Jun Gaoa,
Jing Xieb,
Xueyan Liua and
Hui Hu*a
aSchool of Environmental Science & Engineering, Huazhong University of Science and Technology, Wuhan 430074, China. E-mail: huhhust@163.com; Fax: +86 2787792141; Tel: +86 2787792141
bFaculty of Materials Science and Chemistry, China University of Geosciences, Wuhan 430074, China
First published on 7th April 2017
A series of porous carbon sorbents obtained by carbonization and activation by KOH/ZnCl2 of the abundant waste material cyanobacteria was utilized for the adsorption of H2. During experiments to determine the optimal activation parameters, the activation time had little effect, whereas the KOH/C and ZnCl2/C mass ratios and activation temperature had a significant impact on adsorption performance. Samples activated by KOH exhibited better adsorption characteristics (such as higher values of SBET, Vtotal, Vmicro, etc.) than those activated by ZnCl2. In particular, ACK-2-8, which had an SBET of 1951 m2 g−1, displayed H2 uptake capacities of nearly 17.3 mg g−1 at −196 °C and 1 bar. In addition, for evaluation of the H2 adsorption performance, N-doped and P-doped porous carbons were synthesized using HNO3, NH3·H2O and H3PO4, respectively, to modify the abovementioned cyanobacteria-derived activated carbon ACK-2-8, and exhibited H2 adsorption amounts that were 16.8%, 31.8%, and 45.7% higher, respectively, than those of undoped ACK-2-8. Furthermore, it was remarkable that P-doping in conjunction with a moderately high SBET enhanced the uptake of H2 by ACK-2-8-2, which had a smaller SBET than ACK-2-8-3 but the best uptake capacity of up to 25.2 mg g−1, and thereby showed that the relationship between the H2 adsorption capacity and SBET of these materials was scarcely linear and was therefore noticeably different from previously reported results for the uptake of H2 by other carbon sorbents. Hence, it is probable that the considerable H2 adsorption properties of the material with a moderate SBET have great potential applications for hydrogen capture or storage.
Recently, abundant research into porous materials including carbon materials,10–13 zeolites,14,15 metal–organic frameworks (MOFs),16–18 and covalent organic frameworks (COFs)19,20 has been widely undertaken. Among these, carbon materials have been extensively studied as candidates for hydrogen storage owing to their large surface area, well-developed pore structure, low cost, low mass density, and so on.21,22 In general, a large surface area and large micropore volume are essential for enhancing the uptake of hydrogen.23–26 Activated carbons based on carbon materials can be prepared from a large number of precursors, which include vegetable, mineral, and purely synthetic sources such as organic gels and polymers.4 However, from the viewpoint of sustainability, environment-friendliness, and continuous availability, biomass-based materials are more promising sources of carbon for porous carbons.5,27–31 Cyanobacteria are phototrophic bacteria that exist in several ecosystems across the planet and are key contributors to global photosynthesis.32 However, not all cyanobacteria are beneficial to the environment and human health; some cyanobacteria grow and expand too fast, contaminating freshwater and creating toxins.33 Owing to the abundance and accessibility of cyanobacteria, it is desirable to confirm the suitability of converting this form of biomass into active carbon for energy storage. Thus far as we know, few studies have attempted to use cyanobacteria as a precursor for activated carbon in materials science other than as supercapacitor electrodes.32 In this study, for use as low-cost, abundant and available carbon precursors, cyanobacteria (CB) obtained from Dianchi in Yunnan Province, China were prepared for precursors. As hydrogen adsorption performance requires very large surface areas and very narrow pores, activation by KOH is known to be among the best methods for obtaining carbon materials having such characteristics. Thus, cyanobacteria-based activated carbons prepared by activation by KOH and also other carbons prepared using ZnCl2 were used for comparison. As a number of studies have reported,34–37 the weight ratio of the activating agent to the precursor and the activation temperature have a great effect on the uptake of hydrogen. The influence of the activation parameters will be investigated in the following research.
The adsorption of H2 could be characterized as physisorption with weak van der Waals interaction forces. Much effort has been devoted to increasing the specific surface area because a highly porous structure is indispensable for a high adsorption capacity.38 Moreover, it is necessary to improve the adsorption efficiency and enhance the interactions between the gas and carbon material, which is of great importance for the adsorption performance of carbon materials. Heteroatom doping is widely used to modify carbon materials for efficient adsorption.39 For the adsorption of different gases, the presence of heteroatoms leads to a remarkable performance.5,38–41 Some studies suggest that the surface polarity created by the discrepancy in electronegativity between heteroatoms and carbon could enhance the interactions between gas molecules and the carbon surface.5,38 For the adsorption of hydrogen, Li et al. investigated the influence of doping nitrogen, sulfur, and phosphorus into activated carbons on the adsorption of H2, CH4 and CO2 gases, which exhibited a favorable effect on the adsorption of H2.38 In order to achieve further enhancements in adsorption efficiency, further modifications of cyanobacteria-derived activated carbon were performed by impregnation with HNO3, H3PO4, and NH3·H2O, respectively. The H2 adsorption properties were investigated systematically and the possible effects and causes were also discussed.
In turn, further modifications of the samples were carried out by adding ACK-2-8 to 50 mL of the corresponding 10 wt% solution of HNO3, H3PO4, or NH3·H2O, respectively, in a water bath at 60 °C for 3 h, followed by washing with distilled water until the wash water reached a neutral pH and drying at 105 °C for 24 h in a vacuum drying oven. These samples were respectively named as ACK-2-8-1, ACK-2-8-2 and ACK-2-8-3 for simplicity.
The physical parameters of the initial and modified AC samples, including their adsorption–desorption characteristics, BET surface area (SBET), total pore volume (Vtotal), micropore volume (Vmicro) and average pore size (), were determined using an automatic specific surface area and porosity analyzer (JW-BK122W, JWGB Ltd.). The adsorbed volume of high-purity N2 was measured under different pressures at −196 °C. The SBET value was calculated using the Brunauer–Emmett–Teller method. The pore size distribution was computed using the Barrett–Joyner–Halenda method from the adsorption branch of the isotherm.44 The micropore volume (Vmicro) and micropore-specific surface area (Smicro) were determined using the t-plot method.43 All samples were characterized by microscopy techniques. Scanning electron microscopy (SEM) was performed using a Jeol JSM-6301F microscope. X-ray photoelectron spectroscopy (XPS) was carried out using a Thermo Scientific Al Kα source. A static gas adsorption instrument (NOVA 3200e, Quantachrome) was used to measure the adsorption of H2 in the pressure range of 0.01–1 bar at −196 °C.
TG/DTG experiments on CB were performed at a heating rate of 20 °C min−1 and the thermal decomposition was studied from ambient temperature to 800 °C, and the corresponding curves are shown in Fig. 1. It was demonstrated that the thermal decomposition of CB could be divided into three main stages. Stage I occurred in the low-temperature region (below 250 °C) and resulted in low mass loss (TG curves). It was found to be attributed to the evaporation of physically adsorbed water and light volatile compounds. Stage II, which covered the temperature range from 250 °C to 400 °C and exhibited a high mass loss percentage (approximately 50%), was ascribed to the decomposition or devolatilization of CB. The thermal degradation behavior in stage III, which was characterized by low mass loss, was probably due to the decomposition of carbonaceous materials retained in char residues. Overall, the mass losses of CB amounted to over 60% during stages I and II of the thermal decomposition process. The reason was that CB contained large amounts of volatile matter and moisture but less ash content. From the DTG curve, it could be observed that the sharp peak that appeared near 300 °C indicated the maximum mass loss rate, and then the mass loss rate practically remained unchanged with an increase in temperature above 400 °C. Therefore, this would be appropriate for selection of the carbonization temperature during the preparation of activated carbon.
When the activation temperature and time were fixed at 600 °C and 2 h, respectively, the NADIs and PSD curves for some materials are presented in Fig. 2, and the corresponding parameters of the porous architectures are summarized in Table 2. In comparison with AC (Fig. S2 (ESI†)), the data for the activated counterparts ACK-X-6 and ACZ-X-6 all exhibited a steep increase, which indicated better absorption characteristics, i.e., SBET, Vtotal and Vmicro all displayed evident increases. The two kinds of sample with activation temperatures of 600 °C exhibited highly microporous structures with type I adsorption curves. The sharp increases in the adsorption curves at low relative pressures were indicative of the development of micro- and supermicropores. Specifically, the increase in the amount of N2 adsorbed by the samples with an increase in relative pressure exhibited a nearly linear relationship, with a hysteresis loop occurring at high relative pressures. This phenomenon implied the existence of a considerable number of mesopores, in which capillary condensation enabled the adsorption capacity to rise rapidly with respect to an increase in pressure.43
Sample | SBET (m2 g−1) | Vtotal (cm3 g−1) | Vmicro (cm3 g−1) | (nm) |
---|---|---|---|---|
ACK-0.5-6 | 644 | 0.404 | 0.312 | 4.81 |
ACK-1-6 | 705 | 0.429 | 0.344 | 4.62 |
ACK-2-6 | 1006 | 0.578 | 0.505 | 2.30 |
ACK-3-6 | 970 | 0.545 | 0.454 | 2.23 |
ACZ-1-6 | 901 | 0.514 | 0.428 | 2.28 |
ACZ-2-6 | 996 | 0.640 | 0.496 | 2.31 |
ACZ-3-6 | 1268 | 0.760 | 0.531 | 2.39 |
In addition, the amount of N2 adsorbed on activated carbon increased with an increase in the KOH/C or ZnCl2/C mass ratio (Fig. 2a and c). The maximum value was achieved at a KOH/C or ZnCl2/C mass ratio of 3, but a remarkable difference was observed in that the adsorbed amounts were nearly identical at KOH/C mass ratios of 2 and 3. Therefore, in the subsequent experiments KOH/C mass ratios of 2 and 3 and a ZnCl2/C mass ratio of 3 were utilized, respectively, to determine the optimum activation temperature.
Similarly, the effect of the activation temperature on samples (denoted as ACK-2-Y, ACK-3-Y and ACZ-3-Y) was studied via N2 adsorption–desorption experiments, in which the activated carbon was prepared with KOH/C mass ratios of 2 and 3 or a ZnCl2/C mass ratio of 3 and an activation time of 2 h. The results are illustrated in Fig. 3, whereas the structural parameters are listed in Table 3. The NADIs and PSD curves almost all exhibited a type I nitrogen adsorption isotherm, which indicated the development of micro- and supermicropores at low relative pressures. The remarkable hysteresis loop that occurred at high relative pressures with some samples (i.e., ACK-2-7, ACK-2-8, and ACZ-3-8) provided evidence of the presence of some mesopores. For the materials activated by KOH (Fig. 3a–e), the amount of nitrogen adsorbed increased and reached a maximum at an activation temperature of 800 °C, whereas the volumes of micropores and mesopores underwent appreciable increases with an increase in activation temperature at KOH/C mass ratios of both 2 and 3. As can be clearly seen, samples with a KOH/C mass ratio of 2 achieved greater nitrogen adsorption performance than those with a KOH/C mass ratio of 3 at a certain activation temperature (Fig. 3a and b). For the samples activated by ZnCl2, the amount of nitrogen adsorbed first decreased in the activation temperature range of 600–700 °C and then increased with an increase in activation temperature from 700 °C to 800 °C (Fig. 3c and f). The optimal temperature was 800 °C, and the sample was denoted as ACZ-3-8.
Sample | SBET (m2 g−1) | Vtotal (cm3 g−1) | Vmicro (cm3 g−1) | (nm) |
---|---|---|---|---|
ACK-2-6 | 1006 | 0.578 | 0.505 | 2.30 |
ACK-2-7 | 1694 | 0.887 | 0.700 | 2.10 |
ACK-2-8 | 1951 | 1.092 | 0.756 | 2.27 |
ACK-3-6 | 970 | 0.545 | 0.454 | 2.23 |
ACK-3-7 | 1111 | 0.592 | 0.487 | 2.13 |
ACK-3-8 | 1854 | 0.992 | 0.724 | 2.26 |
ACZ-3-6 | 1268 | 0.760 | 0.531 | 2.39 |
ACZ-3-7 | 1176 | 0.720 | 0.505 | 2.45 |
ACZ-3-8 | 1310 | 0.798 | 0.547 | 2.49 |
In order to obtain better pore structural parameters and greater adsorption of H2, further modified the activated carbons derived from cyanobacteria (denoted as ACK-2-8-1, ACK-2-8-2, and ACK-2-8-3, respectively) were characterized using the N2 adsorption–desorption method. The results shown in Fig. 4 and Table 4 imply that the other three samples exhibited type I nitrogen adsorption isotherms that were unexpectedly the same as that of ACK-2-8, and moreover the development of micro- and supermicropores at low relative pressures and some mesopores at higher relative pressures occurred for all the samples. It was easily found that ACK-2-8-3 exhibited the greatest adsorbed amount of N2 and the largest SBET of 2125 m2 g−1. The samples ACK-2-8-1, ACK-2-8-2 and ACK-2-8-3 on H2 adsorption would be advanced undergone succeeding study.
Sample | SBET (m2 g−1) | Vtotal (cm3 g−1) | Vmicro (cm3 g−1) | (nm) |
---|---|---|---|---|
ACK-2-8 | 1951 | 1.092 | 0.756 | 2.27 |
ACK-2-8-1 | 1846 | 1.023 | 0.735 | 2.22 |
ACK-2-8-2 | 1901 | 1.026 | 0.726 | 2.26 |
ACK-2-8-3 | 2125 | 1.238 | 0.834 | 2.33 |
Fig. 5 Scanning electron micrographs of samples of AC (a and b), ACK-2-8 (c and d) and ACZ-3-8 (e and f). |
To determine the reason for the subsequent adsorption of H2 on some cyanobacteria-derived activated carbons, the classic Boehm method was adopted to characterize the chemical properties of the adsorbent surface, and moreover X-ray photoelectron spectroscopy (XPS) was carried out to identify the nature of the nitrogen or phosphorus species that were impregnated into ACK-2-8 via modification with HNO3, H3PO4 and NH3·H2O, respectively. As can clearly be seen in Fig. S3 (ESI†), the surface functional groups on the adsorbents were mainly acidic groups except in the case of ACK-2-8-3, which after impregnation with ammonium hydroxide contained 2.7 times more basic groups than ACK-2-8. Acid groups were particularly rich in ACK-2-8-1 and were approximately 20% more abundant than in ACK-2-8. In comparison, ACK-2-8-2 displayed a moderate decrease in the number of acidic groups, and the number of basic groups scarcely varied with respect to ACK-2-8. The XPS spectra of the doped elements used to further modify the carbon material ACK-2-8 are illustrated in Fig. 6. The resulting N 1s spectra (Fig. 6a and c) and P 2p spectrum (Fig. 6b) proved that nitrogen and phosphorus were successfully integrated into the porous carbons in a systematic way. In the N 1s spectrum of ACK-2-8-1, three peaks were observed at 398.55 eV, 400.2 eV, and 401.1 eV, which corresponded to pyridinic N, pyrrolic/pyridonic N and graphitic N, respectively.47–49 However, pyrrolic N and pyridonic N species are difficult to distinguish within the range of accuracy of XPS measurements.5 The nitrogen species of ACK-2-8-3 were represented (Fig. 6c) by peaks at 398.55 and 400.2 eV, which were assigned to pyridinic N and pyrrolic/pyridonic N, respectively. Furthermore, the single peak observed at 133.1 eV in the P 2p spectrum of ACK-2-8-2 indicated that phosphorous was doped in the form of P–O.50
Fig. 6 XPS spectra of ACK-2-8 carbon materials with further modifications: (a) ACK-2-8-1, modified by HNO3, (b) ACK-2-8-2, modified by H3PO4, and (c) ACK-2-8-3, modified by NH3·H2O. |
Fig. 7 (a) Hydrogen adsorption isotherms at −196 °C and (b) relationship between the amount of H2 adsorbed (at −196 °C and 1 bar) and the BET surface area. |
Sample | SBET (m2 g−1) | H2 uptake (mg g−1) | H2 uptake per SBET (mg m−2) | |
---|---|---|---|---|
This publication | ACZ-3-8 | 1310 | 11.6 | 0.0088 |
ACK-3-8 | 1854 | 17.1 | 0.0092 | |
ACK-2-7 | 1694 | 16.7 | 0.0099 | |
ACK-2-8 | 1951 | 17.3 | 0.0089 | |
ACK-2-8-1 | 1846 | 20.2 | 0.0109 | |
ACK-2-8-2 | 1901 | 25.2 | 0.0133 | |
ACK-2-8-3 | 2125 | 22.8 | 0.0107 | |
Ref. | C-4 (ref. 8) | 3870 | 39 | 0.01 |
P2 (ref. 31) | 1807 | <20 | <0.0111 | |
Carbide-derived carbons10 | <3000 | 3–27 | <0.01 | |
MOFS7 | 1132–4346 | 11.7–25.4 | <0.01 | |
Zeolite-based carbons43 | 2254 | 22.7 | 0.0101 | |
PC-2-800 (ref. 5) | 2919 | 27.1 | 0.0093 | |
ACs28 | <2500 | <20 | 0.008 | |
ACs3 | 2849 | <30 | <0.01 | |
CAC44 | 1767–3711 | 19.2–32.1 | 0.0086 | |
UCs45 | 1127.2 | 1.43 | 0.0013 |
Similarly, Fig. 8 shows H2 adsorption isotherms measured at −196 °C for further modified cyanobacteria-derived activated carbons. In comparison to ACK-2-8, the H2 uptake at 1 bar increased in order from ACK-2-8-1 via ACK-2-8-3 to ACK-2-8-2, which represented the ACK-2-8 sample modified by HNO3, NH3·H2O and H3PO4, respectively. The H2 uptake at −196 °C and a pressure of 1 bar was found to reach the highest value of 25.2 mg g−1 for ACK-2-8-2, which was 45.7% higher than that for ACK-2-8 (Table 5). Nonetheless, it was remarkable that the SBET of ACK-2-8-2 was not the largest of all four samples, as the SBET of ACK-2-8-3 was 2125 m2 g−1. A weaker linear relationship was found between the adsorption of H2 and the SBET with a correlation coefficient R2 of only 0.0214, as shown in Fig. S4 (ESI†). According to the prior study of surface functional groups (Fig. S3†), it could be concluded that the presence of basic groups would inhibit the uptake of H2, whereas the amount of acidic surface groups might favor the adsorption of H2 to some extent. In comparison with the surface groups, the SBET should exert a much greater effect on the uptake of H2. Regarding the ACK-2-8-1 and ACK-2-8-3 samples, in addition to the sufficiently large SBET doping with nitrogen, as the XPS results showed, would favor the uptake of H2. This result was different from prior reports. Jiang et al.51 considered that doping with nitrogen had no obvious positive influence on the adsorption of hydrogen at 77 K. Xia et al.52 concluded that the effect of N doping on the uptake of hydrogen was only apparent when related to the surface area and pore volume associated with micropores rather than the total porosity. The differences were probably due to the different carbon precursors and doping methods used. Doping with phosphorus in ACK-2-8-2 promoted the adsorption of H2 in this study, which was in accordance with a previous investigation.38 Furthermore, when taking into account the uptake of H2 at the same time as the specific surface area of the material, it can clearly be seen from Table 5 that ACK-2-8-2 exhibited a noteworthy adsorption capacity of 25.2 mg g−1 with a modest SBET 1901 m2 g−1 and holds great potential for the adsorption of H2. In other words, ACK-2-8-2 displayed evidently superior hydrogen storage density (i.e., hydrogen uptake per surface area).
Fig. 8 Hydrogen adsorption isotherms normalized to the adsorption capacity from 0 to 1 bar for different samples. |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c6ra28660g |
This journal is © The Royal Society of Chemistry 2017 |