4 Å2) and incorporating high-density open Ni sites | 3.31/2.33 | 54.2 | 157 | |
PCP-IPA | C3H8/C3H6 | Suitable pore sizes (4.7 × 5.6 Å2) and incorporating parallel-aligned aromatic-based units | 2.23/2.25 | 2.48 | 169 |
FDMOF-2 | Optimizing pore sizes (3.0 Å) and incorporating –CF3 groups | 5.04/4.15 | 2.18 | 170 | |
ELM-12 | C3H4/C3H6 | Suitable pore cavities (6.1 × 4.3 × 4.3 Å3 and 6.8 × 4.0 × 4.2 Å3) and incorporating dynamic dangling OTf− groups | 2.79/1.45 | 83 | 181 |
UTSA-200 | Optimizing pore size (3.4 Å) and incorporating SiF62− sites | 3.58/1.20 | >20000 | 182 | |
sql-NbOFFIVE-bpe-Cu-AB | Optimizing pore size (3.96 × 5.56 Å2) and incorporating NbOF52− sites | 3.04/2.10 | 220 | 189 | |
ZU-52 | C4H6/n-C4H8/i-C4H8 | Optimizing pore size (4.31 Å) and incorporating fluoroniobate sites | 2.64/2.26/0.48 | — | 192 |
ZU-33 | Optimizing pore size (4.20 Å) and incorporating GeF62−sites | 2.67/0.57/0.42 | — | ||
MAF-23 | i-C4H8/n-C4H8/C4H10/C4H6 | Incorporating flexible quasi-discrete pores | 2/2/2/2 | — | 193 |
Zn-bzc-2CH3 | n-C4H10/i-C4H10 | Optimizing pore size (4.13 Å) | 2.42/0.03 | — | 195 |
Zr-abtc | nHEX/3MP/23DMB | Suitable pore window size (4.5 Å) | 1.28/1.02/0.58 | — | 197 |
HIAM-203 | nHEX/3MP/22DMB | Suitable pore window size (4.8 Å) | 1.7/1.43/0.07 | — | 198 |
CopzNi | nHEX/2MP/22DMB | Incorporating open Ni sites | 2.17/1.46/0.08 | — | 199 |
Mn-dhbq | pX/mX/oX | Incorporating multiple open Mn sites, rich π-electrons, and structural flexibility | 1.74/1.48/0.22e | — | 206 |
1.33/0.16/0.21f | |||||
ZU-61 | Incorporating adaptable pore structure and NbOF52− sites | 3.44/3.37/3.2g | — | 207 | |
ZUL-C3 | pX/mX/oX/EB | Incorporating nonaromatic low-polar pore environment | 3.25/3.35/3.41/3.27 | — | 208 |
MAF-41 | EB/ST/Tol/Bz | Incorporating structural flexibility | 2.31/0.3 | — | 209 |
Ma et al. used an alkyl MOF, Cu2(ATC) (ATC-Cu, H2ATC = 1,3,5,7-adamantane tetracarboxylic acid), as a methane nano-trap that features oppositely adjacent open metal sites (OMSs) and dense alkyl groups for capturing methane molecules.23 At 1 bar and 298 K, this MOF exhibits the highest methane uptake capacity (2.90 mmol g−1) among reported MOFs, showing a high CH4/N2 selectivity of 9.7 for an equimolar mixture under ambient conditions. ATC-Cu thus shows promising potential for capturing methane from CBM with low content of methane (<30%). Structural and computational modelling indicated that pairs of open Cu sites with a Cu⋯Cu distance of 4.43 Å between two neighboring Cu paddlewheels afford considerable dual Coulombic interactions and act as strong binding sites for methane molecules. Also, there are cavities with an aliphatic surface that can serve as the second binding sites for CH4, with an average interaction distance of ca. 3.5 Å.
Yang et al. studied four nickel-based coordination networks with functional sites (–NH2) or varied pore sizes for the separation of CH4/N2, which supports that the pore size and chemical environment of adsorbents play an important role during methane purification.24 Among those four MOFs, Ni(ina)2 showed the highest CH4/N2 selectivity (15.8) with an adsorption capacity of 1.82 mmol g−1 under ambient conditions. Ni(ina)2 shows good thermal and moisture stability as well, which can be easily scaled up at a low cost.
The influence of humidity on the separation performances of MOFs for CH4 separation has been noticed. Li et al. investigated a series of isostructural MOFs, [Zn2(1,4-NDC)2(DABCO)], [Zn2(ADC)2(DABCO)], [Ni2(ADC)2(DABCO)], and [Cu2(ADC)2(DABCO)] (namely, DMOF-N, DMOF-A1, DMOF-A2, DMOF-A3, respectively, H21,4-NDC = 1,4-naphthalenedicarboxylic acid, H2ADC = 9,10-anthracene dicarboxylic acid, and DABCO = 1,4-diazabicyclo[2.2.2]octane), for CH4 purification.25 Altering their aromatic moieties and/or metal centers results in varied pore sizes, hydrophobicity and stability. The hydrophobic pore space suppressed the water sorption and enhanced the moisture resistance of those MOFs, which show high CH4 uptakes and CH4/N2 selectivity. Breakthrough experiments for the CH4/N2 mixture under humid conditions indicated that their CH4/N2 separation performance can be retained even under high humidity (40% RH).26
Zhang et al. reported two isostructural flexible metal-azolate frameworks (abbreviated as MAFs, a subclass of MOFs with azolate ligands19) [Zn3(OH)2(pzdc)(tz)]·DMA and [Zn3(OH)2(pzdc)(atz)]·DMA (MAF-91·DMA and MAF-92·DMA, respectively, H3pzdc = 3,5-pyrazoledicarboxylic acid, Htz = 1,2,4-triazole, and Hatz = 3-amino-1,2,4-triazole), which possess quasi-discrete pores with analogous sizes (MAF-91·DMA: 3.6 × 2.4 and 4.0 × 2.1 Å2, and MAF-92·DMA: 3.7 × 1.3 and 4.0 × 2.1 Å2).27 Due to the stronger intra-framework hydrogen-bonding interaction in MAF-92, there is a higher gating energy than MAF-91. Thus, MAF-92 showed tremendous shrinkage of apertures (1.0 × 0.8 and 2.5 × 1.0 Å2) after guest removal, while those in MAF-91 (3.5 × 2.2 and 4.4 × 2.0 Å2) showed negligible changes (Fig. 1). Single-component gas adsorption revealed that MAF-92 can adsorb a large amount of CO2 (2.1 mmol g−1 at 273 K and 1 bar), but completely excludes N2 and CH4. The molecular sieving performance was further confirmed by breakthrough experiments for CO2/N2 and CO2/CH4, giving selectivities of >1500. This work revealed that the controlled gated barrier can be expected to achieve definite and ideal molecular sieve effect. In contrast, the very commonly encountered framework flexibility of MOFs could be an important drawback to size-dependent molecular sieving for separation of similar molecules.
Fig. 1 (a) and (c) Crystal structures of MAF-91 and MAF-92. (b) CO2, CH4, and N2 adsorption isotherms of MAF-91 and MAF-92 at 298 K. (d) Column breakthrough behaviors of MAF-92 for 10:90 CO2/N2, 10:90 CO2/CH4 and 10:90 CO2/He mixtures. Reprinted with permission from ref. 27. Copyright 2021 Cell Press. |
Usually, the introduction of OMSs on the pore surface of MOFs enables preferential adsorption of C2H4 over C2H6.28–33,38,41–44 For example, HKUST-128 and M2(dobdc)29–31 (M-MOF-74; M = Mg, Mn, Fe, Co, Ni, and Zn) exhibit stronger binding enthalpies for olefins than alkanes due to the metal–π interactions. Altering the charge density of the metal centers can improve the olefin adsorption and selectivity as revealed by M2(dobdc) isomers.33 The appropriate aperture combined with OMSs of high density can also significantly improve the bonding affinity for olefins. In 2020, Qian et al. reported two microporous MOFs functionalized with different amounts of carboxylate groups, in which the carboxylate groups not only can adjust the aperture size, but also chelate with copper(I) ions via post-synthetic modification.41 Therefore, CuI@UiO-66-(COOH)2 exhibits optimal apertures and exposed Cu(I) centers to form a strong binding affinity for C2H4, while suppressing the adsorption of C2H6. Compared with other UiO-66 materials, CuI@UiO-66-(COOH)2 showed the highest ideal adsorbed solution theory (IAST) selectivity of 80.8 for an equimolar C2H4/C2H6 mixture at 298 K and 1 bar.
Molecular sieves can show the maximum C2H4/C2H6 selectivity via molecular size exclusion, though it is quite challenging due to their similar molecular sizes. In 2018, Chen et al. reported a rigid ultramicroporous MOF [Ca(C4O4)(H2O)] (UTSA-280, H2C4O4 = squaric acid) with one-dimensional (1D) pore channels for molecular sieving separation of C2H4/C2H6. UTSA-280, being assembled by calcium oxide chains and squarate linkers, shows 1D pores with the minimum cross-sectional area of 14.4 Å2, which falls precisely between the sizes of C2H4 and C2H6 (13.7 Å2 and 15.5 Å2, respectively). Therefore, UTSA-280 can adsorb C2H4 with an adsorption capacity of 2.5 mmol g−1 at 298 K and 1 bar while blocking the diffusion of the relatively large C2H6 molecules (Fig. 2).35 The C2H4/C2H6 selectivity of UTSA-280 was estimated to be over 10000. The adsorption heat (Qst) of UTSA-280 for C2H4 ranges from 20.5 to 35.0 kJ mol−1, which is lower than those of MOFs with OMSs (40–85 kJ mol−1).30,45 Breakthrough experiments confirmed that high purity (>99.2%) of C2H4 can be obtained from an equimolar C2H4/C2H6 mixture with a productivity of 1.86 mmol g−1. It is worth noting that UTSA-280 is capable of efficiently capturing C2H4 from a quaternary CH4/C2H4/C2H6/C3H8 mixture (45/25/25/5). Dispersion-corrected density functional theory (DFT-D) calculations and single-crystal X-ray diffraction experiments revealed that C2H4 molecules are adsorbed by UTSA-280 in a linear array with weak C–H⋯O hydrogen bonding, π⋯π stacking and van der Waals (vdW) interactions.
Fig. 2 (a) Structure of UTSA-280. (b) Sorption isotherms of UTSA-280 for C2H4 and C2H6 at 298 K. (c) Breakthrough curves for UTSA-280 from different scales for an equimolar mixture of C2H4/C2H6 at 298K and 1bar. Reprinted with permission from ref. 35. Copyright 2018 Nature Publishing Group. |
In 2018, Ren et al. reported a series of gallate-based MOFs, [M(C7O5H4)·2H2O] (termed M-gallates, M = Mg, Ni, and Co), for C2H4/C2H6 separation with high sieving effect.36 These MOFs contain 3D interconnected zigzag channels and have Brunauer–Emmett–Teller (BET) surfaces of ca. 424 (Ni), 559 (Mg), and 475 (Co) m2 g−1. The pore sizes (3.47–3.69 Å) of these MOFs are close to the molecular sizes of C2H4 (3.28 × 4.18 × 4.84 Å3) and C2H6 (3.28 × 4.18 × 4.84 Å3). Therefore, M-gallates could highly selectively adsorb C2H4 over C2H6. Among them, Co-gallate displays the highest performance for separation of C2H4/C2H6. The C2H4 uptake capacity of Co-gallate is much higher than that for C2H6 (3.37 mmol g−1vs. 0.31 mmol g−1), resulting in a high IAST selectivity of 52 at 298 K and 1 bar for an equimolar C2H4/C2H6 mixture. The IAST selectivity of Mg-gallate is about 37.3 for an equimolar C2H4/C2H6 mixture at 298 K and 1 bar. Breakthrough experiments for a 50/50 C2H4/C2H6 mixture further demonstrated the excellent C2H4/C2H6 separation performances of these low-cost M-gallates.
In 2020, Xing et al. reported a phosphate-pillared MOF, [Zn3(atz)3(PO4)]n (ZnAtzPO4, Hatz = 3-amino-1,2,4-triazole), for C2H4/C2H6 separation with high selectivity (12.4 at 298 K and 32.4 at 273 K).39 Single-component gas adsorption and kinetic studies revealed that ZnAtzPO4 has a higher C2H4 adsorption capacity (1.92 mmol g−1) than for C2H6 (1.04 mmol g−1) at 298 K and 1 bar, as well as a faster adsorption rate for C2H4 compared with C2H6, giving a kinetic selectivity of 36.6. DFT calculations demonstrated that electronegative groups decorated on the narrow pore apertures of ZnAtzPO4 can effectively capture C2H4 and inhibit the diffusion of C2H6, resulting in an efficient equilibrium-kinetic C2H4/C2H6 separation. A flexible ultra-microporous MOF, [Cu2(pyz-CH3)(pzdc)2] (ZU-901, pyz-CH3 = 2-methylpyrazine, and H2pzdc = 2,3-pyrazinedicarboxylic acid), with a pore size of 3.4 × 4.2 Å2 was recently reported to show a C2H4 adsorption–desorption curve in an S shape with high C2H4 working capacity and facile regeneration.40 Single-component sorption experiments showed that ZU-901 can adsorb 1.55 mmol g−1 C2H4 and much less C2H6 (0.26 mmol g−1) at 298 K and 1 bar. The adsorption selectivity of ZU-901 calculated for the pressure swing adsorption (PSA) process is 65. The Qst of ZU-901 for C2H4 was calculated to be ∼25 kJ mol−1, which indicates that ZU-901 can be mildly regenerated. The simulated two-bed PSA process revealed that polymer-grade ethylene (ca. 99.5%) can be obtained by ZU-901 with only 1/10 of the energy consumption compared to simulating cryogenic distillation (2.03 kJmol−1vs. 21.84 kJmol−1).
For C2H4-selective MOF materials, multiple adsorption and desorption cycles are typically required to achieve high-purity ethylene. In contrast, C2H6-selective adsorbents can directly give pure ethylene by one single separation operation, making it simple to operate and more energy efficient. Compared to the C2H4 molecule, the C2H6 molecule has a slightly larger polarizability and two additional hydrogen atoms. MOFs with OMSs usually interact strongly with C2H4 molecules via π complexation, whereas MOFs with relatively less polar sites, usually, can preferentially adsorb C2H6 over C2H4.46–66
In an earlier study, Gascon et al. firstly reported preferential capture of C2H6 over C2H4 by utilizing the gate-opening effect of ZIF-7 (also known as MAF-3).58 However, the separation efficiency was low due to the lack of active binding sites. In 2015, Zhang et al. reported a porous MAF [Zn(batz)] (MAF-49, H2batz = bis(5-amino-1H-1,2,4-triazol-3-yl)methane), which shows a high C2H6/C2H4 selectivity of 9 at 316 K.59 In MAF-49, there are quasi-discrete cages functionalized with a high density of electronegative nitrogen atoms on the surface, which are further interconnected by smaller paths into 1D channels (Fig. 3). DFT calculations and crystallographic study indicated that a C2H6 molecule confined in the cage can form stronger and more non-classical C–H⋯N hydrogen bonds or electrostatic interactions through better structural matching with the cage surface of MAF-49 as compared to the C2H4 molecule, which is beneficial for capture, or stronger binding of C2H6 compared with C2H4. MAF-49 showed, for the first time, an exceptional reversed selectivity compared with porous materials including MOFs, which conventionally bind more strongly with C2H4vs. C2H6. Breakthrough experiments for the C2H4/C2H6 (15:1) mixture showed that MAF-49 can give highly pure C2H4 (99.95%+) within a single breakthrough operation under ambient conditions.
Fig. 3 (a) Crystal structure of MAF-49. (b) Preferential adsorption sites for C2H6 in MAF-49 revealed by DFT calculations. (c) Gas adsorption isotherms for C2H6, C2H4, CO2 and CH4 in MAF-49 at 316K. (d) Breakthrough curves of the CH4/CO2/C2H4/C2H6 mixture (1:1:1:1 (vol)) for MAF-49 measured at 313K and 1bar. Reprinted with permission from ref. 59. Copyright 2018 Nature Publishing Group. |
An appropriate combination of pore sites and pore surface can maximize the weak host–guest interactions, thus highly enhancing the performance of MOFs for C2H6/C2H4 separation. In 2018, Chen et al. reported two isoreticular MOFs, [Cu(Qc)2] (HQc = quinoline-5-carboxylic acid) and [Cu(ina)2] (Hina = isonicotinic acid), featuring 1D channels with pore sizes of ∼4.1 and ∼3.3 Å, respectively, and an array of low-polarity aromatic surfaces with different contact areas on the channels (Fig. 4).60 Single-component sorption results demonstrated that [Cu(Qc)2] shows a higher C2H6 uptake than C2H4 (60.0 cm3 cm−3vs. 25.3 cm3 cm−3, i.e., 1.85 mmol g−1vs. 0.78 mmol g−1) at 298 K and 1 bar, thus giving a high C2H6/C2H4 selectivity of 3.4 for an equimolar C2H6/C2H4 mixture at 298 K and 1 bar. In contrast, [Cu(ina)2] shows comparable adsorption capacity for both gases (C2H4: 67.4 cm3 cm−3, and C2H6: 64.3 cm3 cm−3, i.e., 1.99 mmol g−1vs. 1.90 mmol g−1) due to the smaller polar surface. Neutron powder diffraction and DFT-D calculations showed that the high C2H6 selectivity in [Cu(Qc)2] can be attributed to the more C–H⋯π interactions formed between C2H6 and [Cu(Qc)2]. Breakthrough experiments demonstrated that high purity of C2H4 (> 99.9%) can be directly collected from a 50/50 C2H6/C2H4 mixture by a packed column bed of [Cu(Qc)2], with a separation productivity of 587 mmol L−1.
Fig. 4 (a) Neutron diffraction crystal structure of [Cu(Qc)2]·0.41C2D6. (b) Preferential binding sites for the C2D6 molecule and the close vdW contacts within the rhombic cavity of aromatic rings, highlighting C–H⋯π interactions in pink dashed bonds. (c) Experimental column breakthrough curves for an equimolar C2H6/C2H4 mixture (298 K, 1 bar) in an adsorber bed packed with Cu(Qc)2. Reprinted with permission from ref. 60. Copyright 2018 American Chemical Society. |
The incorporation of the peroxo sites into MOFs can improve the affinity for C2H6. In 2018, Chen et al. reported a microporous MOF [Fe2(O2)(dobdc)] (dobdc4− = 2,5-dioxido-1,4-benzenedicarboxylate) decorated with Fe–peroxo sites that exhibits a high C2H6 affinity with a large Qst of 66.8 kJ mol−1 (Fig. 5).61 Single-component sorption isotherms showed that [Fe2(O2)(dobdc)] can adsorb a large amount of C2H6 (74.3 cm3 g−1, 3.32 mmol g−1) at 1 bar and 298 K and the IAST selectivity for 50/50 C2H6/C2H4 was calculated to be 4.4 under the same conditions. High-resolution neutron powder diffraction showed that C2D6 molecules can form strong non-classical C–D⋯O hydrogen bonds with very short D⋯O distances (∼2.17 to 2.22 Å). Therefore, [Fe2(O2)(dobdc)] exhibits excellent separation performance, yielding polymer-grade C2H4 (≥99.99%) from 50/50 C2H4/C2H6 mixtures in a single breakthrough operation and a productivity of 0.79 mmol g−1. This result further confirms the unique and important role of non-classical C–H⋯O hydrogen bonds in the molecular recognition and selective adsorption of ethane by MOFs.
Fig. 5 Crystal structures of (a) pristine [Fe2(dobdc)] and [Fe2(O2)(dobdc)] (b) after oxidization and (c) after final C2D6-loading. (d) Sorption isotherms of [Fe2(O2)(dobdc)] for C2H6 and C2H4 under ambient conditions. (e) Breakthrough curves of [Fe2(O2)(dobdc)] for an equimolar C2H6/C2H4 mixture under ambient conditions. Reprinted with permission from ref. 61. Copyright 2018 the American Association for the Advancement of Science. |
To obtain materials with high C2H2 adsorption capacity and high selectivity, in 2016, Chen et al. reported a series of SIFSIX MOFs, namely, SIFSIX-1-Cu, SIFSIX-2-Cu, SIFSIX-2-Cu-i, SIFSIX-3-Ni, and SIFSIX-3-Zn, which allow preferential capture of C2H2 from the C2H2/C2H4 mixture with high selectivity and adsorption capacity.70 These materials possess different pore sizes, which can be systematically fine-tuned by replacing ligands, metal nodes, inorganic anions or framework interpenetration. Among them, SIFSIX-2-Cu-i with a two-fold interpenetrated framework and pore size of 5.2 × 5.2 Å2 (BET surface area 503 m2 g−1) exhibits a high uptake for C2H2 (2.1 mmol g −1, i.e., 47 cm3 g−1) at a low pressure of 0.025 bar, indicating its strong binding affinity for C2H2 (Fig. 6). The IAST selectivity of SIFSIX-2-Cu-i for C2H2/C2H4 (1/99) is up to 44.54. SIFIX-2-Cu with a pore size of 8.0 × 8.0 Å2 (BET surface area: 1178 m2 g−1) shows the highest C2H2 uptake of 8.5 mmol g−1 and a moderate IAST selectivity for C2H2/C2H4 (1/99) of 10.6. Breakthrough experiments demonstrated that all these SIFSIX MOFs can produce polymer-grade C2H4 from C2H2/C2H4 (1/99 or 50/50 mixtures). DFT-D calculations and high-resolution neutron powder diffraction studies reveled that SiF62− pillars in the framework can form strong hydrogen-bonding interactions with C2H2, resulting in the high selectivity and adsorption capacity for C2H2. This work revealed that the combination of optimal pore size and multiple active sites can greatly improve the selectivity and adsorption capacity of the MOFs.
Fig. 6 (a) Crystal structure of SIFSIX-1-Cu·C2H2. (b) DFT-D simulated structure of C2H2-loaded SIFSIX-2-Cu-i. (c) Single-component sorption isotherms of SIFSIX-1-Cu, SIFSIX-2-Cu, SIFSIX-2-Cu-i, SIFSIX-3-Zn, and SIFSIX-3-Ni for C2H2 and C2H4 under ambient conditions. (d) Breakthrough curves of SIFSIX-1-Cu, SIFSIX-2-Cu, and SIFSIX-3-Zn for a 1/99 C2H2/C2H4 mixture. Reprinted with permission from ref. 70. Copyright 2016 the American Association for the Advancement of Science. |
In 2017, Chen et al. reported a 2-fold interpenetrated MOF SIFSIX-14-Cu-i (UTSA-200) with a smaller pore size (3.4 Å) than SIFSIX-2-Cu-i (4.4 Å) and also functional as SiF62− sites that can enhance the binding affinity for C2H2 (Fig. 7).71 The pore size of the activated structure (UTSA-200a) ideally falls between the kinetic diameter of C2H4 (4.2 Å) and C2H2 (3.3 Å), endowing UTSA-200a with a high performance of molecular sieving separation of C2H2/C2H4. Single component equilibrium adsorption isotherms showed that UTSA-200a exhibits a high low-pressure uptake (58 cm3 cm−3) for C2H2 at 0.01 bar but a negligible uptake (∼0.25 mmol g−1) for C2H4 below 0.2 bar, which is significantly lower than the absorption of SIFSIX-2-Cu-i (2.28 mmol g−1). The IAST selectivity for a 1/99 C2H2/C2H4 mixture of UTSA-200a was calculated to be 6000 at 298 K and 1 bar. High-resolution neutron powder diffraction further revealed that the strong binding affinity of UTSA-200a for the C2D2 molecule was achieved by short C–D⋯F hydrogen-bonding interactions (1.921 Å). Breakthrough experiments revealed that UTSA-200a can efficiently separate C2H2 from a 1/99 C2H2/C2H4 mixture to give an extremely high purity C2H4 (99.9999%) with a productivity of 87.5 mmol g−1.
Fig. 7 (a) Crystal structure of UTSA-200. (b) C2H2 and C2H4 adsorption isotherms of UTSA-200a at 298 K. Adapted from ref. 71 with permission from Wiley-VCH, Copyright 2018. |
In 2017, Chen et al. reported an ultramicroporous SIFSIX-MOF [Zn(dps)2(SiF6)] (UTSA-300, dps = 4,4′-dipyridylsulfide) with small apertures (2.4 × 3.3 Å2) for specific recognition of C2H2 from C2H4.72 The desolvated structure UTSA-300a (aperture size: 3.3 Å) exhibits large affinity toward C2H2 with a Qst of up to 57.6 kJ mol−1 and thus can be selectively gate opened by C2H2. It should be noted that UTSA-300 shows complete size exclusion of C2H4, giving IAST selectivity for the equimolar C2H2/C2H4 mixture up to >104 at 298 K. Breakthrough experiments confirmed its good separation performance for an equimolar C2H2/C2H4 mixture. Subsequently, an isostructural framework of UTSA-300 [Cu(dps)2(SiF6)] (NCU-100 or UTSA-300-Cu) was reported.76 In contrast to UTSA-300, NCU-100 possesses elongated Cu(II)–F bonds, showing a larger cavity size (3.6 × 4.3 × 4.2 Å3vs. 3.5 × 3.9 × 4.1 Å3) in the closed-pore phase. Single-component sorption experiments revealed that NCU-100a shows not only higher low-pressure uptake (0.73 mmol g−1vs. 0.04 mmol g−1) for C2H2 at 0.01 bar and 298 K but also a higher total uptake capacity (4.57 mmol g−1vs. 3.08 mmol g−1) at 298 K and 1 bar, resulting in an IAST selectivity for 1/99 C2H2/C2H4 up to 7291 (298 K and 1 bar). This excellent performance for C2H2/C2H4 separation can also be attributed to the combination of optimal pore size and strong binding sites, as confirmed by DFT calculations and crystallographic studies. Breakthrough experiments confirmed that high purity C2H4 (>99.99%) can be obtained from a 1/99 C2H2/C2H4 mixture with a productivity of 14.9 mmol g−1.
Recently, Zhai et al. synthesized a series of cluster-based MOFs, [M9(μ4-TAZ)6(μ3-HTAZ)x(μ3-TAZ)12−x(A)y] solvent (SNNU-98-M, M = Mn, Co, Ni, and Zn), for the purification of C2H2, in which the tetrazolate (TAZ) ligands coordinate with metal centers in tridentate (μ3-TAZ) and tetradentate (μ4-TAZ) bridging modes.78 These MOFs of acs topology show high framework densities and high stabilities, as well as small pore sizes of 5.2 Å (Mn), 4.8 Å (Co), 4.8 Å (Ni), and 4.2 Å (Zn), respectively, which are expected to increase the separation selectivity and volumetric storage capacity. Single-component gas adsorption revealed that SNNU-98-Mn exhibits the highest volumetric C2H2 uptake (222.9 cm3 cm−3) at 298 K and 1 bar, and a high uptake for C2H2 (175.3 cm3 cm−3) at 298 K and 0.1 bar, whereas SNNU-98-Co shows the highest C2H2/C2H4 IAST selectivity (2405.7) under room temperature and 1 bar. Column breakthrough experiments revealed that all these materials show good C2H2/C2H4 separation performance, with SNNU-98-Mn displaying a higher C2H4 productivity of 64.6 mmol g−1 from a 1/99 C2H2/C2H4 mixture and a longer breakthrough retention time (1362 min g−1 and 701 min g−1 at 273 K and 298 K, respectively, with a gas flow rate of 2 mL min−1).
The separation of C2H4 from multicomponent mixtures in one step is significant for obtaining polymer-grade C2H4 due to the presence of multiple impurities in the cracking gas. Recently, more MOFs have been revealed to be capable of such multicomponent separation.79–94 In 2018, Lu et al. reported the highly selective adsorption of C2H4 from a C2H2/C2H4/C2H6 mixture by a stable MOF, (Me2NH2)[Co3(DCPN)2(μ3-OH)(H2O)]·11H2O (TJT-100, DCPN = 5-(3′,5′-dicarboxylphenyl)nicotinate).79 TJT-100 exhibits a 1D channel (pore size: ∼8.0 Å) decorated with a high density of carboxylate oxygen atoms. Single-component adsorption showed that the adsorption capacities of TJT-100 for C2H2, C2H4, and C2H6 were 127.7 cm3 g−1, 98.1 cm3 g−1, and 105.4 cm3 g−1, respectively. The breakthrough experimental results of TJT-100 for the C2H2/C2H4/C2H6 mixture (0.5:99:0.5) confirmed the preferential capture of C2H2 and C2H6, giving C2H4 with an excellent purity of 99.997%. DFT calculations revealed that C2H2 and C2H6 have multiple electrostatic interactions with the framework, which facilitates preferential adsorption of C2H2 and C2H6 by TJT-100.
In 2019, Zaworotko et al. reported a synergistic sorbent separation technique (SSST), which enables the one-step production of polymer-grade C2H4 from a ternary (C2H2/C2H6/C2H4) gas mixture, and even a quaternary (CO2/C2H2/C2H6/C2H4) gas mixture (Fig. 8).80 Three microporous MOFs, TIFSIX-2-Cu-I, SIFSIX-3-Ni, and Zn-atz-ipa, were placed in tandem on the sorbent bed, offering selective adsorption of C2H2, CO2, and C2H6, respectively. Notably, Zn-atz-ipa shows a rare, higher uptake of C2H6 than CO2, C2H2 and C2H4 at 0 to 0.4 bar. Breakthrough experiments showed that the packing order of the three MOFs in the sorbent bed has a significant impact on the separation performance, whereas the particle size and amount of the adsorbent have a minor effect. When the packing order is SIFSIX-3-Ni@Znatz-ipa@TIFSIX-2-Cu-i, high purity C2H4 can be gained from a 1/49.5/49.5 C2H2/C2H4/C2H6 or 1/33/33/33 C2H2/C2H4/C2H6/CO2 mixture and the working capacities are 0.32 and 0.10 mmol g−1, respectively. This work provides a new path for selective separation of a specific component molecule from a multicomponent gas mixture.
Fig. 8 (a) SSST involves an adsorption bed with three task-specific physisorbents to purify the commodity (red) with specific binding sites for each trace impurity (blue, green, and yellow). (b) and (c) Experimental column breakthrough curves for C2H2/C2H4/C2H6 separation (1:1:1 mixture) on TIFSIX-2-Cu-i and Zn-atz-ipa at 298 K and 1 bar. Breakthrough experiments were conducted in a column (inner diameter, 8 mm) at a flow rate of 2.1 ml min−1. (d) Experimental column breakthrough curves for C2H2/C2H4/C2H6 separation (1:1:1 mixture) on a tandem-packed column of TIFSIX-2-Cu-i (∼250 mg) and Zn-atz-ipa (∼600 mg) at 298 K and 1 bar. Reprinted with permission from ref. 80. Copyright 2019 the American Association for the Advancement of Science. |
In the early studies, Kitagawa et al. reported that a microporous MOF material, Cu2(pzdc)2(pyz), with non-coordinated oxygen atoms on the pore surface forms strong hydrogen-bonding interactions with C2H2, showing high C2H2/CO2 separation potential.99 This study firstly demonstrates the effective role of Lewis base sites in enhancing the affinity of a MOF for C2H2. In addition, MOFs with high density of OMSs can facilitate the recognition of acetylene.100–108 In 2016, Chen et al. reported a MOF-74 isomer, namely, UTSA-74, which has two different (octahedral and tetrahedral) metal coordination geometries along the 1D channel.101 Each octahedrally coordinated metal ion provides two OMSs upon removal of the coordinated water molecules, leading to enhanced C2H2/CO2 separation. The single-component adsorption isotherms showed that UTSA-74 has a comparable C2H2 uptake capacity (145 cm3 cm−3) to Zn-MOF-74 but a smaller CO2 uptake capacity (90 cm3 cm−3vs. 146 cm3 cm−3), resulting in UTSA-74 with a good C2H2/CO2 separation performance. This result can be attributed to that each open Zn site can bind with two C2H2 molecules, whereas two oxygen atoms of a CO2 molecule occupy two adjacent OMSs, as demonstrated by the single-crystal X-ray structures and molecular modeling studies. Breakthrough experiments for a 50/50 C2H2/CO2 mixture further demonstrate its good practical separation performance. This is also the first example of using breakthrough experiments to demonstrate the separation performance of MOFs for the C2H2/CO2 mixture.
Based on copper(I)-alkynyl chemistry, anchoring Cu(I) on the surface of a MOF can significantly improve its specific recognition for C2H2. Qian et al. reported a Cu(I)-modified porous MOF, Cu(I)@UiO-66-(COOH)2, which exhibits significantly enhanced C2H2/CO2 separation performance with a high C2H2/CO2 IAST selectivity of 185, compared to the prototype UiO-66-(COOH)2.107 The strong π-complexation between the π electrons on C2H2 and Cu ions enables Cu(I)@UiO-66-(COOH)2 to adsorb a large amount of C2H2 (0.9 mmol g−1) at low pressure (0.01 bar) and exhibit a high Qst of 74.5 kJ mol−1. Breakthrough experiments demonstrated its highly efficient separation performance for C2H2/CO2. In addition, optimal distribution of OMSs on the pore surface of MOFs can achieve the maximum utilization of these sites. Recently, Li et al. reported a microporous MOF (JNU-4) with high-density OMSs.108 These sites consist of square-planar copper centers separated by organic ligands, allowing each metal center to effectively bind with C2H2; thus, JNU-4 achieves a high C2H2 adsorption capacity (222 cm3 g−1, 9.91 mmol g−1) and a moderate IAST selectivity of 8.2 for an equimolar C2H2/CO2 mixture. Notably, this material absorbs C2H2 up to 200 cm3 g−1 (8.93 mmol g−1) at 298 K and 0.5 bar, but demonstrates a low Qst of 26.8 kJ mol−1. Grand Canonical Monte Carlo (GCMC) simulations demonstrated that C2H2 molecules can bind on both sides of OMSs, while CO2 molecules can only bind on one side. Breakthrough experiments revealed that it has a high C2H2 absorption capacity (160 cm3 g−1, 7.14 mmol g−1) from an equimolar C2H2/CO2 mixture and can provide fuel-grade C2H2 gas.
Although a high density of OMSs can improve the selectivity for C2H2, electrostatic interactions between CO2 and metal also exist simultaneously.109–111 This requires a rational distribution of metal sites or the combination of multiple functions such as the pore size and shape to achieve a better C2H2 selectivity.100,105,112 However, OMSs of high density may result in a high Qst, thus leading to an increase of the energy consumption for adsorbent regeneration. In addition to OMSs, the introduction of functional groups (–NH2, –F, –Cl, –Br, –CF3, etc.) on organic ligands is also an effective strategy to promote selective adsorption of C2H2.113–116 In 2021, Zhao et al. reported that an amine-functionalized flexible MOF (CPL-1-NH2) with a 1D channel (3.8 × 4.4 Å2) exhibits a high IAST selectivity of 119 for a 50/50 C2H2/CO2 mixture at 298 K and 1 bar.114 Theoretical calculations showed that the high selectivity of CPL-1-NH2 for C2H2 can be attributed to the NH2 functionalization that enhances C2H2 interaction with the framework, but blocks the stronger interaction between the non-coordinated oxygen atoms and CO2 molecules by occupying the adsorption site of CO2. In the same year, Qian et al. reported an Al-MOF (CAU-10-H) with a pore size of 4.7 Å, exhibiting a high C2H2 storage density (392 g L−1) and a separation factor (3.4).115 GCMC simulations showed that the suitable pore size not only enhances the interaction of C2H2 with high density oxygen atoms and aromatic rings on the pore surface, but also enables synergistic interaction between adjacent C2H2 molecules. Subsequently, CAU-10-H was functionalized with amine to furnish a new MOF (CAU-10-NH2).116 The later study showed that the amine groups can improve the uptake capacity of C2H2 at low pressure, and significantly enhance the stacking density (0.46 cm3 g−1) and C2H2/CO2 selectivity (10.8) compared with the prototype MOF. In addition, these materials have the advantages of high stability, low Qst, easy scale-up, and low cost.
It is well known that pore size and shape play an important role in the separation process, as an appropriate pore size can enhance the strength of interactions between the pore surface and adsorbate, as well as among adsorbates themselves.97,100,112,117–123 MOFs can be designed and modified to alter the pore sizes, even at the sub-nanometer scale, through substitutions of metal ions, organic ligands, or inorganic anions. Strategies such as building self-interpenetrated networks and pore space partition (PSP) can also be used for the pore size or space modulation.13,124 In 2019, Chen et al. reported a PSP approach for highly efficient C2H2/CO2 separation. The new porous MOF (FJU-90) was synthesized by inserting a triangular ligand (2,4,6-tris(4-pyridyl)pyridine) into the cylindrical channel of prototype FJU-88.122 The 1D channel of FJU-88 was separated into a number of aperture cavities with the aperture size decreasing from 12.0 × 9.4 to 5.4 × 5.1 Å2. Thus, the combination of optimized pore space and oxygen atom sites endows FJU-90a with a high C2H2 adsorption capacity (180 cm3 g−1, 8.04 mmol g−1). The separation performance of the activated MOF (FJU-90a) for a 50/50 C2H2/CO2 mixture was further confirmed by breakthrough experiments with a productivity of 1.87 mol kg−1.
In 2017, Chen et al. reported a SIFSIX-MOF UTSA-300 that exhibits not only efficient separation of C2H2/C2H4 but also a high selective uptake for C2H2 from the C2H2/CO2 mixture.72 Single-component adsorption isotherms revealed that the activated MOF (UTSA-300a) shows a high capacity for C2H2 adsorption (68.9 cm3 g−1, 3.08 mmol g−1) but adsorbs negligible CO2 (3.25 cm3 g−1, 0.14 mmol g−1) at 298 K and 1 bar, resulting in a high IAST C2H2/CO2 selectivity of 743 (298 K and 1 bar) (Fig. 9). Due to the strong C–H⋯F interactions formed between C2H2 molecules and SIF62−, C2H2 can easily diffuse into UTSA-300a, while CO2 is restricted because of electrostatic repulsion, as confirmed by DFT calculations and neutron powder diffraction studies. The separation performance of UTSA-300a for a 50/50 C2H2/CO2 mixture was further demonstrated by breakthrough experiment in a packed column bed of UTSA-300a. Subsequently, systematic fine-tuning of the pore size of UTSA-300 was performed by replacing the fluoride anionic linkers and metal ions.125 Three new SIFSIX-type MOFs, namely SIFSIX-dps-Cu (NCU-100), GeFSIX-dps-Cu, and NbOFFIVE-dps-Cu, were reported to exhibit different pore sizes (1.4 × 3.0 Å2, 1.5 × 3.0 Å2, and 2.2 × 2.7 Å2, respectively) and interlayer distances (4.10 Å, 4.06 Å, and 3.69 Å, respectively). Single-component adsorption isotherms indicated that SIFSIX-dps-Cu shows the highest C2H2 uptake (4.57 mmol g−1) with a high IAST C2H2/CO2 selectivity up to 1787 at 298 K and 1 bar. In addition, the gate-opening pressure of SIFSIX-dps-Cu for C2H2 is 0.035 bar, which is lower than those of GeFSIX-dps-Cu (0.05 bar), NbOFFIVE-dps-Cu (0.3 bar), and UTSA-300 (0.06 bar), probably because of its larger interlayer distance. DFT and grand canonical Monte Carlo simulations further revealed that C2H2 molecules have multiple host–guest interactions (H⋯F hydrogen-bonding interactions) in both inter- and intra-layer cavities. Breakthrough experiments confirmed that high purity C2H2 (≥99.9%) can be obtained from C2H2/CO2 (50/50) with a high productivity of 2.48 mmol g−1.
Fig. 9 (a) and (c) Neutron diffraction crystal structure of UTSA-300⊃C2D2 and (b) C2H2, CO2, and C2H4 sorption isotherms for UTSA-300a at 273 K. (d) Experimental column breakthrough curves for equimolar C2H2/CO2 (purple) and C2H2/C2H4 (orange) mixtures (298 K, 1 bar) in a fixed-bed packed with UTSA-300a. Reprinted with permission from ref. 72. Copyright 2017 American Chemical Society. |
A suitable pore size combined with active sites and a flexible structure can greatly improve the adsorption capacity of a material for C2H2.95,106,114,125–127 Recently, Hong et al. reported that a flexible MOF, namely, [Ni(DTBDA)(MeOH)2(DMA)(H2O)2] (FJI-H36, DTBDA = 3′,5′-di(1H-1,2,4-triazol-1-yl)-[1,1′-biphenyl]-3,5-dicarboxylic acid), with adaptive channels shows efficient adsorption of C2H2.127 FJI-H36 contains two types of cavities with the size of 12.9 × 12.9 Å2 and 8.4 × 10.2 Å2, respectively, as well as high-density active sites of open NiII (4.52 mol L−1) and free N atoms (9.04 mol L−1). Single-component sorption experiments confirmed that FJI-H36 shows a high C2H2 uptake of 159.9 cm3cm−3 at 298 K and 1 bar, and an ultra-high C2H2 storage density of 561 g L−1. Breakthrough experiments for a 50/50 C2H2/CO2 mixture further demonstrated its high adsorption capacity for C2H2 (3.82 mmol g−1). The structure of FJI-H36 adaptively changes with the adsorption of C2H2, leading to a dense packing of C2H2 in it, as demonstrated by the X-ray crystal structure of C2H2@FJI-H36.
Recently, Wang et al. reported a sulfate-pillared MOF [Zn(tepb)(SO4)] (SOFOUR-TEPE-Zn, TEPB = tetra(4-pyridyl)benzene), which possesses dense electronegative pore surfaces to highly promote the separation of C2H2/CO2 (Fig. 10).97 SOFOUR-TEPE-Zn is an isostructural framework with SOFOUR-1-Zn,128 but with more electron-rich pore surfaces due to the higher electronegative ethylene groups in the TEPE ligand in contrast to the phenyl ring in the TEPB ligand. Single-component sorption results of SOFOUR-TEPE-Zn reveled a higher C2H2 uptake (89.1 cm3 g−1, 3.98 mmol g−1) than SOFOUR-1-Zn (69.4 cm3 g−1, 3.10 mmol g−1) at 1 bar and 298 K, but a much lower CO2 uptake (14.1 cm3 g−1, 0.63 mmol g−1), resulting in a very high IAST selectivity of 16833 for 50/50 C2H2/CO2. Breakthrough experiments for 50/50 C2H2/CO2 of SOFOUR-TEPE-Zn give a productivity of 60.1 cm3 g−1 (2.68 mmol g−1) of 99.5% purity or 33.2 cm3 g−1 (1.48 mmol g−1) of 99.99% purity in its desorption process by stepped helium purging and mild heating. Moreover, SOFOUR-TEPE-Zn also maintains a high C2H2 productivity of 75.5 cm3 g−1 (3.37 mmol g−1) of 99.5% purity with 99.82% C2H2 recovery in the simulated pressure swing adsorption processes. DFT-D and GCMC simulation studies revealed that the preferential binding of C2H2 in SOFOUR-TEPE-Zn can be mainly attributed to electron-rich pore surfaces, providing multiple optimal adsorption sites for C2H2.
Fig. 10 (a) and (b) The building blocks of SOFOUR-TEPE-Zn and electrostatic surface potential. (c) C2H2 and CO2 adsorption isotherms for SOFOUR-1-Zn and SOFOUR-TEPE-Zn at 298 K. (d) Breakthrough curves of SOFOUR-TEPE-Zn for C2H2/CO2 (50/50, v/v) at different flow rates at 298 K. Reprinted with permission from ref. 97. Copyright 2023 Wiley-VCH. |
CO2-selective adsorbents can yield high purity C2H2 in one step rather than multiple adsorption–desorption steps, making the operation simple and more energy efficient. Currently, only a limited number of CO2-selective MOF materials have been reported, manifesting the challenge in the design of CO2-selective materials.129–148 Fortunately, several strategies have been reported to promote the selective adsorption of CO2 in MOFs. For example, Chen et al. introduced hydroxyl functional groups into MOF frameworks, enabling selective capture of CO2 from C2H2, with a high IAST selectivity of 118.7 for CO2/C2H2 (1:2, v:v) at 0.1 bar and ambient temperature.137 In 2021, Chen et al. reported an ultramicroporous MOF [Cu(F-pymo)2]·1.25H2O (Cu-F-pymo, F-pymo = 5-fluoropyrimidin-2-olate) with zeolitic gismondine (GIS) topology exhibiting a high selective adsorption of CO2 over C2H2, which depends on activation temperature (Fig. 11).143 Cu-F-pymo contains two distinct pore environments, namely, spherical cavities and 1D helical channels, both of which are occupied by removable water molecules. Single-component adsorption isotherms revealed that partially dehydrated Cu-F-pymo can adsorb 1.19 mmol g−1 C3H6 and show negligible C2H2 uptake (0.1 mmol g−1) at 298 K and 1 bar. Breakthrough experiments revealed that highly pure acetylene (>99.9%) can be obtained directly from a 50/50 CO2/C2H2 mixture by a single separation operation. Modeling studies demonstrated that CO2 can be preferentially adsorbed in the 1D channels, while C2H2 primarily occupies the spherical cavities. Therefore, the remaining water molecules in the spherical cavities blocked the preferential site, leading to the molecular sieving effect of Cu-F-pymo for CO2/C2H2.
Fig. 11 (a) Schematic structure of Cu-F-pymo MOF with residual water molecules. (b) Breakthrough cycling tests of the equimolar CO2/C2H2 mixture. (c) and (d) Separation performance toward CO2 and C2H2 in Cu-F-pymo under different activation conditions. Reprinted with permission from ref. 143 Copyright 2021 Wiley-VCH. |
Besides size-matching between gas molecules and the pore structure, reasonable charge distribution would also facilitate the selective recognition of CO2 over C2H2. Chen et al. reported an ultramicroporous porous material Cd[Fe(CN)5NO] (Cd-NP) that exhibits stronger affinity for CO2 in contrast to C2H2. Cd-NP contains quasi-discrete ellipsoidal cavities (6.1 × 4.5 × 4.5 Å3) connected by small apertures (3.2 Å), and its BET surface area is 305 m2 g−1 (Fig. 12).144 Thanks to suitable pore sizes and electrostatic distribution on pore surfaces, Cd-NP shows a high CO2 uptake of 58.0 cm3 g−1 (2.59 mmol g−1) but a lower C2H2 uptake of 9.7 cm3 g−1 (0.43 mmol g−1) at 1 bar and 298 K, thus showing a high IAST selectivity (85) for an equimolar CO2/C2H2 mixture. The Qst of CO2 was calculated to be 27.7 kJ mol−1, which would facilitate regeneration of the material under mild conditions. The breakthrough process showed that Cd-NP was capable of producing a high purity C2H2 (99.9%) directly from 50/50 CO2/C2H2 with a productivity of 2.34 mol L−1. GCMC simulations and neutron powder diffraction experiments showed that the preferential adsorption of CO2 in Cd-NP can be attributed to the confinement effect of the pore cavity and electrostatically complementary pore surface.
Fig. 12 (a) Electrostatic potential (ESP) of Cd-NP⊃CO2 mapped onto the 0.15 e−Å−3 electron density isosurface. (b) Electrostatically driven adsorption mechanism towards CO2 and C2H2 molecules. (c) CO2 and C2H2 sorption isotherms for Cd-NP at 298 K. (d) Cycling tests of the equimolar CO2/C2H2 mixture in a column packed with Cd-NP at 298 K and 1 bar. Reproduced with permission from ref. 144. Copyright 2021 Wiley-VCH. |
CO2/C2H2 inverse separation can also be achieved using synergistic effects of thermodynamics and kinetics. Li et al. reported an ultramicroporous MOF, Y-bptc, to achieve one-step C2H2 purification from a CO2/C2H2 mixture. Y-bptc processes small windows (4.2 Å) interconnected with large cubic cages with ftw topology. Equilibrium and kinetic adsorption studies reveled that Y-bptc absorbs 55 cm3 g−1 (2.45 mmol g−1) CO2 and a lower C2H2 uptake at 298 K and 1 bar with an IAST selectivity of 4.1 for 50/50 CO2/C2H2.136 Moreover, CO2 diffuses faster than C2H2 in Y-bptc, and the calculated kinetic separation coefficient reaches 114 at 298 K. Breakthrough experiments confirmed that CO2 in a 1:1 CO2/C2H2 mixture can be readily removed by Y-bptc, giving C2H2 with a purity of >99% and productivity of 1.52 mmol g−1 in a one-step separation process. GCMC simulations further revealed the high affinity of Y-bptc for CO2 resulting from the formation of hydrogen-bonding interactions between μ3-OH− groups of the framework and CO2 molecules.
In 2023, Wade et al. reported two isostructural MOFs [Zn5Cl4(bbta)3] (MUF-4, bbta2− = benzo-1,2,4,5-bistriazolate) and MUF-4-F, which exhibited completely opposite adsorption selectivity for CO2/C2H2. MUF-4-F can be derived by F− to Cl− ligand exchange of MUF-4.139 Both MUF-4-F and MFU-4 possess alternating large pore and small pore cavities but have different connecting windows (∼3.7 Å and ∼2.2 Å, respectively). C2H2 molecules can easily enter MFU-4-F. Equilibrium and kinetic adsorption studies revealed that MFU-4-F exhibits a higher C2H2 (6.66 mmol g−1) uptake than CO2 (3.24 mmolg−1) at 300 K and 1 bar and shows a fast adsorption rate for both gases. In contrast, MFU-4 exhibits high kinetic selectivity for uptake of CO2 over C2H2 up to 3360 at 300 K. Computational studies revealed that C2H2 was blocked by the smaller windows created by the Zn–Cl groups in MUF-4. Breakthrough experiments demonstrated that high purity (>98%) C2H2 can be obtained directly from a 50/50 CO2/C2H2 mixture in MUF-4.
The incorporation of active sites in MOFs’ pore surface improves not only kinetic selectivity but also thermodynamic selectivity for gas separation. In 2019, Zhang et al. reported a MAF, MAF-23-O, which can be easily synthesized by heating the flexible prototype [Zn2(btm)2] (MAF-23, H2btm = bis(5-methy-1H-1,2,4-triazol-3-yl)methane) under oxygen gas flow (Fig. 13).149 Single-crystal structure analyses showed that MAF-23-O is isostructural to MAF-23 and contains half the amount of the oxidized btm2− ligands, namely, btk2− (H2btk = bis(5-methyl-1,2,4-triazol-3-yl)methanone). This in situ ligand oxidative modification makes the framework more rigid and more hydrophilic. The IAST selectivity for C3H6/C3H8 in MAF-23-O was calculated to be 8-9, which was higher than that of MAF-23 (3-4). Moreover, C3H6 and C3H8 exhibit similar diffusion rates in MAF-23, but show very different diffusion rates in MAF-23-O with a high kinetic selectivity of 71. Theoretical calculations demonstrated that the exposed oxygen atoms in the framework of MAF-23-O can form strong C–H⋯O/N interaction with C3H6, improving the thermodynamic selectivity of MAF-23-O for C3H6. Additionally, the decreased flexibility of the framework slows down the diffusion of C3H6, thus improving the kinetic selectivity. Breakthrough experiments revealed that MAF-23-O exhibits efficient separation for an equimolar C3H6/C3H8 mixture at 298 K and 1 bar with an adsorption selectivity of 15, which is 10 times that of MAF-23.
Fig. 13 Crystal and pore structures of (a) MAF-23 and (b) MAF-23-O. Breakthrough curves (filled symbols) and adsorption kinetic curves (open symbols) for (c) MAF-23 and (d) MAF-23-O using an equimolar C3H6/C3H8 (blue/red) mixture at 298 K and 1 bar. Reprinted with permission from ref. 149. Copyright 2019 Wiley-VCH. |
In 2016, Eddaoudi et al. reported a oxyfluoride-based MOF [Ni(pyr)2(NbOF5)]·2H2O (NbOFFIVE-1-Ni, or KAUST-7, pyr = pyrazine) for selective adsorption of C3H6 from C3H8.150 KAUST-7 is isostructural to SIFSIX-3 and composed of Ni(II)-pyrazine square-grid layers and (NbOF5)2− pillars with pcu topology, exhibiting 1D channels with an aperture size of 3.0 Å and a periodic array of fluoride anions on the pore surface. Single-component sorption experiments revealed that KAUST-7 can adsorb ∼60 mg g−1 (1.43 mmol g−1) C3H6 but negligible C3H8 uptake at 298 K and 1 bar. Breakthrough experiments demonstrated that C3H8 of 97% purity can be obtained from C3H6/C3H8 50/50 mixed-gas by a packed column bed of KAUST-7, with a separation productivity of 0.6 mol g−1. KAUST-7 also can adsorb C3H8 by pore-opening sorption behavior at 273 K.
In 2023, Chen et al. reported another SIFSIX MOF [Ni(WO2F4)(pyz)2] (UTSA-400) featuring 1D channels that can exclude C3H8 molecules and adsorb C3H6 molecules with a high binding affinity (Fig. 14).151 UTSA-400 shows an isostructural framework with SIFSIX-3 and NbOFFIVE-1-Ni, but with highly tilted pyrazine linkers owing to larger WO2F42− in contrast to SiF62− and NbOF52−. The pore cavities in UTSA-400 are 6.7 × 5.5 × 3.7 Å3 with exposed oxide/fluoride pairs on the pore surface (BET surface area: 226 m2 g−1) that can serve as the binding sites for propylene molecules. Single-component sorption results of UTSA-400 indicated a much higher C3H6 capacity (92.1 cm3 cm−3, 2.62 mmol g−1) than NbOFFIVE-1-Ni (54.3 cm3 cm−3, 1.34 mmol g−1) by 63%, at 1 bar and 298 K, which is also higher than those of Y-abtc (64.6 cm3 cm−3, 1.98 mmol g−1) and Co-gallate (66.6 cm3 cm−3, 1.79 mmol g−1). Under the same conditions, UTSA-400 showed negligible C3H8 uptake because of inaccessible inward diffusion of propane molecules. The Qst of UTSA-400 for C3H6 is 60.5 kJ mol−1, being comparable to those of MOFs with OMSs (44–57 kJ mol−1).30,45 Breakthrough separation experiment demonstrated that polymer-grade (99.7%) propylene can be obtained from an equimolar C3H6/C3H8 mixture with a productivity of 56.7 L L−1. Besides size exclusion, the separation performance of UTSA-400 can also be attributed to strong C–H⋯O/F interactions, as confirmed by in situ infrared spectroscopy and DFT-D calculations.
Fig. 14 (a) Crystal structure of UTSA-400. (b) Connolly surface of UTSA-400 mapped with electrostatic potential with a probe of 1.2 Å. (c) Single-component adsorption isotherms of C3H6 and C3H8 for UTSA-400 and NbOFFIVE-1-Ni at 298 K. (d) Breakthrough curves for NbOFFIVE-1-Ni and UTSA-400 for an equimolar binary mixture of C3H6 (solid line)/C3H8 (dashed line) at 298 K and 1 bar. Reprinted with permission from ref. 151. Copyright 2023 American Chemical Society. |
In 2018, Li et al. studied four microporous MOFs, namely, Zr-bptc, Zr-abtc, Y-bptc, and Y-abtc, which were obtained by the combination of two analogous metal clusters (Zr6 and Y6 clusters) and two different ligands (abtc = 3,3′,5,5′-azobenzenetetracarboxylates, and bptc = 3,3′,5,5′-biphenyltetracarboxylates).152 Among these materials, Y-abtc has cage-like pores connected through small windows, exhibiting ftw topology and optimal pore size (4.72 Å) that enables it to adsorb small C3H6 molecules (4.48 Å) with fast kinetics but completely exclude larger C3H8 molecules (5.1 Å). Single-component sorption experiments revealed that Zr-bptc exhibits similar adsorption capacities for C3H6 and C3H8, whereas its isostructural Y-bptc excludes both gases, attributable to the presence of equilibrium cations (dimethylammonium) in the Y-bptc affecting its pore size. In contrast, Y-abtc with the optimal pore size shows a high adsorption capacity for C3H6 (∼2 mmol g−1) and a negligible C3H8 uptake at 298 K. Column breakthrough experiments indicated that polymer-grade C3H6 (99.5%) can be obtained from 5/95 C3H6/C3H8 mixtures by Y-abtc. Recently, the same group reported a new Y-based MOF, Y6(OH)8(eddi)3(DMA)2 (HIAM-301, H4eddi = 5,5′-(ethene-1,2-diyl)diisophthalic acid, and DMA = dimethylammonium), also exhibiting the molecular sieving separation of C3H6/C3H8 mixtures. HIAM-301 is composed of 12-connected Y6(OH)8(COO)12 clusters bridged by 4-connected eddi4− linkers to form a 3D framework with ftw topology and a pore size of 4.6 Å.153 It is isostructural to Y-abtc and possesses distorted cubic cages (size: 10 × 10 Å2), which provides better control over guest accessibility. Single-component adsorption isotherms revealed that HIAM-301 can adsorb 3.16 mmol g−1 C3H6 and exhibit minor C3H8 adsorption (<0.3 mmol g−1) at 298 K and 1 bar, resulting in a high IAST selectivity (>150) for equimolar C3H6/C3H8 under the same condition. The practical performance for separation of 5/95 C3H6/C3H8 was confirmed by dynamic breakthrough experiments with a high productivity of 46.4 cm3 g−1 (>99.5% purity).
In 2020, Chen et al. reported an ultramicroporous Co-gallate MOF [Co(C7O5H4)] (Co-gallate) with 3D channels, which exhibits efficient C3H6/C3H8 separation by molecular sieving effect.154 Co-gallate shows elliptical windows (size: 4.2 × 5.1 Å2), which are precisely between the sizes of C3H8 and C3H6 (Fig. 15). Single-component adsorption isotherms showed that Co-gallate has a high adsorption capacity of C3H6 (66.6 cm3 cm−3, 1.79 mmol g−1), whereas the adsorption of C3H8 (5.2 cm3 cm−3, 0.14 mmol g−1) is minor at 298 K. The IAST selectivity of Co-gallate for a 50/50 C3H6/C3H8 mixture was calculated up to 330 at 1 bar and 298 K. Fixed-bed breakthrough experiments further confirmed its molecular sieving separation performance for 50/50 C3H6/C3H8, with a C3H6 productivity of 36.4 cm3 cm−3, 0.98 mmol g−1 (97.7%+ purity).
Fig. 15 (a) Structure of the Co-gallate MOF and rationale for C3H6/C3H8 separation. (b) Gas sorption isotherms of propylene and propane at 298 K for Co-gallate. (c) The breakthrough experiments were carried out in a packed column. Reprinted with permission from ref. 154. Copyright 2020 American Chemical Society. |
In 2021, Li et al. reported a MOF (JNU-3a) featuring 1D channels (size ∼4.5 × 5.3 Å2) attached with small pockets arranged on both sides for C3H6/C3H8 separation, where 1D channels could facilitate fast adsorption–desorption kinetics (Fig. 16).155 In addition, the small pockets were connected with the 1D channel through small apertures (∼3.7 Å) that can undergo gate-opening for C3H6 and C3H8 at different partial pressures. JNU-3a exhibits a stepwise adsorption isotherm and shows temperature-dependent gate-opening for C3H6 and C3H8, where C3H8 exhibits a higher gate-opening pressure than C3H6. Therefore, the high selectivity of JNU-3a for C3H6/C3H8 can be obtained at optimal temperature (303 K). JNU-3a can adsorb 58.6 cm3 g−1 (2.62 mmol g−1) C3H6 at 303 K, and the C3H6 packing density inside JNU-3a was calculated to be 404 g L−1. The dynamic feature of pore aperture was further revealed by single-crystal X-ray diffraction and theoretical calculation studies. Breakthrough experiment revealed that high-purity C3H6 (≥99.5%) can be obtained from a 50/50 C3H6/C3H8 mixture by JNU-3a. After applying helium purge to those adsorbed gases, C3H6 was collected with a maximum productivity of 53.5 L kg−1. The unique pore structure reported in this work would inspire future design of novel MOFs for application in adsorptive separation.
Fig. 16 (a) Pore structure of JNU-3 viewed along the b axis showing the molecular pockets (turquoise) and 1D channels (yellow); (b) pure C3H8 (green), pure C3H6 (red), and an equimolar C3H6/C3H8 mixture (orange) adsorption/desorption isotherms of JNU-3a at 303 K; (c) C3H6 adsorption isotherms of JNU-3a at different temperatures; (d) breakthrough curves (starting at t = 0) of an equimolar C3H6/C3H8 mixture (1.0 mL min−1) on JNU-3a, followed by desorption curves (starting at t = t1) under helium gas (10.0 mL min−1) sweeping at 303 K. C3H8, open diamonds; C3H6, solid diamonds. C and C0 are the concentrations of each gas at the outlet and inlet, respectively. Grey area, mixed gas input; yellow area, C3H6 gas output; t1, the beginning of desorption; t2, starting point of collecting C3H6; t3, the end point of collecting C3H6. Reprinted with permission from ref. 155. Copyright 2021 Nature Publishing Group. |
In 2023, Bai et al. reported a supertetrahedral-cluster (Cu10O13)-based MOF (NTU-85) which possesses square-shaped 1D channels that host lattice water molecules.156 The partial lattice water molecules can be precisely removed to form a MOF (NTU-85-WNT) of pore surface decorated with water nanotubes (∼4.5 Å). Single-component sorption results of NTU-85-WNT indicated a rapid C3H6 uptake (20.9 mL mL−1, 0.45 mmol g−1), while the adsorption of C3H8 (0.13 mL mL−1, 0.003 mmol g−1) at 298 K can be neglected. The IAST selectivity of NTU-85-WNT for an equimolar C3H6/C3H8 mixture reaches up to 1570. Fixed-bed breakthrough experiments further confirmed its molecular sieving performance for an equimolar C3H6/C3H8 mixture, with a C3H6 productivity of 1.6 mL mL−1 (98.8%+ purity). It is worth noting that high purity C3H8 (>99.5%) can be obtained in one adsorption–desorption cycle due to the efficient sieving performance.
An optimal pore size combined with high-density binding sites can efficiently separate C3H6/C3H8, allowing for high-density stacking of C3H8 and maximizing its adsorption capacity. Recently, Chen et al. reported a robust Hofmann-type MOF, [Co(pyz-NH2)Ni(CN)4] (ZJU-75a, pyz-NH2 = 2-aminopyrazine), with high-density binding sites, showing excellent separation performance for C3H6/C3H8.157 ZJU-75a exhibits an isostructural framework with [Co(pyz)Ni(CN)4] (ZJU-74a, pyz = pyrazine), decorated with amino groups. ZJU-75a exhibits an appropriate pore size (4.1 × 4.4 Å2) and OMSs of high density (8.89 mmol cm−3). Single-component sorption isotherms showed that ZJU-75a and ZJU-74a exhibit comparable C3H6 uptakes of 104.3 cm−3 cm3 (3.31 mmol g−1) and 111.4 cm−3 cm3 (3.68 mmol g−1) at 1 bar and 296 K, respectively, whereas the C3H8 adsorption capacity of ZJU-75a (73.5 cm−3 cm3, 2.33 mmol g−1) is obviously smaller than that of ZJU-74a (103.6 cm−3 cm3, 3.42 mmol g−1). Thus, the IAST selectivity of ZJU-75a for C3H6/C3H8 was calculated to be 54.2 at 296 K and 1 bar, much higher than that of ZJU-74a (4.3). The breakthrough studies indicate that ZJU-75a can yield C3H6 of high-purity (99.5%+) with a productivity of 18.7 L kg−1 and separation factor of 14.7. Structural and computational studies indicated that high-density OMSs and nitrogen atoms (from [Ni(CN)4]2 units and -NH2 groups) in ZJU-75a contribute jointly to the strong adsorption of C3H6, thus resulting in a high C3H6 storage density (0.818 g mL−1).
C3H8-selective adsorptive separation would be a relatively simple and energy-efficient way to get pure propylene. However, the differences of the molecular size (∼0.5 Å) and polarizability (C3H6: 62.6 × 10−25, and C3H8: 62.9–63.7 × 10−25 cm3) between C3H6 and C3H8 are smaller than those between C2H4 and C2H6. So far, only a few C3H8-selective MOFs have been reported.169–180
In 2022, Xing et al. reported an ultramicroporous pillared layered MOF [Co(IPA)(DPG)]n (PCP-IPA, IPA = isophthalic acid, and DPG = meso-α,β-di(4-pyridyl)glycol) featuring 1D pores (size ∼4.7 × 5.6 Å2) and periodic parallel-aligned isophthalic acid units on the pore surface, exhibiting an excellent selectivity for C2H6 and C3H8.169 Although C2H6 and C3H8 have different molecular sizes, the suitable pore size of PCP-IPA facilitates their directional adsorption and maximizes the interaction between PCP-IPA and C3H8/C2H6. Therefore, PCP-IPA exhibits not only a C3H8/C3H6 (50/50) IAST selectivity of 2.48 but also a relatively high adsorption selectivity (2.80) for C2H6/C2H4 (50/50) at 1.0 bar and 298 K. Both C3H8 and C2H4 can be directly obtained with high purity (99.99%) through a fixed-bed column from C3H8/C3H6 (50/50) and C2H4/C2H6 (50/50) mixtures, respectively, affording a high C3H6 productivity (15.23 L kg−1) and excellent C2H4 productivity (26.2 L kg−1). Modeling simulation studies revealed that tighter and more multiple vdW interactions (C–H⋯O/C) can be formed between paraffins and PCP-IPA compared to olefins.
Very recently, Li et al. reported two isostructural MOFs (FDMOF-1 and FDMOF-2) functionalized with different amounts of fluorinated functional groups (–CF3), showing strong affinity for C3H8 over C3H6 (Fig. 17).170 Compared with the protype MOF Zn2(BDC)2(DABCO) (Zn-DMOF, BDC = 1,4-benzenedicarboxylate), the introduction of different amounts of –CF3 groups into a MOF not only increases its stability but also adjusts the pore size/shape. Therefore, FDMOF-2 with the maximal amount of –CF3 groups shows the smallest aperture (5.1 Å) and exhibits the optimal C3H8 affinity. Single-component sorption isotherms showed that FDMOF-2 displays a higher C3H8 uptake of 140 cm3 cm−3 (5.04 mmol g−1) but a lower C3H6 uptake of 115 cm3 cm−3 (4.14 mmol g−1), resulting in the IAST selectivity for 50/50 C3H8/C3H6 up to 2.18 at 298 K and 1 bar. Breakthrough experiments revealed that high purity (>99.99%) C3H6 can be directly produced from 50/50 C3H8/C3H6 mixtures, affording 0.501 mol L−1 production of C3H6. It is worth pointing out that the excellent separation performance of FDMOF-2 for C3H8/C3H6 can be maintained under 70% relative humidity conditions. Single-crystal X-ray diffraction and theoretical calculation studies confirmed that the strong affinity of UTSA-400 for C3H8 can be attributed to strong non-classical C–H⋯π/F hydrogen-bonding interactions, resulting in a stronger binding affinity for C3H8vs. C3H6 with an initial Qst value difference of −3.7 kJ mol−1.
Fig. 17 (a) Crystal structures of Zn-DMOF, FDMOF-1, and FDMOF-2. (b) Single-component gas adsorption isotherms of the samples at 298 K. Reprinted with permission from ref. 170. Copyright 2023 Wiley-VCH. |
In 2017, Chen et al. reported a flexible-robust MOF [Cu(bpy)2(OTf)2] (ELM-12, bpy = 4,4′-bipyridine, and OTf− = trifluoromethanesulfonate) which exhibits excellent performance for removing trace C3H4 from a 1/99 C3H4/C3H6 mixture. ELM-12 composed of 2D square-grid sheets with dynamic dangling OTf− groups exhibit two kinds of cavities of different shapes and sizes (6.1 × 4.3 × 4.3 Å3 and 6.8 × 4.0 × 4.2 Å3), which were comparable with the size and shape of C3H4 (6.2 × 3.8 × 3.8 Å3) (Fig. 18).181 Single-component adsorption isotherms revealed that ELM-12 shows a sharp increasing adsorption for C3H6 with an uptake of 1.83 mmol g−1 at 298 K and 1 bar, as well as a large Qst of 60.6 kJ mol−1 for C3H6, indicating its strong interaction with the C3H6 molecule. In contrast, both the uptake capacity (0.67 mmol g−1 at 0.1 bar and 298 K) and Qst (15.8 kJ mol−1) of ELM-12 for C3H8 are significantly lower. The multiple interactions, such as weak or non-classical C–D⋯O hydrogen bonds, between ELM-12 and C3D4 molecules were further confirmed by high-resolution neutron powder diffraction studies. Breakthrough experiments demonstrated that high purity (99.9998%) of C3H6 can be obtained from a 1/99 C3H4/C3H6 mixture.
Fig. 18 (a) Crystal structure of ELM-12. (b) C3H4 and C3H6 adsorption isotherms of ELM-12. Reprinted with permission from ref. 181. Copyright 2017 American Chemical Society. |
In 2018, Chen et al. studied a series of MOFs with different types of structures, functionalities, and pore sizes (Fig. 19).182 Besides for highly selective C2H2/C2H4 separation,70,71 SIFSIX-type MOFs such as SIFX-1-Cu, SIFSIX-2-Cu-i, SIFSIX-3-Ni, and UTSA-200 also exhibit strong binding affinities for C3H4 compared to C3H6 and show high C3H4 adsorption capacities at very low pressure. The former three SIFSIX-MOFs show slightly larger pore sizes than both C3H4 and C3H6, which lead to moderate C3H4/C3H6 selectivity. The activated UTSA-200 with the optimal pore size (3.4 Å) and strong binding sites has the best separation performance for C3H4/C3H6. Single-component adsorption isotherms revealed that UTSA-200 exhibits the highest C3H4 uptake capacity of 95 cm3 cm−3 (2.99 mmol g−1) at 0.01 bar and 298 K, while adsorbs negligible C3H6 (0.33 mmol g−1, at 298 K and 0.4 bar), resulting in an extremely high IAST selectivity of 20000 for 1/99 C3H4/C3H6 at 298 K and 1 bar. Breakthrough experiments demonstrated that high purity (99.9999%) C3H6 can be yielded from 1:99 and 0.1:99.9 C3H4/C3H6 mixtures with a productivity of 62.9 mmol g−1 and 143.8 mmol g−1, respectively. Neutron powder diffraction studies and DFT-D calculations revealed that C3H4 molecules can open the pores of UTSA-200 and form strong C–H⋯F interactions with the framework.
Fig. 19 (a) DFT-D optimized structure and binding sites of UTSA-200⊃C3H4. (b) C3H4 and C3H6 adsorption isotherms of UTSA-200 at 298 K. Reprinted with permission from ref. 182. Copyright 2018 Wiley-VCH. |
In 2022, Xing et al. reported a flexible MOF GeFSIX-14-Cu-i (ZU-33, GeFSIX = hexafluorogermanate, and 14 = 4,4′- azopyridine), which exhibits guest/temperature-dependent structural dynamics and shows strong binding affinity towards acetylene and propadiene.188 ZU-33 featuring a 2-fold interpenetrated structure is composed of Cu(II)-4,4′-azobipyridne 2D layers and GeF62− pillars, and its pore size (3.08–5.04 Å) was dynamically adjustable by the rotational motion of GeF62− pillars and the organic ligands. Single-component gas adsorption experiments revealed that ZU-33 shows a steep uptake for alkynes (acetylene and propyne) and propadiene at low pressure (0.01 bar) and 303 K, while there is a threshold pressure for olefin adsorption and a size exclusion effect for alkanes. In addition, for C2H4 that is smaller than propyne and propadiene regarding the kinetic diameters, ZU-33 nearly inhibits C2H4 molecules to diffuse into its pores, suggesting the inverse size sieving below 0.5 bar at 303 K. Molecular simulations and single-crystal X-ray diffraction revealed that the interactions between the alkyne molecules (propyne and propadiene) and ZU-33 are more intense, thus requiring less input energy to overcome the energy barrier for the structural deformation. Breakthrough tests on a ZU-33 packed column verified that acetylene and propadiene can be directly removed from simulated cracking gases.
Xing et al. reported several interpenetrated anion-pillared ultra-microporous MOFs, such as GeFSIX-2-Cu-i (ZU-32), NbFSIX-2-Cu-i (ZU-52) and GeFSIX-14-Cu-i (ZU-33), and realized highly efficient separation of C4 olefins through molecular recognition.192 This series of materials show ultrafine-tuning of the pore size/shape (4.20–4.83 Å) by replacing pillared inorganic anions with different bulks and different lengths of organic ligands. Among them, NbFSIX-2-Cu-i with a pore aperture size of 4.31 Å (F⋯F distance) exhibits high C4H6 (2.64 mmol g−1) and n-C4H8 (2.26 mmol g−1) uptake but negligible i-C4H8 uptake (0.48 mmol g−1), showing uptake selectivities of about 5.00 and 5.74 for n-C4H8/i-C4H8 and C4H6/i-C4H8, respectively. In contrast, GeFSIX-14-Cu-i shows a smaller pore size of 4.20 Å (F⋯F distance), resulting in negligible adsorption of n-C4H8 (0.57 mmol g−1) and i-C4H8 (0.42 mmol g−1), but still retaining large uptake for C4H6 (2.67 mmol g−1), accompanying a gate-opening adsorption behavior for C4H6. Breakthrough experiments demonstrated that these materials can efficiently separate C4H6 from C4H6/n-C4H8/i-C4H8/He (50/15/30/5) mixtures, as well as efficiently separate C4H6/n-C4H8 (50/50) and n-C4H8/i-C4H8 (50/50) mixtures.
Because of its high degree of unsaturation and strong coordination ability, 1,3-C4H6 is commonly adsorbed preferentially over other C4 hydrocarbons by MOFs with functional sites. It is thus energy-intensive and might induce undesired polymerization as the purification involves capture of 1,3-C4H6 and its subsequent release through heating in general. Zhang et al. noticed that the collaborative interactions between the host framework and guest flexibility can significantly change the conformation of certain C4 hydrocarbons and thus exhibit abnormal adsorption and reversed selectivity (Fig. 20).193 In particular, a hydrophilic pore of a MAF with free N atoms, namely, [Zn2(btm)]2 (MAF-23), with 1D quasi-discrete pores (aperture size 3.6 Å, and cage size ca. 6 Å) was employed for separation of four hydrocarbons, n-C4H8, i-C4H8, C4H10 and 1,3-C4H6. As revealed by experimental and DFT calculations, n-C4H8, the most similar one to 1,3-C4H6 among these gas molecules, adopts a metastable cis conformation to form stronger non-classical C–H⋯N interactions, and hence has a significantly stronger binding affinity, whereas 1,3-C4H6 adopts the stable trans conformation and has the weakest binding affinity because of the unfitting configuration for forming stronger non-classical hydrogen-bonding interactions. In other words, MAF-23 with a unique pore structure and surface serves as a guest conformation-controlling adsorbent to achieve preferential adsorption of n-C4H8, i-C4H8 and C4H10 over 1,3-C4H6. Therefore, 1,3-C4H6 can be first eluted during the breakthrough operation under ambient conditions, and directly purified for the desired purity (≥99.5%) to meet the industrial requirement in one single separation operation.
Fig. 20 (a) Schematic diagrams of controlling the guest conformation through the quasi-discrete pore in MAF-23. (b) Breakthrough curves of MAF-23 for a 5:2:2:1 C4H6/n-C4H8/i-C4H8/C4H10 mixture. (c) Crystal structures of host–guest complexes of C4H6, n-C4H8, i-C4H8, and C4H10. Reprinted with permission from ref. 193. Copyright 2017 the American Association for the Advancement of Science. |
The separation of C4 geometric isomers is also a challenging separation process, among which the separation of trans/cis-2-butene is of prime importance to increase the value of C4 olefins. Ren et al. reported that M-gallate (M = Ni, Mg, and Co), featuring oval-shaped pores, are ideally suitable for shape-selective separation of trans/cis-2-butene through their difference in the minimum molecular cross-section sizes, in addition to a highly efficient separation of 1,3-butadiene, 1-butene, and i-butene.194 Mg-gallate displays a narrow pore window size of 3.6 × 4.6 Å2, capturing the smaller trans-2-butene (3.5 × 4.6 Å2) while excluding the slightly larger cis-2-butene (3.6 × 4.9 Å2), affording a high trans/cis-2-butene uptake selectivity of 3.19 at 298 K and 1.0 bar in single-component adsorption isotherms. DFT-D study showed that Mg-gallate interacts with trans-2-butene and 1,3-butadiene through short distances of intermolecular C⋯H–O interactions (C⋯H distances 2.57–2.83 and 2.45–2.79 Å, respectively).
The separation of isomeric C4 paraffins is also an important task in the petrochemical industry. Zhong et al. regulated the pore aperture of the cage-like Zn-bzc by stepwise installation of methyl groups on its narrow aperture to achieve both molecular-sieving separation and a high n-C4H10 uptake.195 The resulting Zn-bzc-2CH3 is not only a new benchmark adsorbent featuring molecular sieving for n-C4H10/iso-C4H10 separation and a high n-C4H10 adsorption capacity (2.42 mmol g−1), but also hydrophobic to eliminate the negative effect of water vapor on gas separation under humid conditions. Breakthrough tests proved that high-purity i-C4H10 (99.99%) can be collected. The minimum energy path of n-C4H10 and i-C4H10 from cage to cage passing through the narrow aperture was determined for Zn-bzc-nCH3 (n = 0, 1, 2), and the results suggested easy transports of both n-C4H10 and i-C4H10 for the larger apertures of the parent Zn-bzc MOF and Zn-bzc-CH3 due to the low energy barrier together with a small barrier difference, while kinetic forbiddance with a dramatical increase of the diffusion energy barrier from 23.8 to 131.6 kJ mol−1 for n-C4H10 to migrate through Zn-bzc-2CH3.
Eddaoudi et al. reported two new 12-connected rare-earth metal (Y3+ and Tb3+) fumarate based fcu-MOFs with both octahedral and tetrahedral cages that were solely interconnected with triangular windows of aperture size ca. 4.7 Å, and discovered that both of them can act as a adsorbate-size cut-off for the total sieving of C4 and C5 branched paraffins.196
In addition, Li et al. prepared two Zr-MOF compounds, Zr-bptc and Zr-abtc, which are highly stable with optimal pore structures for the separation of C6 alkane isomers (Fig. 21).197 For instance, Zr-abtc featuring an scu-type structure with 1D channels (d = 7 Å) accommodates all C6 alkane isomers (n-hexane, 3-methylpentane and 2,3-dimethylbutane), but favors n-hexane because of its stronger interactions with the pore surface, resulting in a mono/dibranched separation factor (∼1.3) in the breakthrough test.
Fig. 21 (a) and (c) Organic ligands, crystal structures, and topologies of Zr-bptc and Zr-abtc. (b) and (d) Breakthrough curves of an equimolar ternary mixture of C6 alkane isomers at 150°C for Zr-bptc (top) and Zr-abtc (bottom). The green curve represents the real-time RON of the eluted products. Reprinted with permission from ref. 197. Copyright 2018 Nature Publishing Group. |
In 2020, Li et al. reported a new flexible MOF, calcium chloranilate (HIAM-203), which specially possesses chloro-decorated 1D channels.198 HIAM-203 exhibits structural flexibility upon adsorption of C6 alkanes with different branching, as well as similar temperature-dependent adsorption behavior toward alkane isomers. It can take up a plentiful amount of n-hexane and 3-methylpentane at 30 °C, but completely excludes 2,2-dimethylbutane, while at 150°C 3-methylpentane is also excluded. This phenomenon may be rationalized by the significant difference in binding affinity near the pore aperture of HIAM-203. As the pore size of HIAM-203 (5.6 Å) is between the kinetic diameters of 3-methylpentane (5.5 Å) and 2,2-dimethylbutane (6.2 Å), it thus inhibits the diffusion of 2,2-dimethylbutane.
In 2023, Bao et al. employed the Hofmann-type MOFs, [M(pz)Ni(CN)4] (M = Co and Ni) to demonstrate similar temperature-swing molecular exclusion for separation of hexane isomers.199 CopzNi displays excellent separation efficiency for linear/mono-branched and mono-branched/di-branched alkanes with the highest adsorption capacity to date. CopzNi exhibits lower-energy regeneration, scalability, recyclability and high stability, representing a promising candidate for relevant separation processes.
There are also needs for purification of valuable C5-C7 olefins. Isoprene, which accounts for 15–25% of C5 fractions including important olefins like 1-pentene and trans-2-pentene, is widely used in the production of synthetic rubber, pharmaceutical and pesticide intermediates.200 The regeneration and desorption efficiency should also be taken into account for separation.201 Cui et al. found that anion-pillared hybrid porous materials, namely, ZU-62 (also termed NbOFFIVE-2-Cu-i) and TIFSIX-2-Cu-i, exhibit a good separation performance for C5 olefin mixtures (trans-2-pentene, 1-pentene and isoprene).202 Owing to a contraction of pore aperture originating from the rotation of 4,4′-dipyridylacetylene ligand, ZU-62 excludes the relatively large molecule of isoprene in the low pressure range (0–6 kPa), while TIFSIX-2-Cu-i is able to distinguish the three C5 olefins with a high uptake of trans-2-pentene (3.1 mmol·g−1), superior to that of zeolite 5A (2.0 mmol·g−1). DFT-D calculations confirmed that the selective adsorption was achieved by a favorable electrostatic environment as well as suitable pore confinement. Also, the regeneration tests showed that C5 olefins can be easily desorbed from ZU-62 and TIFSIX-2-Cu-i at 298 K.
MOFs featuring structural flexibility like breathing or gate-opening have been applied for separation of aromatic isomers.18,37,205 Li et al. reported that a stacked 1D manganese-based MOF [Mn(dhbq)(H2O)2] (Mn-dhbq, H2dhbq = 2,5-dihydroxy-1,4-benzoquinone) exhibits temperature-dependent discriminative adsorption of xylene isomers owing to reversible framework swelling.206 At 363 K, pX can be fully intercepted from the pX/mX/oX ternary mixture by a column of Mn-dhbq, whereas the effluent of the mX/oX mixture can be further separated by another column of Mn-dhbq at a lower temperature (303 K) where mainly oX finally flows out. The purity of pX is over 97% collected during the desorption cycle when using 1,4-diethylbenzene as an eluent at 433 K for 1 hour after liquid-phase adsorption of a quaternary mixture (pX/mX/oX/EB, 22/22/50/6) at 393 K. DFT calculations indicated that the temperature-dependent flexibility between 1D coordination chains (different degrees of swelling at different temperatures) endows such selective adsorption of xylene isomers through π–π stacking interactions with the aromatic ligand.
Xing et al. reported a flexible anion pillared MOF [Ni(bpy)2(NbOF5)] (ZU-61) with pcu topology and a pore size of 7.8 Å exhibiting efficient separation performance for xylene isomer.207 Single-component adsorption revealed that ZU-61 shows a higher low-pressure uptake for mX and oX than pX at 0.01 bar and 333 K, as well as a high capacity for mX (3.4 mmol g−1) and oX (3.2 mmol g−1). Breakthrough experiments for a 1:1:1 pX/mX/oX mixture confirmed that high purity (>99.9%) pX can elute from the column first, and then followed by mX and oX. The excellent performance for xylene isomer separation can be attributed to the rotational NbOF52− anions, which allows adaptive host–guest interaction (C–H⋯F interactions) depending on the shape of the xylene isomer, as confirmed by DFT calculations and crystallographic studies. These results showed that ZU-61 exhibits great potential for the purification of pX.
Given that all xylene isomers contain phenyl rings for π–π stacking interactions, another approach to enhance the separation selectivity would be utilizing the difference of their alkyl groups while inhibiting the interactions with phenyl rings. Yang et al. constructed a pillar-layered MOF Cu(bpdc)(ted)0.5 (ZUL-C3) by using poly-cycloalkane-type ligands to show a non-aromatic pore environment for xylene separation.208 The pore space of the MOF magnifies the difference of host–guest interactions with xylene isomers and ethylbenzene owing to their different distribution of methyl (ethyl) groups. Liquid-phase batch experiment indicated that this MOF can separate xylene isomers and ethylbenzene from each other, showing separation potential for oX/pX and oX/mX separation.
A flexible MOF, [Cu2(fbdim)]·p-xylene (MAF-41·pX), showing a 3D hinged-fence-like framework and 1D channels (4.2 × 9.8 × 10.1 Å3 cavities and 3.9 × 6.7 Å2 apertures), was demonstrated by Zhang et al. to exhibit unprecedented inversed molecular sieving (so called intermediate-sized molecular sieving) for the purification of styrene (Fig. 22).209 The framework structure can transform to a nonporous one upon removal of template molecules. The activated MAF-41 can adsorb styrene (ST) to restore the as-synthesized structure while totally excluding ethylbenzene (EB), toluene (Tol), and benzene (Bz). Styrene with a purity of 99.9%+ can be obtained from the multicomponent mixture after one single adsorption–desorption cycle because the pores are individually opened and simultaneously occupied by the target guest. The aperiodic pore opening is believed to avoid co-adsorption of guest molecules smaller than the opened pores. Kinetic sorption studies revealed that the EB/Tol/Bz adsorptions stayed quite low all the time, while the ST uptake of MAF-41 significantly increased for both the single-component and mixtures, which confirms no EB/Tol/Bz co-adsorption or replacement of ST in MAF-41. Although Cu(I) complexes and Cu(I)-based MOFs may have poor stability in air and/or water, guest-free MAF-41 did not collapse not only at temperatures up to 500 °C, but also in boiling water for at least one week, and even remained stable in a solution of pH 3–14 at room temperature for at least 3 days.
Fig. 22 (a) Crystal structure of guest-free MAF-41. (b) Adsorption isotherms of activated MAF-41 for ST (styrene, 298K), EB (ethylbenzene, 298K), Tol (toluene, 298K), Bz (benzene, 298K), N2 (77K), and CO2 (195 K). Reprinted with permission from ref. 209. Copyright 2019 Nature Publishing Group. |
In 2022, Li et al. reported a family of double-walled metal-dipyrazolate frameworks (BUT-53 to -58) composed of divalent metal ions and dipyrazolate ligands with different symmetries, lengths, and functionalities for trace benzene removal (Fig. 23).210 In this study, multiple merits, e.g., high stability, tunable pore, high adsorption capacity and selectivity, were integrated into these hydrophobic MOFs, which all exhibited high benzene uptakes (2.47–3.28mmolg−1) at room temperature and ultra-low pressures (<10Pa). BUT-55 is the best-performing adsorbent for the capture of trace benzene among them. It shows an extremely long breakthrough time of ∼8000 h g−1 for a benzene-containing (10 ppm, 10 mL min−1) gas mixture under both dry and humid (relative humidity = 50%) conditions. When the relative humidity was 80%, the breakthrough time decreased to ∼6000 h g−1, which is still much higher than that of other previously reported materials. After adsorption of benzene, BUT-55 can be regenerated under mild heating. As revealed by both the single-crystal structure of benzene-loaded BUT-55 and DFT calculations, multiple non-classical hydrogen-bonding C–H⋯X (X = N, O, π) interactions are the key to its strong affinity and high sensitivity toward benzene. The high benzene binding energy of BUT-55 contributes to its high adsorption selectivity of benzene over water or other volatile organic compounds (VOCs), such as cyclohexane and ethanol. It should also be pointed out that the BUT-55 sample is able to work continuously around one year under the breakthrough experiment conditions. In other words, a certain amount of BUT-55 can be used to capture trace airborne benzene for a long time due to its high benzene adsorption capacity under ultra-low pressures and high adsorption selectivity. The performance of these MOFs demonstrates high potential in the removal of benzene from ambient air.
Fig. 23 (a) Structures of C6H6@BUT-55 and benzene–benzene interactions. (b) Logarithmic-scale plots of P/P0 to view the benzene adsorption of BUT-53 to BUT-58 at low partial pressure. Reprinted with permission from ref. 210. Copyright 2022 Nature Publishing Group. |
Very recently, Mo et al. reported a flexible MOF, [Sr2(BINDI)(H2O)2)] (WYU-62, H4BINDI = N,N′-bis(5-isophthalic acid)-naphthalenediimide) with electron-deficient NDI cores, which shows fast adsorption of trace benzene vapor at low pressure, accompanying a fluorescence-enhanced sensing (limit of detection = 0.133 mgL−1).211 WYU-62 could be easily obtained by immersing the as-synthesized MOF [Sr2(BINDI)(DMF)(H2O)] (MYU-61) in water, during which discrete 0D pores of MYU-61 have transformed to 1D channels (aperture size = 5.1 × 9.1 Å2). Aromatic hydrocarbon vapor adsorption isotherms revealed that WYU-62a can show high benzene uptake at very low pressure (P/P0 < 0.01). DFT calculations and crystallographic studies indicated that electron-rich benzene was tightly wrapped between the two electron-deficient NDI moieties with strong π–π and C−H⋯π interactions. Therefore, it has excellent benzene adsorption capacity, whereas the accompanying host–guest charge transfer enables visual detection of trace benzene vapor.
Modification of MOF membranes with the composite ionic liquid/Ag+ (IL/Ag+) can efficiently improve their olefin/paraffin separation properties. Yang et al. synthesized layered Zn2(bim)4 membranes215 using the in situ interfacial assembly (ISIA)216 method and further modified them with varied IL/Ag+ composites.217 Adsorption isotherms for Zn2(bim)4 powder and its IL/Ag+ modified sample showed that the adsorption capacity for olefin can significantly improve after modification with IL/Ag+ but the adsorption for paraffin shows negligible changes, which is attributed to the strong π-complexation of olefins with Ag+. Further study revealed that the pristine Zn2(bim)4 membrane showed a C3H6/C3H8 separation factor of 1.14 with a C3H6 permeance of 106 GPU (SFC2H4/C2H6: 1.42, and PC2H4: 311) (Fig. 24). In contrast, the modified membranes exhibited a significant improvement in olefin/paraffin separation with the optimized C3H6/C3H8 separation factor of 28.8 ± 3.8 with the C3H6 permeance of 129.8 ± 40.4 GPU (SFC2H4/C2H6: 12.0 ± 2.2, and PC2H4: 45.6 ± 23.7 GPU). The preferential binding affinity of Ag+ in IL for olefins facilitates the delivery of olefins in the modified Zn2(bim)4 membranes. On the other hand, Ag+ filling in the space of laminated modified Zn2(bim)4 membranes further blocks paraffin penetration and thus improves the olefin/paraffin selectivity. In addition to the composite modification membrane strategy, intrinsic structural regulation of MOF membranes is also crucial. Recently, a series of Zn2(bim)4 membranes functionalized with different amounts of amino groups, namely, Nx-Zn2(bim)4(x represents the molar ratio of raw 5-aminobenzimidazole, bim) were also investigated for separation.218 Among them, the N10-Zn2(bim)4 membrane exhibits the highest H2/CO2 separation performance with a separation factor of 1158 and a H2 permeance of 1417 GPU. Moreover, its ideal selectivities for H2/CO2, H2/CH4 and H2/C3H8 were 829, 99, and 33, respectively, showing a distinct size exclusion effect for relatively large molecules.
Fig. 24 (a) C3H6/C3H8 separation performance of Zn2(bim)4 membranes modified by diversified composites, IL/Ag+(8-0), IL/Ag+(8-1), IL/Ag+(8-2) and IL/Ag+(8-5). (b) C2H4/C2H6 separation performance of Zn2(bim)4 membranes modified by diversified composites, IL/Ag+(8-1), IL/Ag+(8-2) and IL/Ag+(8-5). Reprinted with permission from ref. 217. Copyright 2021 Elsevier. |
Long et al. fabricated a series of membranes with M2(dobdc) (M = Co, Ni, Mg, and Mn) as fillers and 6FDA-DAM as the primary polymer by reducing the filler size to the sub-100 nm level to specially improve the filler-polymer compatibility and dispersion.219 Among them, Ni2(dobdc) showed the best C2H4/C2H6 separation performance without reduction in selectivity even under high-pressure owing to the presence of strong and multiple nanocrystal-polymer interactions, which suppresses plasticization by reducing polymer chain mobility.
Polycrystalline MOF membranes are less explored but also important. Liu et al.220 have recently prepared a polycrystalline Co-gallate membrane with a reported freezing contra-diffusion protocol221 that can enable more accurate control over the reaction kinetics between metal ions and ligands to effectively tune the MOF nucleation and growth in the bulk solution. Maintaining the frozen state of the metal precursor inside the macroporous α-Al2O3 substrate resulted in the formation of the preferred c-oriented and well-intergrown Co-gallate membrane with not only abundant open metal sites (at the increased missing-linker defects), but also reduced the thickness of the membrane. The multiscale structure endows the Co-gallate membrane with an outstanding C2H4/C2H6 separation performance superior to those of state-of-the-art membranes including polycrystalline MOF membranes, MOF-based MMMs, and polymeric membranes. The optimized C2H4/C2H6 selectivity is 8.3 with a C2H6 permeance of 72.6 GPU. The resultant membrane also shows a negative correlation with the operation temperature and high long-term stability.
There are many important issues remaining unaddressed before further industrial and commercial usage of MOFs. Shaping/pelleting of MOFs would be the first step in actual processes given engineering considerations, but that would lead to loss of adsorption capacity; thus, further study on mechanical stabilities of MOFs might be necessary. Simultaneously, the diffusion kinetics of MOF pellets should be comprehensively investigated. There are also concerns on current research for evaluations of their separation performances through swing adsorption or membrane separation processes, as these evaluations mainly focus on evaluating candidate materials under simulated conditions rather than the actual applications. In relevant simulated evaluations, the presence of contaminants such as water has gradually got involved. In contrast, the actual gas streams would be more complicated, while the separation condition can be even harsher (under elevated pressures/temperatures), which require the adsorbents to show good stability and durability, including good water resistance and impurity tolerance. The long-term durability and regeneration of MOFs during separation processes have been rarely involved in current research. Moreover, systematic evaluation of materials production, including capital and operating costs, should be performed prior to large-scale deployments of MOF-based adsorptive separation technology. Solvent-free and continuous synthesis methods have been demonstrated to be applicable for MOFs, which show great potential for large-scale production of MOF materials. In addition, new technical issues such as thermal management during the adsorption process would come out when sorption is scaled up. For membrane-based separation, there are also several challenges although it is capable of direct production of pure gas and can be simply operated under mild conditions. Several mixed-matrix MOF-based membranes have been developed, which show large permeance differences for hydrocarbon separation. However, the processability, defect, compatibility, and scaling up in membrane fabrication as well as the permeability-selectivity trade-off are still quite challenging. In terms of membrane separation, molecular sieving of hydrocarbons is still highly desirable. As the structure numbers of MOFs keep growing, there are also emerging technologies like machine learning under artificial intelligence for the computational design and discovery of novel MOF materials, while automated chemistry for high-throughput screening is also possible by combination with robotics.
As promising adsorbent materials for hydrocarbon separation, MOFs with high separation performance can be synthesized by combination of rational control of their pore size and pore surface. Continuous collaborative efforts among scientists, engineers and industrial partners will promote the application of MOF adsorbents to scientifically and technologically important industrial hydrocarbon separation, which would reap great benefits for society.
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