Venkata S. Pavan K. Netia,
Xiaofei Wub,
Ping Penga,
Shuguang Dengb and
Luis Echegoyen*a
aDepartment of Chemistry, University of Texas at El Paso, El Paso, TX 79968, USA. E-mail: echegoyen@utep.edu; Fax: +1-915-747-8807; Tel: +1-915-747-7573
bDepartment of Chemical Engineering, New Mexico State University, Las Cruces, NM 88003, USA
First published on 28th January 2014
A new benzothiazole linked nanoporous polymer, imine benzothiazole polymer (IBTP), was synthesized via a Schiff base condensation reaction. IBTP showed high isosteric heat of adsorption (Qst) (37.8 kJ mol−1 at 273 K) and reasonable CO2 adsorption (7.8 wt% at 273 K/1 bar) as well as good selectivities, CO2/N2 (51) and CO2/CH4 (6.3). The Brunauer−Emmett−Teller (BET) surface area of IBTP was 328 m2 g−1 and it also showed good thermal stability up to 450 °C under a N2 atmosphere, thus showing good potential for CO2 capture.
Scheme 1 Synthesis of IBTP from 1,3,5-tris-(4-formylphenyl)-benzene and 2,6-diaminobenzo bisthiazole. |
The IBTP porous polymer was isolated in 72% yield as a dark brown powder. It was thoroughly washed with anhydrous dioxane and N,N′-dimethylformamide and was totally insoluble in dimethylsulfoxide, dichloromethane, acetone, and tetrahydrofuran. This new material exhibited a CO2 capture capacity of 7.8 wt% and a CH4 adsorption capacity of 0.9 wt% at 273 K, 1 bar and an adsorption capacity of 0.78 wt% for H2 at 77 K/1 bar. The chemical connectivity, components, crystallinity, porosity, and thermal stability of the IBTP porous polymer was determined by several analytical methods such as Fourier transform infrared spectroscopy (FT-IR) and solid-state 13C CP-MAS NMR, elemental analysis, powder X-ray diffraction (PXRD), surface area measurements, and thermogravimetric analysis. The FT-IR spectrum of IBTP showed highly attenuated N–H and CO stretching frequencies from the 1,3,5-tris-(4-formylphenyl)-benzene and 2,6-diaminobenzo bisthiazole at 3400 cm−1, 3280 cm−1 and 1740 cm−1. The formation of imine bonds between 1 and 2 (see ESI†) was confirmed by FT-IR which exhibited a new characteristic CN stretching frequency at 1690 cm−1 (Fig. S1–S2, ESI†). Solid-state 13C CP-MAS NMR measurements support the presence of benzothiazole and 1,3,5-tris-(4-formylphenyl)-benzene monomers in the framework. The IBTP polymer exhibited peaks at 169 and 156 ppm which correspond to the CN (–CN) carbons in the benzothiazole and imine units (Fig. S3, ESI†), respectively. In addition, the NMR spectrum also showed multiple peaks between 104 and 139 ppm which can be assigned to other aromatic carbon atoms from both building blocks. Powder X-ray diffraction (Cu Kα radiation) did not exhibit any diffraction peaks, as commonly observed for amorphous porous organic polymers (Fig. S4, ESI†).
N2 gas adsorption–desorption measurements of degassed IBTP confirmed its microporosity at 77 K (Fig. 1). The apparent Brunauer–Emmett–Teller (BET) surface area was 328 m2 g−1 and a surface area of 1705 m2 g−1 was obtained by applying the Langmuir model. The steady N2 uptake at low pressure (0–0.1 bar) and the gradual increase at higher pressures (0.1–1 bar) resulting a type I isotherm (Fig. 1a), which is typical for microporous frameworks that show permanent microporosity. This surface area is lower than others reported for imine linked polymers. Pore size distribution curves were analyzed by fitting the uptake of the N2 isotherm using the nonlocal density functional theory (NLDFT) method, and were found to be around 15 Å (Fig. S5, ESI†) and the pore volume was calculated to be 0.81 cm3 g−1. Hysteresis was observed with the desorption low lying above the adsorption, which could be due to the presence of micropores and diffusion of gas through micropores to mesopores that are also present in the framework and vice versa. To find the possible impact of the microporosity and nitrogen rich pore walls of IBTP, we measured CO2, CH4, N2 and H2 adsorption capacities and selectivity and calculated their respective isosteric enthalpies (Qst). All CO2, CH4 and N2 isotherms were measured at 273 and 298 K from 0–1 bar (Fig. 1c and d). Both CO2 and CH4 isotherms are reversible and exhibit a steep rise at P = 0–1 bar, the CO2 capture capacity of IBTP was 7.8 wt% at 273 K and 5 wt% at 298 K, respectively. The Qst value for CO2 was estimated from data collected under these conditions using the Van't Hoff equation. At zero coverage, the Qst is 37.4 kJ mol−1 (Fig. S6, ESI†). The CO2 uptake and Qst are higher than the corresponding value for most COFs and for imine POPs and comparable to ZIFs containing nitrogen functionalized pores. The relatively high binding capacity of IBTP for CO2 is likely due to favorable interactions between CO2 molecules and the nitrogen rich imine and benzothiazole units in the framework. The reversible adsorption–desorption behavior indicates that CO2 interactions with pore walls are weak enough to allow for IBTP regeneration without applying heat. Usually materials that have strong basic sites display high CO2 affinities and require energy input in the form heat to regenerate their active sites as in the case of commercial amine solutions. In addition to CO2 adsorption, we have evaluated the adsorption properties of N2, H2 and CH4 on IBTP at low pressures and different temperatures due to their potential use in automobile applications. The H2 uptake of IBTP shown in Fig. 1b, exhibited a reversible profile and pronounced hysteresis that we believe is due to the sulfur–hydrogen interactions. At 77 K, 1 bar, IBTP exhibited an uptake of 0.78 wt% which is comparable to other crystalline 2D COFs such as COF-102 (0.8 wt% at 77 K and 1 bar). Similarly, we measured CH4 and N2 storage properties on the IBTP polymer at both 273 K and 298 K, which revealed an uptake of 0.9 and 0.5 wt% for CH4 at 273 K and 298 K/1 bar and almost zero for N2 under similar conditions (Fig. 1d). Once again, both isotherms are reversible and exhibit a steep rise at low pressure for CH4 and then reach maxima at 1 bar, 273 and 298 K, respectively. The Qst for CH4 was calculated using adsorption data collected at 273 and 298 K. At zero coverage, the Qst for CH4 is 20.7 kJ mol−1 which is higher than for most COFs and POPs (Fig. S6, ESI†). A higher Qst value for CO2 compared to that of CH4 is likely due to the –N(δ−)–C(δ+)O2 interactions. Furthermore, the selectivity of IBTP towards CO2 over N2/CH4 was investigated by collecting isotherms at 273 and 298 K (Fig. S6, ESI†). At 273 K and 1 bar, the CO2 uptake is 7.8 wt% whereas that of CH4 is only 0.9 wt%. On the basis of Langmuir model fits and Henry's constant values in the pressure range of 0 to 1 bar, the estimated adsorption selectivity for CO2/N2 is 51 and for CO2/CH4 it is 6.3 at 273 K/298 K/1 bar. Similar calculation methods have been reported for COPs, obtaining selectivities higher (63–109 at 273 K) than the IBTP.2m We also measured the absorption spectra of IBTP and diaminobenzo bisthiazole monomer to find the absorption ability of benzothiazole units in the UV-Vis region. The molecular organization of these benzothiazole chromophores in the porous polymer was evident from new absorption peaks at 595 and 640 nm, with the spectrum of monomer 2,6-diaminobenzo bisthiazole, while peaks at 230 and 290 nm (Fig. 2) were conserved. This proves the presence of benzothiazole chromophores in the IBTP polymer which is further evident from the color change of the polymer sample to dark brown whereas the monomers are white and yellow.
Fig. 1 (a) Nitrogen at 77 K; (b) hydrogen at 77 K; (c) CO2 at 273 K and 298 K; (d) CH4 at 273 K and 298 K adsorption (filled symbols) and desorption (empty symbols) isotherm curves. |
Fig. 2 Solid-state UV absorption spectra of IBTP (red) and 2,6-diaminobenzo bisthiazole (blue) obtained from powders using a praying mantis diffuse reflectance accessory. |
To measure the thermal stability, IBTP samples were subjected to thermogravimetric analysis under a flow of N2 (Fig. S7, ESI†). The TGA trace is typical of the other reported POPs, retaining 80% of the mass at 450 °C. Visualization of these imine and benzothiazole based networks using scanning electron microscopy (SEM) showed randomly aggregated particles of IBTP powder, which did not provide any further insight into the porous nature of the framework (Fig. S8, ESI†).
Footnote |
† Electronic supplementary information (ESI) available: Experimental details, Fig. S1 and S9. See DOI: 10.1039/c3ra47587e |
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