Abstract
Adsorption is one of the most promising methods for desulfurization of transportation fuels, due to the strategy which enables removal of organic sulfur compounds to be conducted at ambient conditions with high efficiency. Adsorbent is the key to the adsorptive performance. Both π complexation and direct sulfur metal bonds are efficient methods for adsorptive desulfurization. For construction of these bonds, it is necessary to introduce active metal species on the support. In this work, Ce(NO3)2 was directly introduced into the as-synthesized SBA-15, and high dispersion of CeO2 nanoparticles was obtained. With the loading content of 12–46 wt%, the particle sizes of the CeO2 NPs are in the range of 4.4–6.3 nm. The good dispersion status of CeO2 nanoparticles is contributed to the template P123 preserved in as-synthesized SBA-15, which provides a confined space for the dispersion of CeO2 nanoparticles. However, the large CeO2 particles (7.0 nm) are formed for the sample originated from template-free SBA-15. We also demonstrate that the adsorptive performance of SBA-15 is enhanced with the modification of CeO2 nanoparticles. Besides, the performances of CeO2 nanoparticle-modified samples stay in step with the dispersion status of the CeO2 nanoparticles.
Introduction
Deep desulfurization from transportation fuels has been of great urgency due to more stringent environmental regulations worldwide (Cao et al., 2008; Sitamraju et al., 2015; Wang et al., 2012). Besides, fuel cell technologies call for the hydrogen resource with nearly zero sulfur content (Kannan and Kumar, 2016; Speder et al., 2016). Nowadays, refineries mainly rely on the hydro-desulfurization (HDS) process to remove sulfur compounds in industry. HDS technology is operated at harsh conditions, including super-high temperatures of 300–350℃ and ultrahigh hydrogen pressures of 2–10 MPa (Shang et al., 2004; Singh and Kunzru, 2016; Sun and Prins, 2008; Vit et al., 2015). The HDS technology is efficient in removing inorganic sulfur compounds, including thiols and sulfides. However, it is less effective to remove organic sulfur compounds, including thiophene and its derivatives (Dai et al., 2006; Yang et al., 2003). It is highly desirable to further decline the sulfur concentration. Removal of organic sulfur compounds has been researched by various methods, including extraction, oxidation, and biological strategy (Moghadam et al., 2017; Xu et al., 2017). It is fortunate that these methods show positive effects on the removal of organic sulfur compounds. However, they inevitably show some shortcomings referring to consuming energy, producing byproducts, and generating slow biodegradation. There is thereby an urgent need but it is still a significant challenge to achieve deep desulfurization levels. Among the alternatives, one of the most important future directions of desulfurization is adsorption. There is great potential in using adsorbents for deep desulfurization, because organic sulfur molecules can be captured at ambient conditions with high efficiency (Song et al., 2014; Vilarrasa-Garcia et al., 2011b; Xiong et al., 2010). It is commonly known that both π complexation and direct sulfur metal (S–M) bonds can work for adsorptive desulfurization (Danmaliki and Saleh, 2017; Khan et al., 2017; Shi et al., 2017 Song et al., 2013). Thus, active species, such as Cu2O (Jiang et al., 2013; Wang et al., 2009b), CeO2 (Song et al., 2016; Xiao et al., 2013a), etc. are always incorporated into the porous materials for fabrication of π complexation or direct S–M sites. It is known that the porous materials with high surface areas are highly desirable for loading active species (Li et al., 2016; Xiao et al., 2013b; Yin et al., 2016). In addition, it is demonstrated in a number of studies that key to the adsorption performance of the adsorbent is the status of supported active species (Hernández-Maldonado and Yang, 2004b; Song et al., 2011).
Since the M41-typed mesoporous materials were first synthesized in 1992, a large number of mesoporous materials have been synthesized by use of the surfactant template method (Feng et al., 2012; Liu et al., 2002; Stein, 2003; Thomas, 2010). Among the mesoporous materials, mesoporous silica shows high surface areas and modest pore sizes and is very suitable for application as the support (Cruz et al., 2016; Eedugurala et al., 2015; Gaudin et al., 2016; Sun et al., 2015; Zhang et al., 2008). In general, mesoporous silica is a promising host for preparation of the selective adsorbent (Anbia and Mohammadi, 2008; Tian et al., 2010; Wang et al., 2006; Yin et al., 2014). Normally, the as-synthesized mesoporous silica is first to calcine, which leads to generate template-free mesoporous silica with open pores. The precursor is then incorporated into the open pores, with the second calcination to convert the precursor to active species (Cheng et al., 2015; Shao et al., 2012; Vilarrasa-Garcia et al., 2011b). This conventional method requires repeated calcination, which is low efficiency and energy consuming. According to the previous reports of Zhu and Liu's groups, there is a special confined space between template P123 and silica walls in as-synthesized mesoporous silica (Yin et al., 2012; Yue et al., 2008). By direct introduction of the precursor into the as-synthesized SBA-15 (ASS), high dispersion of active species is achieved by use of the extraordinary confined space.
Herein, we report for a new strategy for functionalization of mesoporous silica SBA-15 with CeO2 nanoparticles (NPs) in order to prepare adsorbents for desulfurization. Before removal of the template P123, Ce(NO3)2 was directly introduced into ASS via solid-state grinding. Followed with calcination in air, the resultant adsorbents were obtained. We denoted the adsorbents as CeO2-ASS. For contrast, Ce(NO3)2 was introduced into template-free SBA-15 (TFS) as well for preparation of the CeO2-TFS sample. The results show that by use of ASS as the support, the CeO2 NPs are controlled in the size of 4.4–6.3 nm. The confined space between template P123 and silica walls in ASS plays an important role on the high dispersion of CeO2 NPs. For the sample based on TFS, however, the large CeO2 NPs (7.0 nm) are formed and give rise to partly disordered and blocked pores of SBA-15. We also demonstrate that the CeO2 NP-modified materials show better performances than pure SBA-15 on adsorptive desulfurization. This is contributed to the formation of S–M bonds between CeO2 and thiophene. It is important to highlight that the CeO2-ASS samples show much better adsorptive desulfurization performances than CeO2-TFS.
Experimental
Materials synthesis
ASS and TFS
Mesoporous silica SBA-15 was synthesized following the literature method, which was first reported by Zhao et al. (1998). Two gram of pluronic EO20PO70EO20 (P123) was first added to 75 g of HCl aqueous solution (1.6 m). The mixture was stirred for half an hour. After dissolving, 4.25 g of silica source tetraethylorthosilicate was added. Then, stirring was conducted once again at 40℃ for 24 h. The mixture was then transferred to the teflon-lined autoclave for hydrothermal treatment at 100℃ for 24 h. After cooling to room temperature, the powder was collected by filtration. ASS was obtained after the powder was dried at room temperature. TFS was obtained by removal of template P123, which was conducted by calcination at 550℃ for 5 h in flowing air.
xCeO2-ASS
The precursor Ce(NO3)3·6H2O was introduced into ASS via solid-state grinding at room temperature for 30 min. The thoroughly mixed powder was calcined in flowing air at 500℃ for 5 h to form active CeO2 NPs, and template P123 was removed simultaneously. The obtained composites were denoted as
xCeO2-TFS
In a conventional process,
Characterization
XRD spectra were collected with a Bruker D8 Advance diffractometer using Cu
Fourier transform infrared (IR) spectra were recorded on a Nicolet Nexus 470 spectrometer with a spectral resolution of 2 cm−1 using transparent KBr pellets. Thermogravimetric (TG) analysis was performed on a thermobalance (STA-499C, NETZSCH). About 10 mg of sample was heated from the room temperature to 800℃ in a flow of air (25 ml min−1).
Adsorptive test
The simulated fuel was prepared using thiophene as the representative of organic sulfur contaminants. By mixing thiophene with isooctane, the sulfur concentration was controlled to be 550 ppmw (parts per million by weight). The desulfurization performance of adsorbents was evaluated on the basis of breakthrough curves. Experiments were performed at room temperature in a vertical quartz column with 6 mm in diameter. Adsorbents (0.2 g) were filled into the vertical quartz column, and a quartz grid was supported. Prior to measurement, the adsorbents were activated in situ by calcination at 200℃ for 2 h in air. After cooling to room temperature, the gas of air was switched to the simulated fuel, which was pumped up with a mini creep pump at a rate of 3.0 ml h−1. Effluent solutions were collected at regular intervals until saturation was reached. The sulfur content in effluent solutions was determined with a Varian 3800 gas chromatograph (GC) equipped with a pulsed-flame photometric detector. A calibration curve was prepared to analyze the GC results. Breakthrough curves were generated by plotting the normalized sulfur concentration versus the cumulative fuel volume. The normalized concentration (
Results and discussion
Status of supported CeO2 NPs
Figure 1(a) depicts the low-angle XRD patterns of SBA-15, CeO2-ASS, and CeO2-TFS samples. Mesoporous silica SBA-15 shows an intense diffraction line indexed as (100), and two weak lines indexed as (110) and (200) reflections. This indicates that SBA-15 contains a 2D (a) Low-angle and (b) wide-angle XRD patterns of SBA-15, CeO2-ASS, and CeO2-TFS samples. ASS: as-synthesized SBA-15; TFS: template-free SBA-15; XRD: X-ray diffraction.
Physicochemical properties of SBA-15, CeO2-ASS, and CeO2-TFS samples.
ASS: as-synthesized SBA-15; BET: Brunauer–Emmett–Teller; TFS: template-free SBA-15.
ICP data.
CeO2 crystallite size calculated by the Scherrer formula.
Figure 2 shows the HRTEM images of CeO2-ASS and CeO2-TFS samples. The TEM image of pure SBA-15 is presented in Figure S1. The silica walls of SBA-15 appear as dark, and pore spaces appear as white. Thus, highly ordered pore structures of SBA-15 can be judged. After functionalization of SBA-15 with ceria, the TEM images have a slight change. For the 36CeO2-ASS sample, the mesopores keep with a long-range order as well as SBA-15. In addition, some shadow areas appeared, which contributed to dispersed CeO2 NPs on the SBA-15. As for the 36CeO2-TFS sample, CeO2 NPs with large sizes can be identified. Moreover, the channels of SBA-15 are found to be partly disordered and blocked by the CeO2 NPs.
HRTEM images of (a), (b) for 36CeO2-ASS and (c), (d) for 36CeO2-TFS samples. ASS: as-synthesized SBA-15; HRTEM: high-resolution transmission electron microscopy; TFS: template-free SBA-15.
Figure 3(a) depicts the N2 isotherms of the adsorbents. Figure 3(b) shows the pore size distribution curves calculated from the desorption branches of isotherms. Table 1 displays the surface areas, pore volumes, and pore sizes of the adsorbents. Support SBA-15 shows a type IV isotherm shape with an H1 hysteresis loop at the relative pressure ( (a) N2 adsorption–desorption isotherms and (b) pore size distributions of SBA-15, CeO2-ASS, and CeO2-TFS samples. Curves are plotted offset for clarity. ASS: as-synthesized SBA-15; TFS: template-free SBA-15.
According to the XRD, TEM, and N2 adsorption–desorption results, it is necessary to have a summary on the combination status of CeO2 NPs and SBA-15. First, due to the similar low-angle XRD patterns with SBA-15, white dark contrast on the TEM images, and distinct hysteresis loop on the N2 adsorption–desorption isotherms, it is safe to deduce that the mesoporous structures of SBA-15 are well preserved after the modification of CeO2 NPs. Second, on the basis of weaken intensity of (100) reflection on the low-angle XRD patterns, identified CeO2 NPs on the TEM images, and movement of the closing point of the hysteresis loop on the N2 adsorption–desorption isotherms, it is reasonable to believe that the CeO2 NPs are introduced into the pores of SBA-15. Third, the CeO2 NPs show various statuses with the diverse ceria content and synthetic methods. In detail, the sizes of CeO2 NPs in the CeO2-ASS samples derived from wide-angle XRD pattern are in the range of 4.4–6.3 nm. In comparison with 36CeO2-ASS (5.1 nm), the size of the CeO2 NPs in the 36CeO2-TFS sample is larger (7.0 nm). Moreover, the 36CeO2-ASS sample shows higher surface area, pore volume, and pore size than the 36CeO2-TFS sample. These data are consistent with the notion that CeO2 NPs in the CeO2-ASS samples have better dispersion status than in CeO2-TFS. In other words, the application of ASS as support is propitious to the high dispersion of CeO2 NPs.
To further verify the location of the ceria, XPS analyses were carried out to study the surface properties of the samples. Figure S2 shows the results, and Table S1 summarizes the atomic concentration of Si, O, and Ce elements in the 36CeO2-ASS and 36CeO2-TFS samples. The theoretical value of the atomic concentration of Ce is 30.78. It is unusual that the value measured with XPS technique (1.03, 1.12) is much lower than the theoretical value (30.78). Take in mind that the XPS is the surface technique. The measured low atomic concentration of Ce is due to the formation of aggregated ceria on the surface of SBA-15. What needs to be emphasized is that the concentration is strongly low both in the 36CeO2-ASS and 36CeO2-TFS samples. Thus, it is safe to say that the location of most ceria is inside the mesopores of the porous silica rather than on the surface.
Proposed mechanism for high CeO2 dispersion in CeO2-ASS
IR spectra of the samples before and after calcination are presented in Figure 4. The bands in the range of 2850–3000 and 1350–1500 cm−1 appearing on the spectrum of ASS are the characteristics of template P123 (Figure 4(a)) (Tian et al., 2002). With calcination, ASS transforms to TFS, the bands of template P123 is absent, which is ascribed to massive decomposition of the template P123. The carbon content in ASS is 30.59 wt%, after calcination, the carbon content in SBA-15 goes down to 0.32 wt%. This indicates that there is little carbonaceous substance remaining after the removal of template P123. With introduction of Ce(NO3)2 into ASS, some new bands at 1380 cm−1 appeared in the 36CeO2-ASS sample. The new bands are due to the asymmetric stretching vibration of N–O (Yin et al., 2012), which illustrates the existence of IR spectra of SBA-15, CeO2-ASS, and CeO2-TFS samples (a) before and (b) after calcination. ASS: as-synthesized SBA-15; TFS: template-free SBA-15.
As shown in Figure 5, the decomposition behaviors of the samples are investigated by the TG technique. In ASS, the removal of template P123 takes place from 155 to 270℃ with a massive weight loss of 50%. In cooperation, there is a sharp DTG peak at 162℃. It is worthwhile to note that pure P123 decomposes at about 210℃ (Zhao et al., 1998). In comparison, the decomposition temperature of P123 in ASS is lower than pure P123. There is the strong possibility that the silica frameworks in ASS catalyze the removal of the template P123. For the Ce(NO3)2-modified template-free SBA-15 sample (36CeO2-TFS), the decomposition procedure due to evaporation of adsorbed water goes from room temperature to 80℃. The decomposition of Ce(NO3)2 in 36CeO2-TFS proceeds from 80 to 450℃ with a weight loss of 35.5%, which coincides with the calculated value of 35.7%. This indicates the massive conversion of Ce(NO3)2 to CeO2. For the Ce(NO3)2-modified ASS, the curve of weight loss shows its own characteristics. In the 36CeO2-ASS sample, the conversion of Ce(NO3)2 in ASS starts from 80 to 168℃. There is a weight loss of 25.2%, which is well consistent with the calculated value of 25.3%. This suggests the massive conversion of Ce(NO3)2 to CeO2 as well. Subsequently, the removal of template P123 starts from 168 to 355℃, corresponding to a sharp DTG peak at 208℃.
(a) TG and (b) DTG curves of SBA-15, CeO2-ASS, and CeO2-TFS samples before calcination. DTG curves are plotted offset for clarity. ASS: as-synthesized SBA-15; DTG: derivative thermogravimetric; TFS: template-free SBA-15; TG: thermogravimetric.
According to the aforementioned results, CeO2 NPs in the CeO2-ASS samples show better dispersion status than in CeO2-TFS. Next, we explored the proposed reasons. For the CeO2-ASS samples, Ce(NO3)2 was directly introduced into the ASS with template P123. IR results prove that both template removal and Ce(NO3)2 conversion can be achieved in a step of calcination. TG results show that the removal of P123 in 36CeO2-ASS occurs at temperature of 216℃. This decomposition temperature is much higher than that in ASS (162℃) and almost the same as pure P123 (210℃). This word points that the Ce(NO3)2 is indeed incorporated into the confined space between template P123 and silica walls. Therefore, the catalysis of silica walls to the decomposition of the template P123 does not work. We have noticed that the conversion of Ce(NO3)2 in the 36CeO2-ASS sample completes before the decomposition of template P123. That is to say, the conversion of Ce(NO3)2 is carried through within the confined space. Hence, at current time, we have to demonstrate that the conversion order of precursor and template P123 is key to the dispersion status of CeO2 NPs. If the conversion of precursor takes precedence over the removal of template P123, the confined space will give a boost for the high dispersion of CeO2 NPs. Otherwise, the earlier decomposition of template P123 will result in the damage of the confined space. As for the 36CeO2-TFS sample, the template P123 decomposes before the introduction of Ce(NO3)2. Therefore, the template P123 can no longer play a role on the dispersion status of CeO2 NPs. To this end, we show that the better CeO2 dispersion in CeO2-ASS results from the confined space in ASS.
Performance on adsorptive desulfurization
The adsorptive desulfurization performances of the samples are measured with the simulated fuels, which contain 550 ppmw of sulfur. The breakthrough curves are shown in Figure 6. The values of adsorption capacity were calculated according to the breakthrough curves at saturation, and results are listed in Table 1. The support SBA-15 is capable of 0.105 mmol g−1 of thiophene, which exhibits the worst performance among all the samples. After modification of SBA-15 with CeO2 NPs, the desulfurization capacities evidently improve. The adsorption capacities for the 12CeO2-ASS, 22CeO2-ASS, and 36CeO2-ASS samples step up from 0.131 to 0.165 mmol g−1 with the increase of ceria content. For the sample of 46CeO2-ASS, the adsorption capacity is 0.136 mmol g−1. The counterpart sample of 36CeO2-TFS shows the worst performance among all the CeO2 NP-modified samples. The uptake is as low as 0.115 mmol g−1. Many adsorbents so far have been prepared for removal of organic sulfur compounds. For Ce(IV) exchanged Y zeolite, the adsorption capacity is 0.122 mmol g−1 with 297 ppmw of sulfur in commercial diesel (Hernandez-Maldonado and Yang, 2004a). The Cu(I)/SBA-15 adsorbent is derived from modification of SBA-15 with CuCl. The sulfur capacity of this adsorbent is 0.123 mmol g−1 with 760 ppmw of sulfur in aromatic oil (Dai et al., 2006). Metallic nickel NPs are supported on mesoporous silica for preparation of Ni/SBA-15. This adsorbent could capture 0.053 mmol g−1 of sulfur with diesel containing 240 ppmw of sulfur (Park et al., 2008). These results indicate that the present 36CeO2-ASS adsorbent is highly competitive for application in adsorptive desulfurization. Adsorption–desorption cycles for the 36CeO2-ASS sample were tested according to a reported method (Oliveira et al., 2009; Rodrigues et al., 2014; Vilarrasa-Garcia et al., 2011a). Figure S3 shows the results that three cycles of adsorption and desorption could be achieved by use of this reported method.
Breakthrough curves of thiophene in a fixed-bed adsorber with SBA-15, CeO2-ASS, and CeO2-TFS samples. ASS: as-synthesized SBA-15; TFS: template-free SBA-15.
We have noticed that with the introduction of CeO2 in SBA-15, the sulfur capacities of the CeO2-ASS and CeO2-TFS samples are much higher than SBA-15. There are a number of studies which indicate that Ce(IV), with the valence electronic configuration 4f05d06s0, has high positive charge and polarizability. Sulfur compounds can be adsorbed over Ce(IV) by a direct S–M interaction (Wang et al., 2009a). The IR spectrum of the 36CeO2-ASS sample adsorption with model fuel was recorded (Figure S4). After adsorption with model fuel, the new bands at ∼3000 cm−1 could contribute to the interaction between the 36CeO2-ASS sample and sulfur via the direct S–M interaction. Thus, the enhanced performances of CeO2-ASS and CeO2-TFS over SBA-15 can contribute to the modified CeO2 species, which form S–M bonds with thiophene. It should be further pointed out that the CeO2-ASS samples show better desulfurization performances than CeO2-TFS. The aforementioned results indicate that CeO2 NPs in the CeO2-ASS samples have better dispersion status than in CeO2-TFS. Taken together, these results suggest that the desulfurization performances of the samples are consistent with the dispersion status of CeO2 NPs. In other words, high dispersion of CeO2 NPs is in favor of better performance on desulfurization.
Conclusions
In conclusion, with the introduction of Ce(NO3)2 into ASS, high dispersion of CeO2 NPs can be obtained (CeO2-ASS). The particle sizes of the CeO2 NPs are in control of 4.4–6.3 nm in the CeO2-ASS samples, with the CeO2 content of 12–46 wt%. The high dispersion of CeO2 NPs can be attributed to the ASS with template P123, which provides a confined space for the dispersion of CeO2 NPs. However, the large CeO2 NPs (7.0 nm) are formed for the sample originated from template-free SBA-15 (CeO2-TFS). The high dispersion of CeO2 NPs makes the CeO2-ASS adsorbents better perform on desulfurization than CeO2-TFS.
Footnotes
Declaration of Conflicting Interests
The author(s) declared no potential conflicts of interest with respect to the research, authorship, and/or publication of this article.
Funding
The author(s) disclosed receipt of the following financial support for the research, authorship, and/or publication of this article: National Natural Science Foundation of China (51602133), Natural Science Foundation of Jiangsu Province (BK20160555), China Postdoctoral Science Foundation (2015M581750), Jiangsu Planned Projects for Postdoctoral Research Funds (1501114B), State Key Laboratory of Materials-Oriented Chemical Engineering (KL15-13) are acknowledged for their financial support of this research.
Supplementary Material
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References
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