Ryan
Luebke
a,
Youssef
Belmabkhout
a,
Łukasz J.
Weseliński
a,
Amy J.
Cairns
a,
Mohamed
Alkordi
a,
George
Norton
b,
Łukasz
Wojtas
b,
Karim
Adil
a and
Mohamed
Eddaoudi
*a
aFunctional Materials Design, Discovery & Development Research Group (FMD3), Advanced Membranes & Porous Materials Center, Division of Physical Sciences and Engineering, King Abdullah University of Science and Technology (KAUST), Thuwal 23955-6900, Kingdom of Saudi Arabia. E-mail: mohamed.eddaoudi@kaust.edu.sa
bDepartment of Chemistry, University of South Florida, 4202 East Fowler Avenue, Tampa, Florida 33620, USA
First published on 15th April 2015
A series of highly porous MOFs were deliberately targeted to contain a 12-connected rare earth hexanuclear cluster and quadrangular tetracarboxylate ligands. The resultant MOFs have an underlying topology of ftw, and are thus (4,12)-c ftw-MOFs. This targeted rare earth ftw-MOF platform offers the potential to assess the effect of pore functionality and size, via ligand functionalization and/or expansion, on the adsorption properties of relevant gases. Examination of the gas adsorption properties of these compounds showed that the ftw-MOF-2 analogues, constructed from rigid ligands with a phenyl, naphthyl, or anthracene core exhibited a relatively high degree of porosity. The specific surface areas and pore volumes of these analogs are amongst the highest reported for RE-based MOFs. Further studies revealed that the Y-ftw-MOF-2 shows promise as a storage medium for methane (CH4) at high pressures. Furthermore, Y-ftw-MOF-2 shows potential as a separation agent for the selective removal of normal butane (n-C4H10) and propane (C3H8) from natural gas (NG) as well as interesting properties for the selective separation of n-C4H10 from C3H8 or isobutane (iso-C4H10).
Fig. 1 Left, the 12-connected rare earth hexanuclear cluster, [RE6(μ3-OH)8(O2C–)12].11 Right, illustration of the MBB coordination geometry: note the positions of the carbon atom of the carboxylates match the vertices of the cuboctahedron. |
The aforementioned RE-based hexanuclear cluster is a suitable MBB for the rational design of highly-connected MOFs as its inherent geometry and high connectivity permit only a limited number of possible topological outcomes for subsequent assembly, making it ideal for the effective practice of reticular chemistry. In this work, the focus is on utilizing 4-connected quadrangular carboxylate-based ligands (Fig. 2 and 3) to synthesize rare earth MOFs having both 12-c and 4-c nodes. There are a total of three known (4,12)-c edge transitive binodal nets, all of which are constructed from one kind of edge and therefore offer the prospect of constructing MOFs with such topologies through use of a single type of symmetrical ligand. Of the three (4,12)-c nets (shp, ftw, ith),10 the ftw topology is the only one composed of 12-connected nodes matching the cuboctahedron vertex figure in the 12-c RE hexanuclear MBB, [RE6(OH)8(O2C–)12], (Fig. 1).
Accordingly RE-MOFs with an underlying topology of ftw (ftw-MOFs) have been purposely targeted13,14,17–19 by employing 4-connected quadrangular tetracarboxylate ligands in combination with the 12-c cuboctahedron MBB. This targeted RE ftw-MOF platform offers the potential to systematically assess the effect of pore functionality and size via ligand functionalization and/or expansion (Fig. 3) by investigating the adsorption properties of relevant gases.
Herein we report a successful reticular chemistry method, where the newly isolated 12-c RE MBB allows the synthesis of a series of highly porous RE-MOFs including Y-ftw-MOF-2, which to the best of our knowledge has the highest specific surface area ever reported for a RE-MOF. Specifically, a tetratopic carboxylate-based ligand with a square-like geometry was reacted with a variety of rare earth metal salts under appropriate reaction conditions – including the use of a fluorinated modulator15 – to predictably form ftw-MOFs (ftw-MOF-1). Furthermore, ligand expansion was achieved via elongating the central core and/or extending the four arms, resulting in two relatively more open ftw-derived MOFs (ftw-MOF-2 and ftw-MOF-3, see Fig. 2 and 3). The versatility of this platform was evidenced by the construction of ftw-MOFs where the central core of the ligand was functionalized/decorated (i.e. three related ligands having a central phenyl (ftw-MOF-2), naphthalene (ftw-MOF-2 (Naphth)), or anthracene (ftw-MOF-2 (Anth)) based core, see Fig. 2 and 3).
As anticipated, based on previous work from our group, the in situ formation of the 12-c rare earth MBB was facilitated by the addition of excess 2-fluorobenzoic acid (2-FBA), a modulator and a directing agent for the in situ formation of highly-connected polynuclear carboxylate-based clusters.15 This allowed for the synthesis of yttrium, terbium, and ytterbium ftw-MOF-1 analogs. Y-ftw-MOF-1 was structurally characterized by single-crystal X-ray diffraction (SCXRD) and phase purity of the Y, Tb and Yb analogs was confirmed by Whole Profile Pattern Matching using the Le Bail method (Fig. S4a, ESI†, Table 1).23
Compound | Y-ftw-MOF-1 | Y-ftw-MOF-2 | Y-ftw-MOF-3 |
---|---|---|---|
a R int is missing due to the fact that de-twinned data have been imported from an FCF file (containing merged data) generated by Shelxl-2013 with LIST 8 instruction. | |||
Formula | C114H86O52Y6 | C138H78O35Y6 | C162H78O32Y6 |
FW | 2821.29 | 2829.46 | 3069.70 |
Crystal system | Cubic | Cubic | Cubic |
Space group | Pmm | Im | Im |
a (Å) | 19.3042(5) | 40.048(3) | 48.111(16) |
V (Å3) | 7193.8(3) | 64229(13) | 111362(112) |
Z, Dcal (g cm−3) | 1 | 8 | 8 |
θ max (°) | 131.92 | 88.92 | 72.688 |
R int | 0.0577 | 0.1045 | n/aa |
R 1 (I > 2σ(I0)) | 0.0834 | 0.0983 | 0.0779 |
wR2 (all data) | 0.2626 | 0.2493 | 0.2196 |
GOF | 1.189 | 1.174 | 0.871 |
Δρmax/Δρmin (e Å−3) | 0.60/−0.88 | 2.27/−0.83 | 1.01/−0.63 |
SCXRD studies revealed that ftw-MOF-1 crystallized in the cubic Pmm space group and was formulated as |(DMA)2|[(Y6(μ3-OH)8(H2O)6)(TetPOMB)3]·(solv)x; DMA = dimethylammonium cations, solv = solvent. Topological analysis confirmed that the material had the expected ftw topology (Fig. S1, ESI†). The ftw-MOF-1 structure can be viewed as a primitive cubic packing of the 12-c rare earth MBBs, which are positioned in the center of the unit cell. The 12-c rare earth MBBs are connected through 12 bis-monodentate carboxylates from the 12 separate TetPOMB ligands (Fig. 4), thus forming one central cubic cage ∼19 Å in diameter that is delimited by six TetPOMB ligands (Fig. 4). Due to the flexibility of the ether linkages of the ligand, its central phenyl core is disordered over four positions in the crystal structure. Preliminary CO2 and N2 adsorption studies revealed that ftw-MOF-1 was not permanently porous using conventional activation procedures. In fact, numerous attempts to activate the ftw-MOF-1 samples for gas sorption analysis resulted in loss of crystallinity. We attributed this lack of robustness to the flexibility in the ligand, which plausibly resulted in the collapse of the material upon guest molecule removal.
Fig. 4 Molecular and vertex figure representation of ftw-MOF-1, yellow spheres denote the open space within each cage; (top left) TetPOMB ligand coordinated to four 12-connected hexanuclear clusters and (bottom right) vertex figure representation.11 |
The ftw-MOF-2 structure is composed of ligands with a para-terphenyl core covalently linked in the 3,3′′,5,5′′ positions to the para position of benzoate moieties, thus forming a rectangular 4-c MBB (Fig. 5). A cubic cage ∼12 Å in diameter, with Th symmetry, is delimited by six ligands: the carboxylates coordinate to the four 12-c RE MBBs positioned at the vertices of the cube face on which the ligand is situated. Compared to the parent ftw-MOF-1, the 12-c MBBs (the hexanuclear [RE6(OH)8(O2C–)12] carboxylate-based clusters) are rotated ∼15° out of perfect alignment along all three axes (i.e. in the x, y and z directions), adapting the orientation to allow for the accommodation of the rectangular ligand (Fig. 5). Consequently, the ligands on the faces of the central cage are all puckered inward. The ligands in the yz-plane are oriented lengthwise in the z-direction; the ligands in the xy-plane are oriented lengthwise in the y-direction; and the ligands in the xz-plane are oriented lengthwise in the x-direction (Fig. 6 and S9, ESI†). Adjacent to, and sharing one face of the cubic cage, are six larger cages with D2h symmetry. This larger cage (21 Å × 21 Å × 12 Å) is a distorted cube delimited by six ligands. The ligands on any two parallel faces are oriented in the same direction with respect to one another and puckered inward; the remaining four faces are puckered outward and the ligands are oriented end to end lengthwise (Fig. 6 and S10, ESI†).
Fig. 5 Illustration of the ligand geometry effect on the orientation of the 12-c cluster in ftw-fragment of ftw-MOF-1 (left) and ftw-MOF-2 (right).11 |
Evidently, from a structural perspective, further isoreticular expansion of the ftw-MOF platform could be accomplished through extension of the arms of the TCPT ligand. Indeed, Y-ftw-MOF-3 was synthesized from 3,3′′,5,5′′-tetrakis[2-(4-ethoxycarbonylphenyl)ethynyl]-p-terphenyl (TCEPT) with alkyne moieties extending the four arms of the TCPT ligand (Fig. 2 and 3). The SCXRD studies revealed that Y-ftw-MOF-3 crystallized in the cubic Im space group and was formulated as |(DMA)2|[(Y6(μ3-OH)8(H2O)6)(TCEPT)3]·(solv)x. Structural analysis revealed that connectivity and ligand orientation in the isoreticular Y-ftw-MOF-3 was similar to the aforementioned Y-ftw-MOF-2. The minimum diameter of the central highly symmetric cubic cage was ∼19 Å (Fig. S11, ESI†) and the cuboidal cage had dimensions of approximately 23 Å × 22 Å × 18 Å (Fig. S12, ESI†). Notably, the cages in Y-ftw-MOF-3 were relatively less distorted than in Y-ftw-MOF-2, as the geometry of the TCEPT ligand is closer to a square than TCPT. This resulted in less strain and torsion as well as a slightly less pronounced rotation of the 12-c MBB. In comparison to the parent ftw-MOF-1, the MBB was rotated only by ∼10° out of perfect alignment along all three axes (i.e. in the x, y and z directions).
SCXRD studies revealed that Y-ftw-MOF-2 (Naphth) crystallized in the cubic Im space group. A modeled structure, based on PXRD and a unit cell determination from single crystal data, was formulated as |(DMA)2|[(Y6(μ3-OH)8(H2O)6)(TCDPN)3]·(solv)x. Experimental PXRD patterns matched the calculated PXRD from the modeled structure. This confirmed the attainment of the anticipated isoreticular structure, Y-ftw-MOF-2 (Naphth). The structure of the Y-ftw-MOF-2 (Naphth) analogue differs from the parent ftw-MOF-2 with regard to the orientation of the bicyclic central core of the ligands: the bulkier naphthalene core is rotated 90° out of plane (Fig. S13 and S14, ESI†). Similarly, the resultant functionalized ftw-MOFs enclose two distinct cages. Namely, a highly symmetric cubic cage, with Th symmetry, delimited by six ligands which are puckered outward with the bulk of the naphthalene core pointed toward the center of the cage, and with a minimum cage diameter of ∼9.5 Å. The 12-c MBBs are rotated ∼13° out of perfect alignment along all three axes (i.e. in the x, y and z directions). Adjacent to, and sharing one face of, the cubic cage, are six symmetry related cuboidal cages with D2h symmetry. These cages, with minimum diameters of approximately 14 Å, 13 Å and 10 Å, are delimited by six ligands, two of which are puckered outward having the bulk of the naphthalene core pointing inward, and the other four ligands are puckered inward with the bulk of the naphthalene core pointing outward into the adjacent cage.
Confirmation of the successful synthesis of Y-ftw-MOF-2 (Anth) was only possible by unit cell indexing from a poor quality highly twinned crystal and further comparing the experimental powder pattern to a modeled and geometry optimized Y-ftw-MOF-2 (Anth) structure (Fig. S7, ESI†). The determined structure was consistent with the Y-ftw-MOF-2 (Naphth) structure with regard to connectivity and ligand geometry. Accordingly, the Y-ftw-MOF-2 (Anth) structure was modeled based on Y-ftw-MOF-2 (Naphth), and further functionalized and geometry optimized in Materials Studio. The Y-ftw-MOF-2 (Anth) encloses two unique cages. The first is a highly symmetric cubic cage, with Th symmetry and a minimum diameter of ∼7 Å (Fig. S15, ESI†). This cage is delimited by six ligands which are puckered inward; the anthracene core is rotated perpendicular to the plane of ligand. The 12-c MBBs are oriented similarly to Y-ftw-MOF-2 (Naphth), i.e. rotated ∼13° out of perfect alignment along all three axes (i.e. in the x, y and z directions). The second cage is a cuboidal cage with D2h symmetry (Fig. S16, ESI†), and minimum diameters of approximately 14 Å, 12 Å and 5 Å. It is delimited by six ligands, two of which are puckered inward while the other four ligands are puckered outward: the anthracene core is rotated and adopts an orientation perpendicular to the plane of the ligand.
Similar to the recently reported rare earth based (3,18)-connected gea-MOF-1,25 Y-ftw-MOF-2 maintained its crystallinity up to 400 °C (Fig. S5a, ESI†) and retained its optimal porosity upon heating beyond 200 °C in vacuo, indicative of a high degree of thermal stability. It is worth mentioning that most other examples of highly thermally stable MOFs are not often supported by porosity measurements after such high temperature treatment.
In order to assess the structure–properties relationship for Y-ftw-MOF-2, gas adsorption measurements were undertaken for CO2, N2, CH4 and H2 at 298 K at low and high pressures. H2 and CO2 showed weak interactions with Y-ftw-MOF-2, as evidenced by their relatively low isosteric heats of adsorption, Qst: 5.7 and 27 kJ mol−1 for H2 and CO2, respectively, at low loading. The Qst values were determined from variable temperature adsorption isotherms at 258, 268 and 278 K for CO2 (Fig. S23 and S24, ESI†) and at 77 K and 87 K for H2 (Fig. S27, ESI†).
The CO2 adsorption isotherm at high pressure (Fig. S30a and S31a, ESI†) indicated a nearly full saturation of the pore system at 25 bar and 273 K (24.62 mmol g−1). This corresponds to a pore volume of 1.17 cm3 g−1 that is in close agreement with the theoretical pore volume calculated from the Ar isotherm at 87 K (1.26 cm3 g−1). The volumetric CO2 uptake at 25 bar and 298 K (278 cm3 (STP) cm−3) was slightly lower (∼7%) than UTSA-20 (ref. 7) (300 cm3 (STP) cm−3) under similar conditions.
Examination of absolute gravimetric (mmol g−1) and volumetric (cm3 (STP) cm−3) CH4 uptake at intermediate and high pressures revealed that Y-ftw-MOF-2 adsorbed 32 and 174 cm3 (STP) cm−3 of CH4 at 5 and 50 bar, respectively (Fig. S30b, ESI†). The resultant CH4 working storage capacity, assuming 50 bar as the highest adsorption pressure and 5 bar as the lowest desorption pressure (following the requirement of the engine methane injection pressure),26 is ca. 142 cm3 (STP) cm−3 (Table S4, ESI†). This volumetric working capacity, based on the crystallographic density of Y-ftw-MOF-2, is significantly higher than UTSA-20 (ref. 7) (80 cm3 (STP) cm−3) and higher than PCN-14 (ref. 5) (130 cm3 (STP) cm−3) but still lower than the working CH4 storage capacity calculated for NU-125 (ref. 26) (165 cm3 (STP) cm−3), tbo-MOF-2 (ref. 20) (152 cm3 (STP) cm−3) and other recently reported MOFs4,27,28 (Table S4, ESI†). The CO2/N2 and CO2/CH4 selectivity, determined using ideal adsorption solution theory (IAST), was moderate in comparison to other best performing MOFs and other classes of CO2 separation agents (Fig. S30b, ESI†).
Encouraged by the higher CH4 uptake of Y-ftw-MOF-2, adsorption of larger and relatively highly polarizable probe molecules such as C2H6, C3H8 and n-C4H10 and iso-C4H10 (C2+) were also investigated (Fig. 7). The results were compared with the corresponding CO2 and CH4 adsorption data and subsequently the C2+/CH4 and n-C4H10/iso-C4H10 separation factors were derived (Fig. S32, ESI†). Interestingly, C2+ adsorption isotherms were much steeper at low pressures than for CH4 and CO2, indicative of a plausibly higher affinity of Y-ftw-MOF-2 for C2+. Examination of single adsorption isotherm data using IAST confirmed the high C2+/CH4 selectivities, namely at 1 bar the selectivity was ca. 50 for C3H8/CH4 (5/95) and ca. 450 for n-C4H10/CH4 (5/95) (Fig. S32a, ESI†). In addition, Y-ftw-MOF-2 exhibited selectivities of 6 and 2.5 in 50/50 mixtures of n-C4H10/C3H8 and n-C4H10/iso-C4H10, respectively, at 1 bar and 298 K (Fig. S32b, ESI†). Accordingly, Y-ftw-MOF-2 offers promise as a separation agent, particularly for n-C4H10 in CH4 containing gas streams.
Fig. 7 Single-gas adsorption isotherms for CO2, CH4, C2H6, C3H8, n-C4H10 and iso-C4H10 on Y-ftw-MOF-2. |
Similar to Y-ftw-MOF-2, weak CO2 and H2 interactions were observed for Y-ftw-MOF-2 (Naphth) and Y-ftw-MOF-2 (Anth), where the Qst values at low loading were 25 and 22 kJ mol−1 CO2 and 6.4 and 6.9 kJ mol−1 for H2, respectively (Fig. S25, S26, S28 and S29, ESI†).
In order to assess the effect of the bulkier naphthalene core on the CO2 and C2+ uptakes, gas sorption studies were performed on Y-ftw-MOF-2 (Naphth). Based on single component adsorption isotherm data, the added functionality (bulkier core, reduced pore size) had a minimal impact on the adsorption properties and selectivity toward CO2 and C2+ (Fig. S33–S37, ESI†). It is foreseeable that the inclusion of aliphatic or polarized groups may offer more promising results.15 Accordingly, further experiments are ongoing to construct ftw-MOFs decorated with suitable functionalities for gas separation. Regarding ftw-MOF-3, work is in progress to determine the optimum activation conditions prior to performing detailed sorption studies.
Footnote |
† Electronic supplementary information (ESI) available: Materials and methods, synthesis of ligands, NMR spectra, synthesis of MOFs, additional structural figures, PXRD, TGA, low and high pressure gas adsorption isotherms, Qst analysis and IAST calculation. CCDC 1050062–1050064. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c5sc00614g |
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