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Pd/activated carbon sorbents for mid-temperature capture of mercury from coal-derived fuel gas Dekui Li1 , Jieru Han1 , Lina Han2,⁎, Jiancheng Wang1 , Liping Chang1,⁎ 1. Key Laboratory of Coal Science and Technology, Ministry of Education and Shanxi Province, Taiyuan University of Technology, Taiyuan 030024, China 2. College of Materials Science and Engineering, Taiyuan University of Technology, Taiyuan 030024, China
AR TIC LE I N FO
ABS TR ACT
Article history:
Higher concentrations of Hg can be emitted from coal pyrolysis or gasification than from
Received 6 August 2013
coal combustion, especially elemental Hg. Highly efficient Hg removal technology from
Revised 20 November 2013
coal-derived fuel gas is thus of great importance. Based on the very excellent Hg removal
Accepted 28 January 2014
ability of Pd and the high adsorption abilities of activated carbon (AC) for H2S and Hg, a
Available online 12 June 2014
series of Pd/AC sorbents was prepared by using pore volume impregnation, and their
Keywords:
laboratory-scale fixed-bed reactor. The effects of loading amount, reaction temperature and
Coal-derived fuel gas
reaction atmosphere on Hg removal from coal-derived fuel gas were studied. The sorbents
performance in capturing Hg and H2S from coal-derived fuel gas was investigated using a
Hg removal
were characterized by N2 adsorption, X-ray diffraction (XRD) and X-ray photoelectron
Pd/AC sorbents
spectroscopy (XPS). The results indicated that the efficiency of Hg removal increased with
H2S removal
the increasing of Pd loading amount, but the effective utilization rate of the active component Pd decreased significantly at the same time. High temperature had a negative influence on the Hg removal. The efficiency of Hg removal in the N2–H2S–H2–CO–Hg atmosphere (simulated coal gas) was higher than that in N2–H2S–Hg and N2–Hg atmospheres, which showed that H2 and CO, with their reducing capacity, could benefit promote the removal of Hg. The XPS results suggested that there were two different ways of capturing Hg over sorbents in N2–H2S–Hg and N2–Hg atmospheres. © 2014 The Research Center for Eco-Environmental Sciences, Chinese Academy of Sciences. Published by Elsevier B.V.
Introduction During the combustion and gasification of coal, mercury can be mostly emitted into the vapor phase. Mercury can travel a long distance and is easily accumulated in the organisms. Once Hg is converted into methylmercury by bacteria in the sediments, it enters the food chain and becomes hazardous to wildlife and humans (Otero-Rey et al., 2003). It has been reported that more amounts and higher concentrations of elemental Hg can be emitted from coal pyrolysis or gasification than that from coal combustion (Yan et al., 2004). There are three forms of mercury that may be present in the coal-derived fuel or flue gas, namely, elemental mercury (Hg0), oxidized mercury (Hg2+, Hg+) and
particle-bound-mercury (HgP) (Presto and Granite, 2006). Oxidized mercury can be removed by wet flue gas desulfurization (WFGD) facilities, and particle-bound-mercury can be captured along with fly ash by the typical air pollution control devices (APCD) such as electrostatic precipitators and bag houses (Yan et al., 2005, 2011). However, elemental mercury (Hg0 ) vapor is very difficult to capture with typical APCD because Hg is highly volatile and insoluble in water (Ozaki et al., 2008). Coal gasification is the leading technology in clean coal conversion and will be widely used in the next ten or twenty years (Pavlish et al., 2010). Therefore, highly efficient Hg control technology, especially for coal gasification, is of great importance.
⁎ Corresponding authors. E-mails:
[email protected] (Lina Han);
[email protected] (Liping Chang).
http://dx.doi.org/10.1016/j.jes.2014.05.016 1001-0742/© 2014 The Research Center for Eco-Environmental Sciences, Chinese Academy of Sciences. Published by Elsevier B.V.
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Recently, some researchers found that several noble metals, such as Ag, Au, Pd and Pt, etc. showed high Hg0 removal efficiency in the mid-temperature range of 150–350°C (Baltrus et al., 2008; Granite et al., 2006). Among these metal-based sorbents, Pd showed the highest removal ability of Hg0 according to modeling and experimental results (Granite et al., 2006). Moreover, Pd supported on Al2O3 can capture Hg at mid-temperatures (Han et al., 2012). As we know, the content of H2S, another harmful gas generated during the coal gasification process (Liu et al., 1998), is several orders of magnitude higher than that of mercury. It has been reported that H2S has a negative effect on the capture of Hg over Pd/Al2O3 sorbents (Han et al., 2012). Activated carbon (AC) can be used as a catalyst support due to the abundant pore structure and large BET surface area. Furthermore, it also possesses high adsorption abilities (Shen et al., 2010; Bandosz, 2002; Murakami et al., 2010). It has been reported that AC, as well as AC impregnated with sulfur, chlorine and iodine, and active metal oxides, was effective for Hg removal (Baltrus et al., 2011; Feng et al., 2006; Kamakoti et al., 2005; Poulston et al., 2007; Hu et al., 2010; Sun et al., 2013). In this work, Pd and AC were selected as the active metal and support, respectively. Pd/AC sorbents were prepared by pore volume impregnation and the removal of Hg and H2S from simulated coal gas was investigated using a laboratory-scale fixed-bed reactor. N2 adsorption, X-ray diffraction (XRD), transmission electron microscopy (TEM) and X-ray photoelectron spectroscopy (XPS) characteristic technologies were used to analyze the physical and chemical properties of the fresh and used sorbents, and a possible approach to capture Hg over Pd/AC sorbents was discussed.
1. Experimental
500°C for 5 hr. The 0.5Pd/AC, 1Pd/AC and 3Pd/AC sorbents were prepared by loading 0.5 wt.%, 1.0 wt.%, 3.0 wt.% Pd on the AC, respectively.
1.2. Adsorption test The adsorption tests were carried out using a fixed-bed quartz flow reactor at atmospheric pressure (Fig. 1). The test apparatus includes five sections: gas system, Hg generating device, fixed bed reactor and online mercury analyzer (Lumex-Marketing JSC, Russia) as the detection system. The Hg generator consists of a mercury permeation tube (Valco Instruments Company Inc., Houston, TX, USA) placed in a constant water bath system at 40°C. Hg vapor was brought into the reactor using ultra high purity N2 as a carrier. The flow rate of each gas stream was accurately controlled by the mass flow controller. Sorbents (0.50 g) were placed in a quartz tube reactor (5.0 mm inner diameter and 64.2 cm length). The gas flow rate was 470 mL/min and was controlled by a mass flow controller where the space velocity was 4.5 × 104/hr. The simulated coal gas included 10% H2 (when used), 20% CO (when used), 300 ppm H2S and N2 as a balance gas. The initial concentration of mercury was 40 ± 3 μg/m3. The contents of Hg vapor and H2S in the inlet and outlet gases of the reactor could be monitored using the mercury analyzer and gas chromatograph with a flame photometry detector, respectively. The removal efficiency (η) of Hg or H2S and Hg content (Q) was used to evaluate the performance of the prepared sorbents capturing Hg or H2S from simulated coal gas. Q and η were calculated using the following formulas
1.1. Sample preparation A commercial coal-based AC was selected as the carrier, in the form of pellets with diameters of 0.25–0.38 mm. A series of sorbents were prepared by pore volume impregnation using palladium nitrate as the precursor. After the impregnation, the sorbents were air-dried at room temperature for 10 hr, and then dried at 100°C for 12 hr, and lastly, calcined in N2 at
η ¼ ðn0 −n1 Þ=n0 100%
ð1Þ
Q ¼ m1 =m0
ð2Þ 3
3
where, n0 (μg/m or ppm) and n1 (μg/m or ppm), are the concentrations of Hg or H2S in the feed and effluent gases, respectively, and m1 (mg) and m0 (g) are the quantities of Hg
Furnace Catalyst
N2
H2S LUMEX/RA915M Mercury analyzer Heating tape CO
Computer
GC950 H2 Activated carbon
N2
Absorber
Mass flowmeter Water bath
Mercury permeation tube
Fig. 1 – Schematic diagram of adsorption apparatus for removing Hg and H2S.
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captured by sorbents and the quality of fresh sorbents, respectively.
1.3. Sample characterization The BET surface area, pore size and pore volume of sorbents were measured by BET analysis (TriStar 3000, Micromeritics Instrument Corporation, China) using N2 adsorption at −196°C. The samples were initially purged at 150°C for 3 hr before adsorption. XRD was employed to investigate the crystal structures of the sorbents. The instrument was a Rigaku D/max2500 diffractometer, fitted with a nickel-filtered Cu Kα radiation source operating at a voltage of 40 kV and 100 mA. The scan rate was 8°/min at the range from 5 to 85°. XPS surface analysis was conducted to determine the surface concentration and binding energy of samples, using an ESCALAB 250 spectrometer (VG Scientific Ltd., UK) equipped with an Al Kα source (hγ = 1486.6 eV, 150 W). Energy correction was performed using the C1s peak at 284.6 eV. No smoothing routine of data was applied to analyze the results. The crystalline phases of samples were measured by high resolution TEM at room temperature with a JEM-2010 microscope operating at 200 kV.
2. Results and discussion 2.1. Effect of Pd loading amount and dispersion on Hg removal Fig. 2 shows the removal efficiency of Hg and H2S over the Pd/ AC sorbents with different Pd loading amounts. At 250°C, the initial efficiency of Hg removal over 0.5Pd/AC, 1Pd/AC and 3Pd/AC sorbents was about 89%, 93% and 94%, respectively. The efficiency of Hg removal over the 3Pd/AC sorbent remained at around 95% over 150 min. That of 0.5Pd/AC and 1Pd/AC sorbents showed a decrease, reducing to 20% and 65% after 150 min, respectively. It is obvious that the efficiency of
Hg removal increased with the increasing of Pd loading amount on the sorbent. The 3Pd/AC sorbent was selected and the mercury balance was evaluated. The total amount of mercury at the inlet was 3.38 μg during the reaction time in N2–Hg–H2S atmosphere at 250°C (40 μg/m3 Hg, 300 ppm H2S in N2, and SV = 4.5 × 104/hr). The mercury adsorbed and catalytic oxidation by sorbents (calculated by Hg content of sorbents) was 2.42 μg. The amount of mercury at the output was 0.17 μg. Because the mercury analyzer can only detect Hg0, the remaining 0.79 μg mercury should be in the form of Hg2+. Fortunately, Hg2+ can be efficiently removed by WFGD facilities, as it is soluble in most aqueous solutions (Ozaki et al., 2008). The Hg content (Q) of the sorbent and the mercury amount adsorbed per mole of Pd (Hg/Pd) are shown in Table 1. For example, the Hg content of 0.5Pd/AC was 3.85 mg Hg/1000 g sorbent at 250°C, with the ratio of Hg/Pd at 0.49 mmol/mol. Although the Hg content of 3Pd/AC was the highest among the three sorbents, the Hg/Pd ratio of the 3Pd/AC sorbent was much lower than the 1Pd/AC and 0.5Pd/AC sorbents. This indicated that the dispersion of Pd on the surface of 0.5Pd/AC and 1Pd/AC was better and their effective utilization rate of Pd was also higher than that of 3Pd/AC. It is suggested that both the dispersion and the loading amount of Pd contribute to the efficiency of Hg removal over the Pd/AC sorbent. There was good dispersion of Pd over the 0.5Pd/AC sorbent, but the active sites were limited compared to the 1Pd/AC and 3Pd/AC sorbents. On the other hand, the Hg/Pd ratio can partly reflect the utilization efficiency of Pd over the Pd/AC sorbents. Fig. 3 shows the TEM images of the Pd/AC sorbents with different Pd loading amounts. It can be found that the Pd loading amount affected the dispersion of Pd and it became slightly worse as the Pd loading amount increased. Therefore, the 1Pd/AC sorbent was selected for the next experiments, considering the effective utilization rate of Pd, the loading amount and the efficiency of Hg removal. The influence of the Pd loading amount on the H2S removal efficiency at 250°C is also presented in Fig. 2. It was
100
H2S removal efficiency (%)
Hg removal efficiency (%)
100
80
60
40
0.5Pd/AC 1Pd/AC/AC 3Pd/AC/AC
20
0
20
40
60
80
60
40 0.5% Pd/AC 1% Pd/AC 3% Pd/AC
20
80
100
Time (min)
120
140
160
0
30
60
90
120
150
180
210
240
Time (min)
Fig. 2 – Efficiency of Hg (left) and H2S (right) removal over 0.5Pd/AC, 1Pd/AC and 3Pd/AC sorbents in N2–Hg–H2S atmosphere at 250°C. Reaction conditions: 40 μg/m3 Hg, 300 ppm H2S in N2, and SV = 4.5 × 104/hr.
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Table 1 – Hg content of sorbents with different Pd loading amounts. Samples
Temperature (°C)
Hg content (Q) (mg Hg/1000 g sorbent)
Hg/Pd (mmol/mol)
0.5Pd/AC 1Pd/AC 3Pd/AC
250 250 250
3.85 4.29 4.84
0.49 0.23 0.09
AC: activated carbon
found that all of the desulfurization efficiency over the three sorbents can be maintained at above 85% for 4 hr at 250°C. The 3Pd/AC sorbent did not show very good desulfurization activity, which suggests that the Pd loading amount has no obvious influence on the H2S removal efficiency.
2.2. Effect of the temperature on the removal of Hg and H2S over sorbents The effect of the temperature on the removal efficiency of Hg and H2S over 1Pd/AC was evaluated at the temperatures of 250, 300 and 350°C, and the results are shown in Fig. 4. At 250°C, the Hg removal efficiency over the 1Pd/AC sorbents could reach 92% and maintain a relatively high efficiency of 68% within 150 min. When the reaction temperature rose to 350°C, the Hg removal efficiency sharply dropped to 14% and was only 1% after 130 min. The results indicated that high temperatures had a negative effect on the efficiency for Hg removal. Pd (mainly Pd0 from Section 2.4) loaded on AC could form amalgams with mercury (Granite and Pennline, 2002; Granite et al., 2000). The decrease of the solubility of Hg in Pd with the increasing temperature and the de-amalgamation at high temperatures were possible reasons for the decrease of Hg removal efficiency from 250 to 350°C (Poulston et al., 2007). The H2S adsorption curves of the 1Pd/AC sorbent at different temperatures are also presented in Fig. 4. It was found that the change of H2S removal efficiency with temperature was different from that of Hg, increasing slightly from 250 to 350°C.
2.3. Effect of H2 and CO atmosphere on the removal of Hg over sorbent The curves of the Hg removal efficiency over the 1Pd/AC sorbent in different atmospheres at 250°C are shown in Fig. 5. It was found that the efficiency for Hg removal over the 1Pd/ AC sorbent in N2–Hg atmosphere at 250°C could be maintained above 80% for at least 300 min. However, in N2–H2S–Hg
a
50 nm
b
50 nm
atmosphere, the efficiency of Hg removal reached over 90% but only for the first 50 min, then decreased to 68%. Moreover, in N2–H2S–H2–CO–Hg atmosphere, the efficiency of Hg removal over the 1Pd/AC sorbent could be maintained above 92% for at least 360 min. These results indicated that Hg removal efficiency over 1Pd/AC can be clearly improved when CO, H2 and H2S exist simultaneously. H2S is known as a poison for Pd (Castro et al., 2002) in N2–H2S–Hg atmosphere. The reason may be that the PdO (in Section 2.4) on the surface of 1Pd/AC sorbent can be significantly converted to PdS, which is difficult to reduce to element Pd (Pd0 is the main active component of Hg removal). PdO was more easily reduced to elemental Pd in N2–H2S–H2–CO–Hg atmosphere. The efficiency of Hg capture can be promoted in the reducing gas (Yu and Shaw, 1998), due to the formation of the Pd–Hg alloy. This result showed that the Pd/AC sorbents have a high potential as a candidate for capturing Hg in the presence of H2S from coal-derived fuel gas, which contains CO, H2, H2S and other gases.
2.4. Characteristics of physical and chemical properties of sorbents The physical properties of the AC support and the Pd/AC sorbents including the BET surface area, the pore volume and the pore diameters are summarized in Table 2. Generally, the surface characteristics of all sorbents were similar, which means physical characteristics are not the main factor in Hg removal. Fig. 6 shows the XRD patterns of 0.5Pd/AC, 1Pd/AC and 3Pd/ AC sorbents before and after the reaction. Representative diffraction peaks of Pd (2θ = 40.1, 46.2, 67.8, 82.0°) were found from the sorbents (Lineberry et al., 2009). These results showed that the active component of the sorbents was mainly elemental Pd, except for the 0.5Pd/AC sorbent due to the relatively low loading amount and the high dispersion of Pd over the AC support. There were no peaks for palladium oxide observed for any of the sorbents. This may be the result of the
c
50 nm
Fig. 3 – TEM of the Pd/AC sorbents with different Pd loading amount. (a) 0.5Pd/AC; (b) 1Pd/AC; (c) 3Pd/AC sorbents.
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1Pd/AC 250°C
1Pd/AC 300°C
1Pd/AC 350°C
H2S removal efficiency (%)
Hg removal efficiency (%)
100 80
60
40
20
0
20
40
60
80
100
120
140
160
80
60
40
20
0
30
60
Time (min)
90
120
150
Time (min)
Fig. 4 – Efficiency of Hg and H2S removal over 1Pd/AC sorbent in N2–Hg–H2S atmosphere at different temperatures. Reaction conditions: 40 μg/m3 Hg, 300 ppm H2S in N2, and SV = 4.5 × 104/hr.
palladium oxide being amorphous, or having low crystallinity (Baltrus et al., 2011). This result differed from that of the Pd/ Al2O3 sorbents in our previous work, whose active component was mainly PdO (Han et al., 2012). The intensity of Pd characteristic peaks of used sorbents became notably smaller compared with the fresh sorbents. In particular, the Pd diffraction peak at 2θ = 46.2° of used 3Pd/AC sorbent disappeared and the intensities of peaks at 2θ = 40.1, 67.8, and 82.0° were clearly smaller than that of the fresh 3Pd/AC sorbent. Similar results can be found from the XRD patterns of the 1Pd/ AC sorbent. It is possible that the consumption of Pd in the reaction resulted in the decrease of the Pd peak intensities. The Pd diffraction peaks at 2θ = 40.1 and 67.8° of the used 1Pd/ AC sorbent were also weakened. Thus, it is suggested that elemental Pd should be the main active component of the Pd/ AC sorbents for the capture of Hg and H2S.
100
Hg removal efficiency (%)
90 80 70 60 50 40
XPS analysis of the fresh and used 1Pd/AC sorbent in N2–Hg and N2–Hg–H2S atmospheres was performed in order to obtain more information about the mechanism of the Hg capture over the Pd/AC sorbents. The Pd 3d XPS patterns are given in Fig. 7a. It can be seen that the binding energies (BEs) 335.3 eV of Pd 3d5/2 and 340.4 eV of Pd 3d3/2 of the fresh 1Pd/AC sorbent correspond to Pd0, which is in agreement with the results of the XRD patterns of the fresh 1Pd/AC sorbent. After capturing Hg in N2–Hg–H2S atmosphere, the BEs 336.9 and 342.1 eV of Pd 3d3/2 of the used 1Pd/AC sorbent were assigned to Pd2+ species. There were also Pd0 characteristic peaks, although the intensity was notably lower compared with Pd2+. After capturing Hg in N2–Hg atmosphere, there was more Pd0 than Pd2+ species on the surface of the sorbents. This indicated that there are different mechanisms of the Hg removal over the Pd/ AC sorbent in the two kinds of atmospheres. The Hg4f XPS patterns are shown in Fig. 7b. In N2–Hg–H2S atmosphere, the BE 101.6 eV of Hg4f7/2 of the 1Pd/AC sorbent was assigned to Hg0, and 103.4 eV of Hg4f 7/2 was assigned to Hg2+. In N2–Hg atmosphere, it can be found that Hg0 and Hg2+ also occurred. Moreover, Hg0 was the main component on the surface of the used sorbents after the capturing of Hg in N2–Hg atmosphere, while Hg2+ was the main component on the surface of the used sorbents in N2–Hg–H2S atmosphere. These results indicated that there are obviously different reaction
30
N2+Hg N2+H2S+Hg N2+H2S+H2+CO+Hg
20 10
Table 2 – Physical properties of the AC support and the Pd/ AC sorbents.
0 0
50
100
150
200
250
300
Time (min) Fig. 5 – Efficiency of Hg removal over 1Pd/AC sorbent in different atmospheres at 250°C. Reaction conditions: 40 μg/m3 Hg, 300 ppm H2S, 10% H2, 20% CO in N2, and SV = 4.5 × 104/hr.
Samples
BET surface area (m2/g)
Pore volume (cm3/g)
Average pore diameter (nm)
AC 0.5Pd/AC 1Pd/AC 3Pd/AC
915.56 879.43 926.48 899.50
0.51 0.49 0.52 0.51
2.39 2.29 2.44 2.47
350
AC: activated carbon
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C
Pd
Pd
Relative intensity (a.u.)
Pd
c1 c b1 b a1 a 20
30
40
50
60
70
80
90
2θ (°) Fig. 6 – XRD spectra of sorbents before and after the reaction. Line a, b, c: fresh 0.5 Pd/AC, 1Pd/AC and 3 Pd/AC sorbents; line a1, b1, c1: the sorbents after reaction in N2–Hg–H2S atmosphere at 250°C.
336.9
342.1 Pd 3d
340.4
335.3
in N2-Hg-H2S
101.9
b
103.4
Hg 4f
in N2-Hg-H2S
Intensity (a.u.)
Intensity (a.u.)
a
mechanisms of Hg removal with and without H2S in the reaction atmosphere. The C1s XPS patterns are shown in Fig. 7c. The C1s BEs at 284.8, 286.3, 287.5, 288.87 eV of the fresh 1Pd/AC sorbent corresponded to C\C, C\O, C_O, COO, respectively (Xu et al., 2013). It is noted that the peak intensities of these oxygencontaining groups become weak after the capture of Hg in N2– Hg–H2S atmosphere, in particular, the peaks of C_O and COO almost disappear. It is possible that these oxygen-containing groups take part in the reaction to oxidize Pd0 into Pd2+ (PdO). The S2p XPS pattern is shown in Fig. 7d. The BEs 163.36 eV and 162.02 eV of S2p of the used 1Pd/AC sorbent corresponded to the formation of HgS and PdS in N2–Hg–H2S atmosphere (Baltrus et al., 2008; Zylberajch-Antoine et al., 1991), respectively. Therefore, it can be deduced that there are two ways of capturing Hg over the Pd/AC sorbents in N2–Hg–H2S atmosphere. On the one hand, a part of Hg can react with Pd0 on the surface of sorbents to produce Hg–Pd amalgam (Poulston, et al., 2007). On the other hand, the oxygen-containing groups of the AC can oxidize Pd0 to Pd2+ (PdO), and the PdO may react with H2S and Hg to form PdS and Hg2+ (HgS). It can also be deduced from the above XPS analysis that H2S competes with
in N2-Hg
in N2-Hg fresh 330
332
334
336
338
340
342
344
98
100
102
Binding energy (eV) 284.8
c
104
106
Binding energy (eV)
d
C 1s
S 2p
286.3
Intensity (a.u.)
Intensity (a.u.)
163.36 in N2-Hg-H2S
287.5 fresh
282
284
286
288
Binding energy (eV)
162.02
in N2-Hg-H2S
288.87
290
167
166
165
164
163
162
161
Binding energy (eV)
Fig. 7 – XPS spectra of the fresh and used 1Pd/AC sorbents over the spectral regions of Pd3d (a), Hg4f (b), C1s (c) and S2p (d).
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Pd
C=O COO
Pd Pd
Hg
S H 2 PdS PdO
Hg
Hg2+
Pd-Hg
Fig. 8 – Diagram of the reaction approach of capturing Hg over Pd/AC sorbent in N2–Hg–H2S atmosphere.
Hg on Pd active sites of sorbents in N2–Hg–H2S atmosphere. H2S can react with PdO to generate PdS, which is difficult to be reduced to elemental Pd in N2–Hg–H2S atmosphere. Therefore, H2S has a negative effect on the removal of Hg. A diagram is given to clearly display the reaction approach of capturing Hg over the Pd/AC sorbents in N2–Hg–H2S atmosphere (Fig. 8).
3. Conclusions The performance of Hg and H2S capture over Pd/AC sorbents and the effects of the Pd loading amount, reaction temperature and reaction atmosphere were studied. The Pd/AC sorbents showed an excellent adsorption activity for the Hg and H2S removal from coal-derived fuel gas. The efficiency of Hg removal increased with the increasing of Pd loading amount on the sorbents, but the effective utilization of Pd gradually decreased at the same time. High temperature was not benefit of the Hg removal, but it was conducive to desulfurization. The addition of CO and H2 in atmospheres can promote the removal efficiency of Hg removal, and prevent H2S poisoning of the sorbents due to the formation of PdS. Pd0 was the main active component of the Pd/AC sorbents for the removal of Hg. It can be deduced from the XPS results that there are two ways of capturing Hg over the sorbents in N2–Hg–H2S atmosphere. One way is a part of Hg reacting with Pd0 on the surface of the sorbents to produce Hg–Pd amalgam. Another way is via Pd0 oxidized by the containing-oxygen groups on the AC to form Pd2+ (PdO), which reacts with H2S and Hg to form PdS and Hg2+ (HgS).
Acknowledgments This work was supported by the National Natural Science Foundation of China (Nos. 21006067, 21276170), the Shanxi Province Natural Science Foundation (Nos. 2010021008-1, 201101008-4) and the National High-Tech Research and Development Program (863) of China (No. 2013AA065404E).
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