DOI:
10.1039/C5RA21980A
(Paper)
RSC Adv., 2016,
6, 1388-1394
A multifunctional cadmium–organic framework comprising tricarboxytriphenyl amine: selective gas adsorption, liquid-phase separation and luminescence sensing†‡
Received
21st October 2015
, Accepted 14th December 2015
First published on 17th December 2015
Abstract
The reaction of tricarboxytriphenyl amine (H3TCA) with CdII and auxiliary ligand 4,4′-bis(1-imidazolyl)biphenyl (bimb) afforded [Cd3(TCA)2(bimb)·(DMA)6]n (1) containing a two-fold interpenetrating three-dimensional microporous framework. Compound 1 showed remarkable adsorption enthalpies for CO2 and H2 and good H2/N2 selectivity at low temperature. Moreover, activated 1 showed a highly selective adsorption towards CO2 over N2 and CH4 under ambient conditions. Interestingly, compound 1 selectively removed methyl orange (MO) over methylene blue (MB) from contaminated water with good recyclability, and possessed the second highest adsorption capacity for MO among the MOFs reported to date. Remarkably, complex 1 showed strong guest-dependent luminescence behavior.
Introduction
Metal–organic frameworks (MOFs) with inherent structural diversities and functional properties, represent a class of crystalline material formed from organic electron-donor linkers and metal cations, demonstrating prominent applications in strategic storage and gas separation, chemical sensing, catalysis, and medical application.1–7
Selective capture of CO2 is very important for the purification of natural gases and the reduction of CO2 emissions.8,9 Employing basic nitrogen-containing organic groups into MOFs has been considered to be advantageous for the selective adsorption of CO2.10,11 Typically, the interaction involving the localized dipoles of the N-containing group and the quadrupole moment of CO2 would induce the dispersion and electrostatic forces, thus improving the CO2 adsorption and separation abilities of MOFs. Recently, using MOFs in liquid-phase adsorption of harmful dyes has drawn great attention,12–14 due to their tunable pore structures,15 relatively heterogeneous surfaces,16 and potentially strong electrostatic interactions with the guest molecules.17 The selectivity and recyclability, adsorption capacity and stability are all crucial for high-performance liquid-phase separation using MOFs. Nowadays, the permanent porosity of some luminescent MOFs favored reversible storage and release of guest substrates, as well as provided differential recognition sites to guest species; and therefore, they were successful in sensing of ions and small molecules.18–22 Even more remarkably, these applications were combined and integrated into individual frameworks to construct multifunctional MOFs.23–25 Despite a tremendous progress in the field of MOFs, currently, it remains extremely challenging to insert more complex functionalities within the lattice in a rational and systematic manner.
In our effort aimed at multifunctional MOFs, tricarboxytriphenyl amine (H3TCA, Scheme S1‡)26–31 and CdII were selected in the presence of auxiliary ligand 4,4′-bis(1-imidazolyl)biphenyl (bimb) to synthesize MOFs based on the following reasons: (1) the collaborative interaction between d10 cadmium(II) and photoactive nitrilotribenzoate organic ligand facilitates the generation of the architecture with enhanced fluorescence; (2) Lewis base triphenylamine sites on the internal surface of framework may prompt the selective adsorption of CO2. Herein, we successfully prepared a two-fold interpenetrating three-dimensional (3D) microporous MOF [Cd3(TCA)2(bimb)·(DMA)6]n (1) that demonstrates impressive adsorption enthalpies for CO2 and H2 and exhibits good H2/N2 selectivity at lower temperature. Moreover, activated 1 showed highly selective adsorption towards CO2 over N2 and CH4 under ambient conditions. Interestingly, compound 1 selectively removed methyl orange (MO) over methylene blue (MB) from contaminated water with a good recyclability. To the best of our knowledge, 1 showed the second highest adsorption capacity for MO among the MOFs up to now. Remarkably, complex 1 showed a strong guest-dependent luminescence behavior, enabling it as a promising luminescent probe for detecting small molecules from their photoluminescence (PL) spectra.
Experimental
Materials and measurements
All the commercially available chemicals were of reagent grade and used as received without further purification. Elemental analyses for C, H and N were determined on a Perkin-Elmer 240 elemental analyzer. IR spectra were recorded in the 4000–400 cm−1 region on a Bruker Vector 22 spectrophotometer using KBr discs. Thermogravimetric analyses (TGA) were conducted on a TA-SDT 2960 at a heating rate of 10 °C min−1 under N2 atmosphere. Powder X-ray diffraction (PXRD) data were collected on a Siemens D5005 diffractometer using CuKα radiation over the 2θ range of 5–30°. UV-vis spectra were collected on a TU-1900 double-beam spectrophotometer. Fluorescent spectra were measured on a Varian Cary Eclipse fluorescence spectrophotometer. The 1-solvent emulsions were prepared by introducing 5 mg of 1 powder into 5.00 mL of methanol, ethanol, and water. Ultra high purity-grade (99.999%) N2, H2, CO2, and CH4 were used for gas sorption measurements, which were carried out on a Quantachrome IQ2 automatic volumetric instrument. The methanol-exchanged samples were degassed at 393 K for 12 h under a dynamic vacuum to remove guest solvent molecules.
Synthesis of [Cd3(TCA)2(bimb)·(DMA)6]n (1)
A mixture of Cd(NO3)·4H2O (15.4 mg, 0.05 mmol), H3TCA (4.9 mg, 0.01 mmol), and bimb (14.3 mg, 0.05 mmol) in a N,N-dimethylacetamide (DMA, 3 mL) was sealed in a 25 mL Teflon-lined autoclave and heated at 110 °C for 2 days and then slowly cooled to room temperature. Yellow crystals of 1 were obtained (81% yield based on Cd). Anal. calcd. for 1 (C84H92Cd3N12O18): C, 53.24; H, 4.89; N, 8.87%; found: C, 53.56; H, 4.01; N, 8.70%. IR spectrum (cm−1): 2930w, 1595s, 41m, 1311m, 1269m, 1173w, 1103w, 1064w, 1014w, 962w, 932w, 831w, 784m, 712w, 675w, 523w, 437w.
X-ray crystallography
The crystallographic data of 1 was collected using a Bruker Smart Apex CCD area-detector diffractometer equipped with graphite-monochromated Mo Kα radiation (λ = 0.71073 Å) at 173 K using the ω-scan technique. Data reductions and absorption corrections were respectively performed with SAINT32 and SADABS33 software packages, respectively. The structure was solved by direct methods, and refined anisotropically with SHELXL-97 (ref. 34) using full-matrix least-squares procedures based on F2. The disordered segments were subjected to geometric restraints during the refinements. The distribution of peaks in the channels of 1 was chemically featureless to refine using conventional discrete-atom models. To solve the problems, the free solvent molecules were removed by the SQUEEZE routine in PLATON.35 The number of solvent molecules in 1 was obtained by element analysis and TG. The crystallographic data were deposited in the Cambridge Crystallographic Data Centre: CCDC 1057133. The relevant crystallographic data are presented in Table 1; the selected bond lengths and angles are given in Table 2.
Table 1 Crystallographic data and other pertinent information for 1
|
1 |
Formula |
C60H38Cd3N6O12 |
Formula weight |
1372.16 |
Crystal system |
Monoclinic |
Space group |
P2/n |
a/Å |
17.7101(9) |
b/Å |
13.2378(5) |
c/Å |
17.8690(9) |
α/° |
90 |
β/° |
90.847(2) |
γ/° |
90 |
V/Å3 |
4188.8(3) |
Z |
2 |
ρcalcd/g cm−3 |
1.088 |
μ/mm−1 |
0.800 |
Collected reflections |
20691 |
Unique reflections |
7545 |
R1 [I > 2σ (I)] |
0.0434 |
wR2 (all data) |
0.1234 |
Table 2 Selected bond distances (Å) and angles (deg) for 1a
Symmetry codes for 1: #1 x, −1 + y, z; #2 3/2 − x, −1 + y, 5/2 − z; #3 3/2 − x, y, 5/2 − z; #4 2 − x, 1 − y, 2 − z; #5 −1/2 + x, 1 − y, 1/2 + z. |
Cd1–O2 |
2.242(3) |
Cd1–O5#1 |
2.242(4) |
Cd1–O5#2 |
2.132(3) |
Cd1–O2#3 |
2.242(3) |
Cd1–O3#4 |
2.368(3) |
Cd1–O3#5 |
2.368(3) |
Cd2–O1 |
2.219(4) |
Cd2–N2A |
2.31(3) |
Cd2–O6#1 |
2.218(5) |
Cd2–O3#5 |
2.296(3) |
Cd2–O4#5 |
2.517(4) |
O2#3−Cd1–O5#1 |
164.47(12) |
O3#4−Cd1#5 |
170.82(14) |
O2–Cd1–O5#2 |
164.47(12) |
O3#5−Cd2–N2A |
144.8(6) |
O1–Cd2–O6#1 |
94.17(15) |
O3#5−Cd2–O4#5 |
54.44(12) |
|
|
Dye adsorption
The adsorption isotherm of MO on compound 1 was measured in the dark by mixing 10 mg of compound 1 with 50.0 mL of MO aqueous solution at the initial concentrations (C0) from 15 to 300 ppm. The suspension was first sonicated for 5 min and then shaken at a constant rate overnight. After the suspension was filtered through a membrane filter (pore size, 0.45 μm), the filtrate was analyzed using a TU-1900 double-beam spectrophotometer to get the equilibrium concentration Ce. The amount of adsorption Qe, was calculated by dividing the decreased concentration of (C0 − Ce) by the amount of adsorbent used and expressed in mol g−1 of 1. The maximum adsorption capacity was calculated from the Langmuir adsorption isotherm.
Results and discussion
Description of crystal structure
As shown in Fig. 1a, there are two crystallographically independent CdII centers in the structure: the Cd1 atom at half occupancy, situated on an inversion center, adopts an octahedral coordination environment occupied by six carboxylate O atoms from six distinct TCA3− anions; the Cd2 center sites in a trigonal bipyramid sphere was defined by four O atoms from three distinct TCA3− anions and one N atom from a bimb ligand. In 1, the Cd–O bond lengths were in the range 2.218(5)–2.517(4) Å, and the Cd–N distances ranged from 2.219(4) to 2.31(3) Å. The TCA3− moiety can be considered as a propeller because its phenyl rings are tilted relative to each other with dihedral angles varying from 74.2 to 87.1°. Interestingly, six carboxylate groups bridge three CdII atoms, generating the centrosymmetric trinuclear cluster Cd3(CO2)6 as the secondary building unit (SBU) with nonbonding Cd1⋯Cd2 distance of 3.6362 Å (Fig. 1b) in complex 1. Apparently, each tricarboxytriphenyl amine (TCA3−) connects three Cd3(CO2)6 clusters to serve as a 3-connected node (Fig. S1a‡), whereas each Cd3(CO2)6 subunit in turn links another six Cd clusters and two TCA3− to act as 8-connected node, therefore, the individual framework of compound 1 can be rationalized as a binodal (3,8)-connected tfz-d net with Schlafli symbol (43)2(46·618·84) (Fig. 1c). The entire structure of 1 adopts three-dimensional (3D) porous architecture with two-fold interpenetrating belonging to class Ia.36 Micropore windows were observed with a size of 6.1 × 4.7 Å2 along the b axis in 1, considering van der Waals distances (Fig. 1d). The free accessible volume in the fully desolvated 1 is ca. 43.6% (1827 Å3) as determined by PLATON.
|
| Fig. 1 (a) Coordination environments of Cd(II) atoms with hydrogen atoms and disordered atoms for clarity of 1. (b) Trinuclear cluster [Cd3(CO2)6] SBU in 1. (c) Schematic representation of (3,8)-connected network for single framework of 1: blue, TCA3− ligand; grey-green, Cd1. (d) two-fold interpenetrated structure of 1 with microporous cavity. The symmetry codes refer to Table 2. | |
PXRD and thermal stability
A careful comparison of PXRD patterns of the as-synthesized and activated 1, as well as the simulated curve from the single-crystal data showed that the evacuated framework of 1 underwent no structural transformation after the activation (Fig. S2‡). The PXRD profiles of 1 also indicated that the framework maintained structural integrity after the recycling test for MO removal and immersion in different solvents. Compound 1 showed a weight loss of 23% below 290 °C, which can be attributed to the loss of guest DMA molecules (calcd 26%). The dehydrated phase remained stable up to 355 °C until the organic ligands were released (Fig. S3‡).
Gas adsorption
To evaluate the porosity of activated 1, gas sorption studies were conducted. The type-I H2 isotherms on the desolvated 1 were collected at 77 and 87 K, as shown in Fig. 2a. Obviously, both desorption isotherms exhibited significant hysteresis loops, indicating a small amount of mesoporosity that can be attributed to the intercrystalline voids.37,38 Complex 1 showed a maximum H2 uptake of 62.2 cm3 g−1 (0.55 wt%) at 77 K/1 bar and 32.8 cm3 g−1 (0.29 wt%) at 87 K/1 bar, respectively. Moreover, the isosteric heat (Qst) of H2 adsorption calculated by the virial method39 from the adsorption isotherms measured at 77 and 87 K was ca. 8.58 kJ mol−1 at zero loading, which is one of the highest values found in MOFs without open metal sites40,41 and significantly higher than those of well-known MOFs, such as NOTT-400 (5.96 kJ mol−1), NOTT-401 (6.65 kJ mol−1),42 SNU-6 (7.74 kJ mol−1),43 MOF-646 (7.8 kJ mol−1)44 and MOF-5 (7.6 kJ mol−1).45 Moreover, the value was obviously superior to that of the typical van der Waals type interactions.46 The Qst decreased slowly with increasing H2 loading and reached ∼5.12 kJ mol−1 at the maximum coverage. Apparently, this high Qst value can be attributed to its narrow pores after the double interpenetration, indicating a strong interaction between H2 molecules and the framework. In contrast, the evacuated 1 only showed an external surface N2 adsorption at 77 K. In this case, the preferential adsorption of H2 over N2 might be due to the size-exclusion effect, where the small windows limit the diffusion of larger N2 (3.64 Å) molecules into the pores, resulting in a lower adsorption over the diffusion time of the measurement, whereas smaller H2 molecules (2.9 Å) entered into the pores under the given conditions.
|
| Fig. 2 (a) H2 (77 K), H2 (87 K) and N2 (77 K) sorption isotherms for desolvated 1, where the filled and open shape represent the adsorption and desorption, respectively. (b) The isosteric heat of H2 adsorption (Qst) for desolvated 1. (c) Sorption isotherms for CO2, CH4, and N2 at 273 K of desolvated 1 (adsorption and desorption branches are shown with filled and empty shape, respectively). | |
Interestingly, the maximum CO2 uptake for desolvated 1 at 273 K/1 bar was 16.7 cm3 g−1 (Fig. 2c), whereas the corresponding CH4 and N2 uptakes were only 5.51 and 0.989 cm3 g−1, respectively, highlighting 1 as a promising material for highly selective separation of CO2/CH4 and CO2/N2 at room temperature. The separation ratios of CO2 vs. CH4 and N2 were calculated from the ratios of the initial slopes based on the single-component sorption isotherms (Fig. S5a‡).47 The calculated CO2/N2 and CO2/CH4 selectivities were 53:1 and 5.9:1 at 273 K, respectively. The values were superior to those of SYSU (CO2/N2: 25.5, CO2/CH4: 4.7),48 Cu6(BTTC)4(H2O)6·xS (CO2/N2: 31, CO2/CH4: 4.9)49 and [Cu2(obb)2(bpy)0.5(DMF)]·2DMF (CO2/N2: 30).50 The isosteric heat (Qst) of CO2 adsorption was calculated using the experimental isotherm data at 273 and 298 K (Fig. S5b and c‡). Compound 1 exhibited strong binding affinity for CO2 (35.6 kJ mol−1) at zero coverage (Fig. S5d‡), which is comparable to the superior values of MOFs containing amine functionality (35–41 kJ mol−1).51–54 The high initial Qst of CO2 can be mainly attributed to the strong interactions between Lewis basic amino sites along the small channels and acidic CO2 molecule. Moreover, the high quadrupole moment of (13.4 × 10−40 C m2) compared to those of N2 (4.7 × 10−40 C m2) and CH4 (nonpolar) could enhance specific interactions with the host framework, leading to the selectivity of CO2 vs. CH4 and N2.
Liquid-phase separation
The removal of dyes from wastewater is of paramount importance as many dyes are toxic and even carcinogenic.55,56 Because of its high efficiency and economic feasibility combined with simple operation, the removal of dyes by adsorption technology has becoming one of the competitive methods57 among many available physical, chemical and biological strategies.
Methyl orange (MO) and methylene blue (MB) (Scheme S2‡) represent well-known anionic and cationic dyes, respectively. To investigate the adsorption ability of compound 1 for hazardous dyes, 10 mg crystals of 1 were added to an aqueous solution of MO (20 ppm, 3 mL) at room temperature. After 20 minutes, the MO was removed from the aqueous solution with the yellow MO solution fading to colorless and the corresponding concentration decreased to 0.758 pm. In the case of MB, no apparent color change was observed after 20 minutes, and the MB concentration mostly remained unchanged (Fig. S6‡). The electrostatic interactions between the metal cation centers with a strong positive electric field effect and anionic MO in addition to the π–π interaction between the benzene rings of MOF and dyes may be responsible for the selective adsorption of MO over MB in water for compound 1.58
Interestingly, after the MO-loaded 1 was soaked in a fresh DMA for 20 minutes at room temperature, the recovery of adsorbent 1 was completed. Remarkably, the colorless DMA solution changed to yellow; meanwhile, the color of absorbent 1 almost shifted back to the original color (Fig. S7‡). Furthermore, a recyclability test with three consecutive runs was carried out for 1 to determine whether the adsorbent could be reused for subsequent removal of MO (Fig. S8‡). Specifically, the removal ability of 1 for MO did not decrease for all the three runs, indicating the applicability of MOFs in the adsorptive removal of anionic dyes from contaminated water.
As shown in Fig. 3, the MO adsorption isotherm of 1 follows the Langmuir equation Ce/Qe = Ce/Qmax + 1/(KQmax), where Qe is the amount of MO adsorption at Ce, the equilibrium concentration of MO in the bulk solution, Qmax is the maximum amount of adsorption, and K is the adsorption constant. Therefore, Qmax can be obtained from the reciprocal of the slope of a plot of Ce/Qe vs. Ce. The Qmax value was 748 mg g−1, higher than the adsorption capacity of MOF-235,59 NH3+-MCM-41,60 LDH61 and activated carbon,62 indicating the high efficient adsorption of 1 for MO. To the best of our knowledge, 1 has the second highest adsorption capacity among the MOFs reported to date (Table 3). Moreover, the Gibbs free energy change ΔG was calculated to be −21.02 KJ mol−1 using the following equation: ΔG = −RTlnK (where R is gas constant), which suggests spontaneous adsorption of MO over 1 under the experimental conditions.
|
| Fig. 3 (a) Adsorption isotherm for the adsorption of MO over 1. (b) Langmuir plot of the isotherm. | |
Table 3 Comparison of MO adsorption capacity in various MOFs
Adsorbents |
Adsorption capacity (mg g−1) |
References |
MOF-235 |
477.0 |
59 |
MIL-53(Cr) |
57.9 |
15 |
PED-MIL-101 |
194.0 |
15 |
MIL-100(Cr) |
211.8 |
17 |
MIL-100(Fe) |
1045.2 |
17 |
1 |
748 |
This work |
Luminescence sensing
The PL spectra of complex 1 and free ligand H3TCA in the solid state were recorded at room temperature. Complex 1 exhibited an intense emission peak at 470 nm upon excitation at 360 nm, which can be largely assigned to the ligand-centered luminescent process because a similar emission was observed at 453 nm for the free ligand H3TCA (Fig. S10‡). Interestingly, complex 1 showed strong guest-dependent luminescence properties: this MOF showed a purple emission at 423 nm in methanol, a significantly red-shifted indigo emission at 461 nm in H2O, and a further red-shifted cyan emission at 490 nm in ethanol, indicating that it is a promising luminescent probe for detecting small molecules through the shift of the PL spectra (Fig. 4). Moreover, the PL spectra did not shift when the same experiment was performed with only H3TCA (Fig. S11‡). This indicates that this discrimination can be attributed to complex 1. The shifts in the PL spectra can be ascribed to the formation of exciplexes (excited complexes) by the interactions between analytes and MOFs in the excited states,63,64 which is less investigated in MOFs.65
|
| Fig. 4 Emission spectra of compound 1 in MeOH, EtOH and H2O. Inset: color changes upon the addition of different solvents. | |
Conclusions
We successfully prepared a two-fold interpenetrating three-dimensional (3D) microporous MOF [Cd3(TCA)2(bimb)·(DMA)6]n (1) that showed remarkable adsorption enthalpies for CO2 and H2 gas molecules and exhibited good separation ratios of H2 over N2 at lower temperature. In particular, activated 1 was efficient for the selective sorption of CO2 over N2 and CH4 under ambient conditions. Interestingly, compound 1 exhibited highly selective and recyclable property in the removal of dyes MO from contaminated water. To the best of our knowledge, 1 has the second highest adsorption capacity for MO among the MOFs reported to date. Notably, complex 1 displayed strong guest-dependent luminescence behavior, indicating that it could be a promising luminescent probe for detecting small molecules.
Acknowledgements
This work was financially supported by the National Nature Science Foundation of China (No. 21171062 and 21371065), Self-Determined Research Funds of CCNU from the Colleges' Basic Research and Operation of MOE (CCNU15A05053).
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Footnotes |
† This paper is dedicated to Prof. Thomas C. W. Mak on the occasion of his 80th birthday. |
‡ Electronic supplementary information (ESI) available: X-ray crystallographic file (CIF), additional crystal figures, Qst calculation details, dye adsorption and separation, emission spectra, TGA data, PXRD patterns for complex 1. CCDC 1057133. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c5ra21980a |
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