Ignacio
Luz
,
Mustapha
Soukri
* and
Marty
Lail
RTI International, Post Office Box 12194, Research Triangle Park, NC 27709, USA. E-mail: msoukri@rti.org
First published on 11th April 2018
Solid-state synthesis ensures a high loading and well-dispersed growth of a large collection of metal–organic framework (MOF) nanostructures within a series of commercially available mesoporous silica. This approach provides a general, highly efficient, scalable, environmentally friendly, and inexpensive strategy for shaping MOFs into a fluidized form, thereby allowing their application in fluidized-bed reactors for diverse applications, such as CO2 capture from post-combustion flue gas. A collection of polyamine-impregnated MOF/SiO2 hybrid sorbents were evaluated for CO2 capture under simulated flue gas conditions in a packed-bed reactor. Hybrid sorbents containing a moderate loading of (Zn)ZIF-8 are the most promising sorbents in terms of CO2 adsorption capacity and long-term stability (up to 250 cycles in the presence of contaminants: SO2, NOx and H2S) and were successfully prepared at the kilogram scale. These hybrid sorbents demonstrated excellent fluidizability and performance under the relevant process conditions in a visual fluidized-bed reactor. Moreover, a biochemically inspired strategy for covalently linking polyamines to MOF/SiO2 through strong phosphine bonds has been first introduced in this work as a powerful and highly versatile post-synthesis modification for MOF chemistry, thus providing a novel alternative towards more stable CO2 solid sorbents.
In these solid composites, polyamines selectively adsorb CO2via chemisorption at primary and secondary amines. MOFs also have the capability to absorb CO2via physisorption, either at Lewis-acid open metal sites5 or via molecular size confinement even in the presence of H2O,6 which have both demonstrated excellent capacity and selectivity over N. However, CO2 physisorption is reduced or limited by temperature, which leaves polyamine-impregnated MOFs as the most suitable strategy involving MOFs to prepare solid sorbents for CO2 capture under flue gas conditions typically operating at temperatures 40 °C and greater, although some promising results have been recently reported.7
In the race for developing more energy-efficient and competitive processes involving amine-containing solid sorbents for CO2 capture from post-combustion flue gas streams, fluidized-bed reactors (FBRs) are proposed as a more energy-efficient CO2 capture technology than packed-bed configurations due to their improved heat and mass transfer.8 In this way, several polyamine-containing solid sorbents using mesoporous silica as fluidized supports have been successfully tested in an FBR at pilot plant scale.9 Nevertheless, the current fluidized solid sorbents show capacities below 10 wt% of CO2 capture and suffer long-term deactivation via leaching of the active adsorbent phase because of the weak interactions via hydrogen bonds between polyamines and the support.
To the best of our knowledge, MOF-based CO2 solid sorbents have never been studied in a fluidized-bed configuration because of the absence or limitation of some essential features required for operating under these conditions, such as fluidizability and attrition resistance. Therefore, it is quite important to develop a general strategy for shaping MOFs into a fluidized form, which may confer MOFs with the required physicochemical properties. Furthermore, additional synergistic features can originate from MOFs and support intimately combined at the nanoscale, such as hierarchical mesoporosity or microporosity, which may host and disperse more active polyamines while providing them with more long-term stability via either a coordination bond at open metal sites or a covalent bond at free functional groups.10
Our group has recently developed an elegant approach to selectively confine MOF nanocrystals within mesoporous materials via novel solid-state synthesis, which allows the preparation of hybrid materials containing a high loading (up to 40 wt%) of the smallest nanocrystals yet reported for any MOF structure within a wide collection of mesoporous supports, also named HyperMOFs.11 The resulting hybrid materials show improved features from the combination of a silica scaffold protecting and supporting the MOF nanocrystallites within its porous network. Some of these improved features include improved attrition resistance, excellent fluidizability and handling, as well as the enhanced catalytic activity recently reported by our group.12 This insight encouraged us to prepare a novel kind of “flying” MOF by using cheap, commercially available mesoporous silica as the fluidizable carrier for MOFs.
Herein, a collection of polyamine-impregnated MOF/SiO2 was tested for CO2 capture under simulated flue gas conditions in a packed-bed reactor (PBR) and compared with the state-of-the-art sorbents composed of polyamines on both “fluidized” silica and “non-fluidized” bulk MOFs. This systematic study reveals the correlations between the features of MOF/SiO2, such as loading, composition, and functionality of the confined MOFs, and the performance of impregnated polyamines for CO2 capture. To study their viability for a larger scale, the most promising materials have been evaluated for long-term stability in a PBR and a visual fluidized-bed reactor (vFBR). In addition, a cost evaluation study was conducted by our group to compare with those of state-of-the-art MOF-based solid sorbents. Furthermore, a novel strategy for covalently bonding polyamines to the fluidized MOF/SiO2 hybrid materials was introduced during this work to precisely tailor the new generation of HyperMOF hybrid materials for specific applications.
Complete descriptions of the PBR and vFBR, as well as the experimental procedures are included in the ESI† and in our previous work.18
Fig. 1 Solid-state synthesis of (Cr)MIL-101(SO3H)/SiO2 at varying MOF loadings: 5, 19 and 40 wt%. (a) Scheme of the fluidised MOF/SiO2 hybrid material showing the dispersion of MOF nanocrystals along mesoporous silica in the transmission electron microscopy image (white scale bar = 20 nm, extended study included in our previous work19). N2 sorption isotherms at 77 K (b) and CO2 sorption isotherms at 273 K (c) for (Cr)MIL-101(SO3H)/SiO2 at varying MOF loadings: 5 wt% (olive green, ■), 19 wt% (green, ▲), 40 wt% (dark blue, ♦) and 100 wt% (blue, ★). Closed symbols correspond to adsorption branches, whereas open symbols correspond to desorption branches. (inset in b) The pore size distribution was calculated from the Barrett–Joyner–Halenda (BJH) adsorption dV/dD plot (pore diameter [nm] at x-axis and pore volume [cm3 g−1 nm−1] at y-axis). |
Two configurations of polyamine-containing fluidized MOF hybrid sorbents were prepared by using (Cr)MIL-101(SO3H)/SiO2 hybrid materials: anchored and confined polyamines. The first approach consisted of treating the hybrid materials with linear, but not highly volatile, polyamines, such as tetraethylenepentamine (TEPA) and diethylenetriamine (DETA), in non-coordinating solvents (chloroform) to anchor them via both coordinative bonds through the open metal site at the chromium oxocluster and the ionic bond through the free sulfonic acid group at the ligand, as shown in Fig. 2. After washing with chloroform, the resulting composites exhibited a full degree of functionalization for both open metal sites and sulfonic groups, as suggested by the nitrogen to chromium ratios (N:Cr) of ca. 10 measured by using a combination of elemental analysis and XRF (see Tables S1 and S2 in the ESI†). TEPA approximately corresponds to one TEPA molecule coordinated to one chromium atom and another reacted with one sulfonic acid group (i.e. Cr3O[TEPA]3[BDC(SO3)−(TEPA)+]3). Attempts to coordinate TEPA on bulk (Cr)MIL-101(SO3H) under the same conditions resulted in a lower degree of functionalization (N:Cr = 2.8). This finding may be attributed to the constrained diffusion of TEPA molecules through the pore system of the bulk material, especially after the partial blockage of MOF pore apertures by TEPA molecules already anchored. Therefore, MOF nanocrystals dispersed on mesoporous silica exhibiting a 100-times smaller crystal size than their bulk counterparts allow for better polyamine diffusion and coordination along the MOF crystalline domain.
Next, 2 g of these composites were tested in a PBR under simulated flue gas conditions for 10 cycles to evaluate CO2 adsorption capacity and stability. As shown in Fig. 2, TEPA coordinated on both 19 and 40 wt% MOF/SiO2 exhibited better performance and amine use for CO2 capture compared with pure bulk MOFs. 43% of amine utilization was calculated for 19 wt%, 26%, and for 40 wt% and only 14% for bulk MOFs under these experimental conditions, that is, considering that four of the TEPA molecules may coordinate to CO2 while one is coordinated to the MOF (Table S2 in the ESI†). Lower CO2 adsorption capacity was measured for materials fully functionalized by shorter polyamines because of their lower number of amines per molecule, such as DETA or ethylenediamine (Table S2 in the ESI†). This evidence shows the beneficial effects of having a moderate concentration of well-dispersed MOF nanocrystals anchoring polyamines to enhance the accessibility and efficiency of the amine adsorption sites under simulated flue gas conditions.
However, the second approach via confinement within the pores leads to a higher loading of active polyamines, and thereby higher CO2 capacities because the hierarchical mesoporosity and microporosity of the MOF/SiO2 hybrid materials can be impregnated with up to 35 wt% of branched polyamines (PEI, Mw = approximately 800) without revealing signs of stickiness, which would avoid their application in fluidized beds.18 The infiltration of PEI on MOF/SiO2 microporosity and mesoporosity, as compared in Fig. 2b for 19 wt% of (Cr)MIL-101(SO3H)/SiO2 containing anchored TEPA (occupying microporosity) and confined 35 wt% of PEI (occupying both microporosity and mesoporosity), has been confirmed by using N2 sorption isotherms. Thus, CO2 adsorption capacity of confined PEI is also highly dependent on the MOF loading because the presence of 19 and 40 wt% of MOF within the mesoporous silica reduces the CO2 adsorption capacity of the amines compared with that of bare silica. This inhibition phenomena may be attributed to the interaction of PEI amines with both open metal sites and free functional groups at the confined MOF and the defective sites located at the MOF boundary inherent to the nanocrystalline domains. Therefore, the CO2 adsorption capacity drops proportionally with the MOF loading because a lower capacity was found for 40 wt% MOF loading. Surprisingly, PEI infiltrated on a HyperMOF containing only 5 wt% of MOF leads to a slight enhancement (ca. 10 wt%) of the CO2 adsorption capacity (Fig. 2c). However, additional experiments confining 35 wt% of TEPA on MOF/SiO2 materials revealed a high deactivation because of the leaching of non-coordinated TEPA molecules during the regeneration step at 120 °C in the presence of wet nitrogen. This finding was also observed for 35 wt% of TEPA impregnated on the same bulk MOF and as described later in this manuscript for other impregnated short polyamines (see Fig. 3 and Table 1). Therefore, the use of TEPA as a polyamine was discarded for this application. Branched PEI was found to be more stable for fluidized MOF hybrid sorbents under simulated flue gas conditions.
Fig. 3 CO2 capture of polyamines impregnated on bulk MOFs compared with MOF/SiO2 under simulated flue gas conditions in a PBR. |
Entry | MOF | CO2b (wt%) | Deactivationc (%) | MOFd (wt%) |
---|---|---|---|---|
a In all cases, 2 g of the solid sorbent were loaded into a PBR blended with SiC4 particles as inert with good thermo-conductivity, and 35 wt% TEPA was used for bulk MOFs instead of PEI. b CO2 adsorption capacity at the second cycle measured in a PBR under simulated flue gas conditions. c 10 cycle CO2 adsorption deactivation. d MOF loading calculated by using XRF. e Sorbent was measured under dry conditions. f 32 wt% mmen was used instead of PEI. g No polyamine was used. | ||||
1 | — | 9.0 | 2.7 | 0.0 |
2 | (Cr)MIL-101(SO3H) | 10.0 | 6.1 | 4.9 |
3 | (Cr)MIL-101(SO3H) | 8.3 | 8.3 | 19.1 |
4 | (Cr)MIL-101(SO3H) | 7.1 | 17.7 | 40.0 |
5 | (Cr)MIL-101(SO3H) | 8.8 | 26.1 | 100.0 |
6 | (Cr)MIL-101(SO3H)e | 5.1 | 0.1 | 100.0 |
7 | (Zr)UiO-66(NH2) | 12.0 | 2.6 | 1.5 |
8 | (Zr)UiO-66(NH2) | 12.5 | 3.3 | 4.2 |
9 | (Zr)UiO-66(NH2) | 10.6 | 3.4 | 6.8 |
10 | (Zr)UiO-66(NH2) | 6.8 | 5.9 | 37.6 |
11 | (Zr)UiO-66(NH2) | 4.6 | 9.5 | 100.0 |
12 | (Zn)ZIF-8 | 12.6 | 1.5 | 4.6 |
13 | (Zn)ZIF-8 | 12.5 | 3.1 | 7.8 |
14 | (Zn)ZIF-8 | 10.1 | 6.5 | 35.1 |
15 | (Zn)ZIF-8 | 9.5 | 15.7 | 100.0 |
16 | (Zn)ZIF-8e | 8.2 | 0.9 | 100.0 |
17 | (Zn)ZIF-7 | 12.0 | 1.2 | 4.9 |
18 | Mg2(dobpdc)f | 6.2 | 12.4 | 100.0 |
19 | Mg2(dobpdc)e,f | 13.5 | 0.2 | 100.0 |
20 | NbOFFIVE-1-Nig | 6.2 | 1.1 | 100.0 |
21 | NbOFFIVE-1-Nie,g | 8.6 | 2.4 | 100.0 |
22 | (Co)ZIF-67 | 12.7 | 18.8 | 5.2 |
23 | (Al)MIL-53(NH2) | 12.2 | 7.6 | 3.9 |
24 | (Cr)MIL100 | 10.4 | 4.6 | 5.6 |
25 | (Fe)MIL-100 | 12.6 | 24.9 | 5.3 |
26 | (Zr)PCN-222 | 11.4 | 1.4 | 3.5 |
27 | (Zr)UiO-66 | 11.9 | 4.9 | 4.7 |
28 | (Zr)NU-1000 | 11.2 | 7.9 | 4.2 |
As shown in Table 1, a similar tendency was observed for 35 wt% of PEI impregnated on HyperMOF hybrid materials at various loadings compared with the results presented in Fig. 2c. In all of the cases, a boost in the CO2 adsorption capacity was found for ca. 5 wt% of MOF loading compared with just PEI impregnated on pure silica, whereas lower CO2 adsorption capacity and higher deactivation were measured for higher MOF loadings. Therefore, the initial CO2 sorption capacity of PEI amines is improved by the presence of MOF nanocrystals, but at moderate loadings, because a concomitant inhibition mechanism is significantly affecting the adsorption performance for excessive presence of MOFs. The irreversible inhibition pathways may be one or a combination of three scenarios. The first scenario involves neutralization of the PEI amines by defective ligands and/or coordinatively unsaturated metal sites. The second scenario involves oxidation of the PEI amines by MOF metal components at the nodes at high temperatures. The last scenario involves hindrance or aggregation of the PEI amines because of confinement within microporous cavities.
By comparing the results obtained for (Zn)ZIF-8 (entries 12 through 16) or (Zn)ZIF-7 (entry 17), which consists of imidazolate-type ligands, with those of the remainder of the carboxylate-type MOFs, such as (Cr)MIL-101(SO3H) (entries 2 through 5) or (Zr)UiO-66(NH2) (entries 7 through 11), the initial CO2 adsorption capacity and the deactivation rate are less affected by the MOF loading. Thus, boundary crystal defects in the MOF nanocrystals containing carboxylate-type ligands may neutralize more numbers of PEI amines than MOFs consisting of N-type ligands. Therefore, better long-term stability was observed for (Zn)ZIFs compared with that of carboxylate-containing MOFs that exhibit higher deactivation in all cases. However, materials containing Co (entry 22) or Fe (entry 25) at the metal nodes show the highest deactivation rates compared with their isostructural counterpart containing Zn (entry 12) or Cr (entry 24) for the same MOF loadings, respectively. This finding can be attributed to the superior activity of these metals for catalytic amine oxidation.
In the same way, deactivation was observed for bulk (Zn)ZIF-8 (entries 15 and 16) and (Cr)MIL-101(SO3H) (entries 5 and 6) in the presence of H2O, although CO2 adsorption capacity is quite similar under both “wet” and dry conditions for (Zn)ZIF-8, but is lower for dry (Cr)MIL-101(SO3H) compared with “wet” conditions. In the same way, very low deactivation (i.e. <1%) was measured for all polyamine-containing bulk MOFs under dry conditions. Moreover, an FTIR analysis of fresh and used TEPA impregnated in (Cr)MIL-101(SO3H) and (Zn)ZIF-8 revealed some differences that may be attributed to the degradation of MOF structures in the presence of polyamines promoted by either O2, H2O, and temperature or a combination of them (Fig. S6 in the ESI†). In the same way, similar stability issues under simulated flue gas conditions were reported in the literature20 for TEPA-impregnated bulk MOFs and were criticized by researchers21 for bulk MOFs adsorbing CO2 by physisorption, such as (Mg)MOF-74 and SIFSIX-3-Cu, which show a drastic drop in CO2 adsorption capacity in a few cycles compared with highly stable copper silicalite. Nevertheless, NbOFFIVE-1-Ni overcame these observed stability issues because of its hydrophobicity (entries 20 and 21), although the CO2 adsorption capacity was lower and reversibly dropped by 28% in the presence of 5.6 v/v% of H2O (Fig. S8 in the ESI†).
Another hypothetical reason for this inherent drop in CO2 adsorption capacity could be caused by the loose polyamine dispersion and subsequent mutual aggregation that leads to an auto-inhibiting effect of the amine sorption sites. This effect was observed for our hybrid materials containing more than 40 wt% of PEI and for PEI confined on pure mesoporous silicas exhibiting both smaller and larger pore sizes (e.g. 9.5 nm in SBA-15 or 42 nm in silica[D], respectively, see Fig. S9 in the ESI†) than mesoporous silica(A). In comparison, silica(A) exhibited a optimal polyamine dispersion and was also enhanced by the presence of MOF nanocrystals. In addition, this effect may also be attributed to a hygroscopic inhibition that leads to a reduction of the CO2 adsorption capacity because of the accumulation of H2O around the highly hydroscopic polyamine-impregnated solids. Therefore, these major limitations for the direct application of polyamine-containing bulk MOFs under simulated flue conditions are efficiently overcome by using a moderate concentration of MOF nanocrystals dispersed within mesoporous silica. Doing so will raise the adsorption efficiency of the impregnated amines while avoiding the inhibition caused by polyamine aggregation and hydroscopic hindrance, which further encourage the use of our MOF/SiO2 hybrid solid sorbents for this application.
To provide insight into the influence the presence of MOF nanocrystals has on the CO2 dynamics of impregnated PEI, the adsorption–desorption profiles for 35 wt% of PEI confined on 4.6 wt% of (Zn)ZIF-8/SiO2 and bare SiO2 at the tenth cycle are compared in Fig. 5. The adsorption breakthrough profile for the MOF-containing solid sorbent shows a superior CO2 adsorption to PEI/SiO2, as shown in Table 1. The characteristic adsorption–regeneration profiles for the PBR filled with inert SiC4 are represented by the red line, which determines the dead volume of the PBR. However, the regeneration profile shows an interesting difference in terms of CO2 desorption for the composite incorporating MOF nanocrystals. Larger concentrations of the early released adsorbate are measured for the MOF/SiO2 hybrid sorbent, which is attributed to weakly adsorbed CO2via physisorption because the temperature required to release them is lower than 80 °C.
Fig. 5 (Top panel) Adsorption and (Bottom panel) regeneration profiles of 35 wt% of PEI/4.6 wt% of (Zn)ZIF-8/SiO2 (entry 12, Table 1) and 35 wt% of PEI/SiO2 (entry 1, Table 1). |
PEI/SiO2 also exhibited an early release, but it is mainly attributed to CO2 trapped in the dead volume of the PBR, as suggested by comparison with the profile for the inert SiC4. In addition, PEI/MOF/SiO2 exhibited higher CO2 desorption between 80 and 100 °C, which suggests the slightly better use of the PEI amines for CO2 chemisorption as well. This result highlights the unusual dual adsorption performance of our hybrid sorbents containing MOF nanocrystals compared with their pure silica counterpart.
Flue gas from coal-fired power plants typically contains other acid-gas impurities, such as SO2 and NOx, that can dramatically influence the CO2 capture efficiency.23,24 Therefore, during this current work, the performance of our MOF-based sorbents in the presence of these contaminants was evaluated. The results show a clear deactivation of the CO2 adsorption capacity of the sorbents in the presence of SO2. This deactivation is because of the irreversible reaction occurring during the adsorption step between SO2 and PEI amines, which are not further active for the CO2 capture (Fig. 6).
Amine deactivation was proportional to the SO2 concentration, as shown by the S content determined by CHNS elemental analysis after 100 cycles (see Table S4 in the ESI†). Also, FTIR spectra of these samples measured after 100 cycles revealed the clear, irreversible binding of SO2 to the hybrid sorbent (Fig. S7 in the ESI†). However, excellent stability at higher NOx concentrations was observed. Therefore, MOF nanocrystals within the hybrid solid sorbent did not reduce the tendency of PEI amines to be deactivated by irreversible binding with SO2, as a similar deactivation for PEI/SiO2 was observed by our group.18 Therefore, another unit should be added upstream for scrubbing the SO2 levels in the flue gas down to a single-digit parts per million level before reaching the FBR to elongate the life of the hybrid solid sorbents and reduce the make-up rate. Good stability was measured in the presence of H2S, typically found in sour gas streams, although an initial drop in capacity was observed because the study was performed under dry conditions and without O2 because H2 was in the H2S cylinder.
During this study, the PEI/SiO2 sorbent and the most promising PEI/MOF/SiO2 sorbent (i.e. 4.6 wt% of [Zn]ZIF-8/SiO2) were exposed to a series of testing conditions to evaluate their fluidizability. First, the sorbents were subjected to an adsorption–regeneration cycle to determine their CO2 adsorption breakthrough curves. Fig. 7b shows the CO2 breakthrough curve for both sorbents during the adsorption step compared with that of bare SiO2, which allows the dead volume of the system to be determined.
The breakthrough for the bare SiO2 occurred after approximately 30 s, whereas the use of 50 g of the solid sorbent containing PEI resulted in a significantly larger lag-time in breakthrough (ca. 6 to 7 min), suggesting that both sorbents are capable of deep CO2 scrubbing, close to 100% efficiency, before saturation. As observed in the results obtained in the PBR (Table 1), the sorbent containing MOF nanocrystals also exhibited higher adsorption capacity than PEI/SiO2 in the vFBR.
Afterwards, both sorbents were exposed to a stream containing 80 v/v% of H2O balanced with N2 at 100 °C for 1 h. These very aggressive conditions in the regeneration step were used because the stability under these conditions is crucial for further application, as the CO2 adsorption capacity of the sorbent could significantly drop because of the amine leaching under steam stripping. It is important to note that the extremely long exposure time of 1 h used for this experiment does not represent the actual residence times of the fluidized sorbent in the regenerator, which is typically 2 to 5 min. Fig. 7c is a photograph of the sorbent bed during the initial CO2 loading test and after exposure to steam stripping for 1 h. Surprisingly, PEI/SiO2 showed a more severe amine leaching in comparison with the material containing MOF nanocrystals under these conditions. Moreover, the PEI/SiO2 sorbent became yellow and wet and stuck to the internal reactor wall, completely losing its fluidizability. In contrast, the MOF-containing sorbent appeared to be more resilient to the steam stripping because the material maintained its fluidizability over 1 h of testing. These results are consistent with the breakthrough adsorption curves measured for these two sorbents after the steam exposure.
After a drying treatment with 1 SLPM of N2 at 100 °C for 2 h, CO2 adsorption capacity was practically maintained for PEI/MOF/SiO2, whereas a significant drop was observed for the MOF-free sorbent (see Fig. 7b). This improved steam stability of the sorbents containing ZIF-8 nanocrystals can be attributed to the well-known hydrophobicity of the MOFs, which can be enhanced further by using longer aliphatic substituents of the imidazole ring.26 Currently, the influence on the CO2 capture performance of other substituents at the imidazole ring of PEI/MOF/SiO2 sorbents is under investigation by our group.
Finally, the pressure drops across the FBR reactor bed for all the materials was also examined by varying the N2 flow from 0.5 to 4.8 L min−1 (SLPM). The sorbent containing MOF nanocrystals exhibited a slightly higher pressure drop than PEI/SiO2, which can be attributed to the higher density because of the presence of the MOF (0.75 kg m−3 for PEI/MOF/SiO2versus 0.68 kg m−3 for PEI/SiO2). The main benefits of using denser fluidized sorbents are the reduction of the column size, the increment of the gas velocity and the lower sorbent carried over by flue gas. Nevertheless, an excessive pressure drop in the system can lead to a higher energy requirement to drive the fluidized sorbent through the bed. Fortunately, the sorbents containing moderate MOF loadings demonstrate an equilibrated combination of opposite features in terms of fluidizability when operating at the optimal gas velocity range (0.1–0.2 m s−1 (ref. 27)) (i.e. denser particles, but not involving drastic pressure drops).
The price determined in our group for the kilogram-scale preparation of these sorbents is approximately $20 per kg according to the cost evaluation study we recently conducted (Fig. S11 in the ESI†). This cost can be reduced to $15 per kg by implementing some cost-saving measures such as recycling solvents and finding alternative mesoporous silica and PEI vendors. That reduced cost is in the same range as the production cost for some limited bulk MOFs via liquid assisted grinding (LAG), as recently reported in the literature.28
During the past decade, a wide collection of strategies for post-synthesis modification have been developed for MOFs containing free functional groups at the organic ligand, especially for amino functionality at the aminoterephthalate ligand.24 However, to the best of our knowledge, an efficient, one-pot, environmentally friendly and general approach for covalently bridging amine to amine is still missing in MOF chemistry. However, the use of THP as a coupling reagent for the immobilization of enzymes onto chitosan films via Mannich-type condensation resulted in greater enzyme performance than many conventional coupling routes involving glutaraldehyde.23,29 Hence, we applied this efficient approach of creating strong covalent bonds amine-to-amine via a methylene phosphine bridge or bridges (N–P–N) to link PEI to (Zr)UiO-66(NH2) nanocrystals while keeping all of the resulting amines still active for CO2 adsorption. This approach is in contrast to conventional glutaraldehyde that forms weak imine bonds, which do not exhibit CO2 chemisorption (see Fig. 8).
An optimal phosphine grafting (99% by XRF) was achieved via gas-phase phosphine functionalization and the material retained most of the PEI impregnated (95% by elemental analysis) after thoroughly washing the material with methanol after 10 cycles, as shown in Fig. 8. This approach provides a powerful synthetic tool to bind amine-containing organic or organometallic compounds to amine-containing MOFs or other solid supports, preserving their activity to be subsequently used for a variety of applications. The applications range from gas adsorption or separation to heterogeneous catalysis to bioimaging or drug delivery.
Long-term stability tests in the presence of contaminants and experiments on a visual FBR showed their excellent stability, fluidizability, and outstanding performance under steam regeneration because of the hydrophobicity conferred by the presence of MOF nanocrystals.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c7sc05372j |
This journal is © The Royal Society of Chemistry 2018 |