Liming Taoa,
Fang Niub,
Di Zhanga,
Jingang Liuc,
Tingmei Wanga and
Qihua Wang*a
aState Key Laboratory of Solid Lubrication, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou, Gansu 730000, P. R. China. E-mail: qhwang@licp.cas.cn; Fax: +86 0931 4968252; Tel: +86 0931 4968252
bCollege of Chemistry and Chemical Engineering, Lanzhou University, Lanzhou, Gansu 730000, P. R. China. E-mail: niufang@lzu.edu.cn
cLaboratory of Advanced Polymer Materials, Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100866, P. R. China. E-mail: liujg@iccas.ac.cn
First published on 5th November 2015
A series of azo-bridged, aromatic, nitrogen-rich, microporous covalent porphyrinic polymers (Azo-CPPs) were synthesized through a metal catalyst-free direct coupling of a kind of tetranitro building block, 4NO2TPP, and several diamine or tetraamine compounds, under basic conditions. The Azo-CPPs were all amorphous and exhibited surface areas between 197 to 591 m2 g−1. The effect of building blocks on the pore properties was discussed. Meanwhile, the capacity of adsorption of CO2 for all the Azo-CPPs was studied and the CO2 uptake capacity was between 7.36% and 9.22% at 273 K and 1.10 bar. The CO2/N2 selectivities were measured between 27.4–53.9 at 273 K and 31.2–107.8 at 303 K, respectively, showing an increase in selectivity with increasing temperature.
Herein, we report a series of azo-bridged covalent porphyrinic polymers (Azo-CPPs) by using the metal catalyst-free direct coupling of nitro and amino groups under basic conditions. We utilized a porphyrin derivative with four nitro groups, 5,10,15,20-tetrakis(4′-nitrophenyl)porphyrin (4NO2TPP), and several aromatic diamines or tetraamines with different length, steric hindrance, and rigidity as the building blocks to synthesize Azo-CPPs with moderate to high surface areas. We expect that the lone pair electrons of nitrogen atoms from the azo segments can enhance the binding affinity between the Azo-CPPs and CO2. The synthesis and properties of the Azo-CPPs, the effect of diamines' structures on the surface areas, pore volumes and distribution, the CO2 adsorption ability and selectivity had been studied in detail.
All of the Azo-CPPs were synthesized in the same procedure in Schlenk tube, according to the literature.33 Azo-CPP-1 was given as an example. 4NO2TPP (238.4 mg, 0.3 mmol), p-PDA (64.9 mg, 0.6 mmol), and KOH (168.3 mg, 3.0 mmol) were placed in a dry 25 mL Schlenk tube. The solids were dissolved in anhydrous DMF (15 mL). The content was degassed by the freeze–thaw method and backfilled with Ar gas three times before closing the tube. Then the tube was placed in oil bath at 150 °C and stirred for 24 hours, during which the purple Azo-CPP-1 precipitated from solution. The solid product was then collected by filtration and washed repeat with water, DMF, acetone, THF, and methanol, respectively. Then it was extracted by acetone, chloroform, and methanol in Soxhlet extractor for 24 hours respectively, in order to remove the residual monomers and/or low-molecular weight by-products. The powder was dried in a vacuum oven for 24 hours to afford the final Azo-CPP-1 (144 mg, yield: 55%). The other Azo-CPPs were synthesized similarly with final yields about 50%.
The degree of polymerization was determined by comparing the FTIR spectra of the polymers and respective monomers. Representative FTIR spectra of a polymer (Azo-CPP-1) and its corresponding monomers were shown in Fig. 1a and b. The formation of azo (–NN–) linkages was confirmed by the stretching bands at 1469 and 1398 cm−1, of which the intensity was obviously enhanced.45 The same bands can be also observed in other Azo-CPPs clearly (Fig. S4 to S6 in the ESI†). At the same time, the bands at about 3300–3400 cm−1 can be attributed to the residual amino groups. The asymmetric and symmetric stretching band of unreacted and/or terminal nitro groups at 1520 and 1350 cm−1 can still be observed, but their intensity attenuated obviously compared with 4NO2TPP. The chemical shifts in the solid-state 13C NMR spectra of Azo-CPP-1 (Fig. 1c) located at 150.4, 143.0, 130.1, and 117.4 ppm confirmed the formation of the azo-linked aromatic polymers.43–45 At the same time, the peak at 138.9 ppm in p-PDA almost disappeared totally in Azo-CPP-1, also indicating the high reaction extent.
The Azo-CPPs were also characterized by thermogravimetric analysis (TGA) and powder X-ray diffraction (PXRD). To investigate the thermal stability of Azo-CPPs, TGA was performed up to 800 °C with a heating rate of 10 °C min−1 under nitrogen atmosphere. As shown in Fig. S7 in the ESI,† all Azo-CPPs exhibited remarkable thermal stability up to 300 °C in N2. Therefore, they had similar thermal stability compared with the networks obtained by C. T. Yavuz.43 All the TGA curves showed two weight losses. The first weight loss between 300 and 400 °C can be attributed to the decomposition of low molecular weight residual impurities and the other weight loss after 450 °C meant the degradation of organic frameworks. All Azo-CPPs showed high char yields higher than 60%. Due to the nature of their rigid structures, there was no observable glass transition temperature within the range of 30–500 °C (Fig. S8 in the ESI†), just like most of reported Azo-CPPs. The PXRD patterns indicated no long-range structure for any of the Azo-CPPs. All the Azo-CPPs were amorphous with broad diffraction peaks at about 2θ = 20°, corresponding to an average distance of 4.4 Å showing a partial stacking of aromatic units, which were in well accordance with the results obtained by C. T. Yavuz and H. M. El-Kaderi,33,43,44 respectively. The PXRD results did not show the characterized eclipsed or staggered structures like the reported covalent organic frameworks (COFs) which derived from 4NH2TPP,50–52 indicating that the reaction between 4NO2TPP and diamines in the presence of excess KOH was irreversible. Therefore, the polymerization had not extended the coplanar structure in the 2-D directions to form regular layered structures. Factually, the Azo-CPPs extended in 3-D directions irregularly (Scheme 1) and an amorphous structure was obtained. The morphology was characterized by HR-TEM as shown in Fig. 1e and f, in which the alternating areas of light and dark contrast revealed their disordered porous structural natures. The SEM images of Azo-CPP-1 were shown in Fig. S9 in the ESI.† The obtained particles were aggregated together to form larger particles in size of several micrometers.
Polymer code | Amine | SABETa [m2 g−1] | SALangb [m2 g−1] | SAmicroc [m2 g−1] | V0.1d [m3 g−1] | Vtote [m3 g−1] | V0.1/Vtot |
---|---|---|---|---|---|---|---|
a BET surface area calculated over the pressure range 0–0.15 P/P0 at 77.3 K.b Langmuir specific surface area calculated from the nitrogen adsorption isotherm by application of the Langmuir equation.c Micropore surface area calculated from the nitrogen adsorption isotherm using the t-plot method.d V0.1, pore volume at P/P0 = 0.1 at 77.3 K.e Vtot, total pore volume calculated at P/P0 = 0.99 at 77.3 K.f Pd–4NO2TPP was used. | |||||||
Azo-CPP-1 | p-PDA | 591 | 798 | 293 | 0.2438 | 0.5617 | 0.434 |
Azo-CPP-2 | m-PDA | 439 | 592 | 213 | 0.1793 | 0.3147 | 0.570 |
Azo-CPP-3 | DABP | 514 | 692 | 271 | 0.2127 | 0.3951 | 0.538 |
Azo-CPP-4 | TFDB | 518 | 696 | 274 | 0.2147 | 0.3803 | 0.565 |
Azo-CPP-5 | ODA | 563 | 759 | 274 | 0.2310 | 0.3925 | 0.589 |
Azo-CPP-6 | DAAzo | 433 | 588 | 164 | 0.1720 | 0.2980 | 0.577 |
Azo-CPP-7 | 4NH2TPP | 197 | 265 | 118 | 0.0824 | 0.1338 | 0.616 |
Azo-CPP-1–Pdf | p-PDA | 432 | 623 | 216 | 0.2285 | 0.4802 | 0.476 |
The effect of the average monomer strut length on the physical properties of Azo-CPPs, such as BET surface area, Langmuir surface area, micropore surface area, and micropore volume, had been studied in detail. We chose seven kind of aromatic amine monomers as the building blocks to investigate the effect of building blocks on the final porosity properties and gas uptake capacities of the Azo-CPPs, as shown in Scheme 1. As the length of linker increased gradually in the order of p-PDA < DABP < DAAzo < 4NH2TPP, the BET surface areas decreased gradually in the order of Azo-CPP-1 > Azo-CPP-3 > Azo-CPP-6 > Azo-CPP-7, under otherwise same conditions. For example, when the linker changed from p-PDA to DABP, the BET surface area shows a loss of 13% (from 591 to 514 m2 g−1). The Langmuir specific surface areas, the micropore surface areas (t-plot method), and even the pore volumes (both V0.1 and Vtot) showed the same tendency. This phenomenon was in well accordance to the ‘strut length’ effects as investigated by A. I. Cooper and coworkers in their study on CMPs.53
To investigate the effect of steric hindrance on the surface areas, we introduce the bulky trifluoromethyl groups into the strut linker (the meta-position to the aminos, Azo-CPP-3 and Azo-CPP-4). Obviously different from a recently reported result,43 it can be seen that the introduction of –CF3 groups had a negligible effect on the surface areas (Azo-CPP-3, SABET = 514 m2 g−1; Azo-CPP-4, SABET = 518 m2 g−1). These phenomena can be attributed to the relatively far distance between the bulky substitute groups (in the meta-position) and the reactive aminos. In the reported results, the methyl substitutes were all in the ortho-position of aminos, which showed relatively greater steric hindrance effect when the amino were attacked in the polymerization. However, in the present study, the bulky –CF3 substitutes were relatively far from the –NN– groups; therefore the force between them were too small to cause a tilted geometry with respect to the aromatic phenyls.
We also investigated the effect of non-linear connectivity on the surface areas by using m-PDA as a linker (Azo-CPP-1 and Azo-CPP-2). When turned p-PDA to m-PDA, the surface area was reduced in expect (decreased from 591 to 439 m2 g−1). Surprisingly, the reduction in the surface area was as high as 25.7%, which was obviously higher than the results obtained by C. T. Yavuz et al. (7%).43
To assess the effect of flexible bridges between biphenyl linkers, Azo-CPP-3 and Azo-CPP-5 were checked. When compared to Azo-CPP-3 with rigid biphenyl units (SABET = 514 m2 g−1), Azo-CPP-5 with flexible ether links showed even higher surface areas (SABET = 563 m2 g−1). This result was rather contrary to the common belief that flexible linkers yield considerable losses in overall porosity, but in well accordance to the reported results. As explained by C. T. Yavuz,43 there were two competitive acts. Although the flexible ether links brought free rotation and consequent contraction in the construction of porous structure, it also eliminated the restriction on the in-plane alignment of biphenylic azo units. As a result, the more conjugated, semi-rigid oxygen bridge showed an enhanced surface area, compared with the biphenyl bridge.
Once the porosity of Azo-CPPs had been established, we considered their applications in gas storage. There are two kinds of CO2-philic groups in the Azo-CPPs obtained herein, e.g., the porphyrin rings which contain pyrrole segments (secondary amine, similar to that of benzimidazole) and the azo groups, either newly generated or originally existed (for Azo-CPP-6). Therefore, it can be predicted that the Azo-CPPs would have high CO2 adsorption ability. In general, with increasing specific surface areas and micropore volumes, the adsorption capacity for CO2 increases. We tested the CO2 adsorption properties at 273 K and a pressure up to 1.10 bar and the data are summarized in Table 2, from which we can see that all Azo-CPPs showed moderate capacity of CO2 adsorption, which was not so consistent with our original expecting. The CO2 adsorption for all Azo-CPPs ranged from 7.36% to 9.22% (Fig. S12 in the ESI†), which were higher than or comparable to those of some reported microporous polymers, for example, some nitrogen containing furan-based porous organic frameworks (FOF-1, 7.70%, 273 K).54 However, they were much lower than those of highly porous benzimidazole-linked polymer BILP-1 (SABET = 1172 m2 g−1, 18.8%, 273 K),55 ALP-1 (SABET = 1235 m2 g−1, 23.6%, 273 K),44 microporous polycarbazole (SABET = 2220 m2 g−1, 21.2%, 273 K),56 Azo-COP-2 (SABET = 729 m2 g−1, 11.2%, 273 K).43 When compared with the abovementioned excellent results, the present Azo-CPPs did not show any advantage in CO2 adsorption, maybe mainly due to their relatively lower surface areas. For example, the BET surface area of Azo-CPP-1 is only 591 m2 g−1, much lower than that of microporous polycarbazole (SABET = 2220 m2 g−1, 21.2%, 273 K). However, it was worth to note that Azo-CPP-7 showed relatively high CO2 adsorption of 7.49%, although the surface area of Azo-CPP-7 (SABET = 197 m2 g−1) was only one third of Azo-CPP-1 (SABET = 591 m2 g−1, 9.19%, 273 K). Otherwise, we used Pd in the inner core to see the CO2 capture abilities compared to materials with free base porphyrins. Azo-CPP-1–Pd was prepared in a similar procedure. We found the BET surface area was a little smaller than that of Azo-CPP-1 (432 vs. 591 m2 g−1) (Fig. S13 to S15 in the ESI†). The CO2 capture for Azo-CPP-1–Pd was almost in the same level as Azo-CPP-1 (9.17 wt% vs. 9.19 wt% at 273 K and 1.10 bar), although the surface area was relatively smaller.
Polymer code | CO2 adsorption (wt%) | N2 adsorption (wt%) | CO2/N2b | |||
---|---|---|---|---|---|---|
273a K | 303 K | 273 K | 303 K | 273 K | 303 K | |
a CO2 absorbance of Azo-CPPs at 273 K and 1.10 bar.b Selectivity estimated using the ratios of the Henry law constant calculated from the initial slopes of the single-component gas adsorption isotherms at low pressure coverage (<0.15 bar). | ||||||
Azo-CPP-1 | 9.19 | 4.80 | 0.61 | 0.07 | 53.9 | 82.0 |
Azo-CPP-2 | 9.11 | 5.54 | 0.82 | 0.30 | 27.4 | 31.2 |
Azo-CPP-3 | 9.22 | 3.99 | 0.54 | 0.10 | 45.3 | 66.5 |
Azo-CPP-4 | 8.52 | 5.12 | 0.41 | 0.05 | 40.6 | 107.8 |
Azo-CPP-5 | 8.52 | 5.08 | 0.60 | 0.09 | 37.9 | 78.6 |
Azo-CPP-6 | 7.36 | 4.02 | 0.36 | 0.07 | 47.2 | 72.2 |
Azo-CPP-7 | 7.49 | 4.17 | 0.52 | 0.16 | 34.3 | 45.3 |
In order to investigate the gas adsorption selectivity of the Azo-CPPs, CO2 and N2 sorption properties were measured by volumetric methods at the same conditions of 273 K, and the selectivity was estimated according to a reported method.33 The ratios of the Henry law constants, which were calculated from the initial slopes of the single-component gas adsorption isotherms at low pressure coverage (0–0.15 bar), were used to calculate the selectivity. For all Azo-CPPs, the calculated CO2/N2 adsorption selectivities were in the range of 27.4–53.9 at 273 K, and 31.2 to 107.8 at 303 K, respectively (Table 2 and Fig. S16 to S22 in the ESI†). These values at 273 K were comparable to or better than those of the nitrogen-containing nanoporous covalent triazine-based frameworks (CTFs, selectivity of CO2/N2 14–41) and some nitrogen containing MOPs (selectivity of CO2/N2 at 273 K, 17.3–30.6) under the same conditions.57–59 Compared with the reported Azo-COPs (selectivity of CO2/N2 at 273 K, from 63 to 124),33,43 the selectivities obtained herein were relatively lower, although they containing the same functional groups (azo bridges). It was considered that the “sieving effect” caused by the small pore width (0.48–0.80 nm)33 lead to the high CO2/N2 selectivity. The dominant pore width of all the Azo-CPPs obtained herein was larger than 1.14 nm, which was also larger than those of Azo-COPs.
As reported by C. T. Yavuz et al., the azo groups were “N2-phobic” groups, therefore the selectivities of CO2/N2 increased with increasing temperature. While according to the results by H. M. El-Kaderi and J. Zhang,44,45 the pore width of Azo-POF-2 (major pore width: 1.5 nm) and ALPs (major pore width: 1.0 nm to 1.3 nm) are larger than those of Azo-COPs, therefore the selectivity of CO2/N2 decreases as temperature increases. In fact, the selectivity of all Azo-CPPs herein showed a similar tendency to the Azo-COPs when temperature rose higher. For instance, when the test temperature went up from 273 K to 303 K, the selectivity of CO2/N2 increased to 31.2–107.8. The same tendency but with larger pore width was due to not only the azo bridges but also the porphyrin groups. In other words, the “N2-phobicity” came from both the azo bridges and the porphyrin groups in the present work. For example, Azo-COP-1 (SABET = 608 m2 g−1)33 and Azo-CPP-1 (SABET = 591 m2 g−1) had a similar surface area, but the N2 adsorption of Azo-COP-1 (2.95% at 273 K and 1.0 bar) was larger than that of Azo-CPP-1 (0.61% at 273 K and 1.1 bar) under otherwise same conditions. At higher temperatures, this phenomenon was even serious (1.19% for Azo-COP-1 at 298 K and 1.0 bar vs. 0.07% for Azo-CPP-1 at 303 K and 1.10 bar). These Azo-CPPs have potential applications in post-combustion CO2 capture and sequestration technology.
Footnote |
† Electronic supplementary information (ESI) available: Structure characterization of the Azo-CPPs; the nitrogen adsorption and desorption isotherms and pore size distributions of all Azo-CPPs; the CO2 adsorption isotherms, and the CO2/N2 selectivities of all Azo-CPPs. See DOI: 10.1039/c5ra17671a |
This journal is © The Royal Society of Chemistry 2015 |