Article Content
1 Introduction
The World Health Organization (WHO) states that exposure to Hg produces harmful effects on the nervous, digestive, and immune systems, as well as on the lungs and kidneys, all of which may be fatal.[1] The incessant emission from different anthropogenic sources has caused a ubiquitous presence in the environment that has tripled in the last few decades. Hence, the need to reduce mercury emissions and releases into land and water is a matter of urgency. In this regard, different agreements and regulations, such as the Minamata Convention on Mercury, a directive of the European Parliament, the US Environmental Protection Agency, and China’s Emission Standard of Air Pollutant for Thermal Power Plants (GB13223-2011), have been established.[2-5]
The combustion of fossil fuels for energy production is one of the primary anthropogenic sources of mercury emissions (accounting for ≈21% of emissions to the air). Although the demand for coal for energy production has decreased in recent years in European countries, it has increased in Asian countries.[6, 7] Therefore, as reflected in various international programs,[8] controlling mercury emissions from this sector remains a global challenge that must be addressed.
As stated in the literature, with numerous reviews conducted,[9-15] various technologies have been developed to control mercury in coal combustion flue gas. Most methods are actually control technologies designed for other pollutants, such as particulate matter collection units (e.g., electrostatic precipitators or fabric filters), selective catalytic reduction systems for NOx control, and desulfurization units, all of which exhibit a synergistic effect on mercury removal. The only specific technology for controlling elemental mercury (Hg0) is the injection of adsorbents. It must be noted that Hg0 is the most challenging species to capture due to its high volatility and low solubility. This makes its retention particularly difficult compared to other mercury species. The aforementioned adsorption onto solid materials, as well as catalytic oxidation, are the technologies currently gaining the most attention for addressing Hg0 removal.[5, 16-20]
There are numerous studies focused on the development of adsorbents and catalysts for the retention of Hg0 from coal-fired power plants.[21-25] Most adsorbents are modified to improve the surface pore structure and/or increase the concentration of active centers. Those modified with halides (iodine, bromine, and chlorine) and sulfur have been widely studied and have been demonstrated to have strong chemical activity for Hg0, with almost 100% retention efficiency.[26] However, one of the drawbacks of this type of adsorbent is their regeneration and recovery, which can lead to a new source of mercury-contaminated waste. Another relevant group of adsorbents includes those doped with metals (Pd, Pt, Ag, Au, etc.) and metal oxides (MnOx, CuOx, FexOy, etc.), which not only effectively catalyze Hg0 oxidation in flue gases but can also be easily regenerated.[24, 27] In particular, adsorbents based on iron oxides have been widely used due to their high efficiency, low cost, and the potential for regeneration.[28-30]
On the other hand, it is well known that, among other characteristics (temperature, flow rate, etc.), the composition of flue gas significantly affects the activity of adsorbents and catalysts, and numerous studies have been conducted on this matter.[14, 31] SO2 is one of the flue gas components most commonly evaluated for its inhibitory effect on Hg0 removal, acting through the following primary mechanisms: 1) competitive adsorption, 2) consumption of active sites, and 3) formation of sulfates that poison the adsorbent/catalyst.[16, 32, 33] Although various strategies can be implemented to mitigate the inhibitory effect of SO2, such as increasing the number of active sites and suppressing SO2 adsorption,[32] the development of a pore structure optimized to enhance SO2 tolerance has not yet been thoroughly evaluated. The impact on SO2 resistance of the combination of microporosity, mesoporosity, and macroporosity in the texture of adsorbents/catalysts is difficult to assess, as developing materials with a hierarchically controlled pore structure is typically not an easy task.
In this work, a model material was developed to further assess the role of pore structure in SO2 resistance during Hg0 adsorption in coal combustion processes. The goal was not to create a new material for mercury removal but rather to address knowledge gaps in this area from a textural characterization perspective, enabling the application of these insights to other carbon-based adsorbents/catalysts.
2 Results and Discussion
In this study, the results are discussed based on: 1) the retention of mercury by the raw and Fe-loaded carbon materials in a simulated flue gas and 2) the influence of textural characteristics on mercury retention capacity in the presence of SO2.
2.1 Physicochemical Characterization of the Materials Tested
The amount of Fe supported was not quantitative for the organic xerogel (OX) and carbonized material (CX) samples (6–7 wt%) (Table 1). However, for the activated materials (AX), the impregnation efficiency reached up to 85% (17 wt%). Generally, a higher surface area promotes a more quantitative immobilization of Fe on the support (Table 1). However, the surface chemistry of the samples may also influence their interaction with Fe during the immobilization process. Therefore, although the Fe content in the OX and CX samples is similar (6–7 wt%), their performance can be compared in terms of their differing textural properties.
| Fe | S BET | S ext | V micro | V t | ρ He | |
|---|---|---|---|---|---|---|
| [wt%] | [m2 g−1] | [m2 g−1] | [cm3 g−1] | [cm3 g−1] | [g cm−3] | |
| OX | – | 226 | 202 | 0.11 | 0.41 | 1.40 |
| CX | – | 619 | 145 | 0.24 | 0.38 | 1.90 |
| AX | – | 1597 | 509 | 0.63 | 1.03 | 2.00 |
| OXFe(g) | 6.30 | 158 | 143 | 0.06 | 0.27 | 1.44 |
| OXFe(h) | 72 | 66 | 0.03 | 0.25 | 3.04 | |
| CXFe(g) | 6.84 | 523 | 142 | 0.21 | 0.34 | 1.98 |
| CXFe(h) | 585 | 170 | 0.23 | 0.36 | 1.88 | |
| AXFe(g) | 17.1 | 1325 | 442 | 0.51 | 0.89 | 1.93 |
| AXFe(h) | 1462 | 601 | 0.58 | 0.98 | 2.29 |
The sol-gel methodology enables the design of mesopores (i.e., pores between 2 and 50 nm in width), often referred to as feeder pores, during the sol-gel process, while microporosity (i.e., pores <2 nm in width) can be developed independently during postsynthesis treatments. Consequently, the OX, CX, and AX samples exhibit similar mesoporosity, with pores in the 6-8 nm range (Figure S1a, Supporting Information), but they show significant differences in microporosity, as indicated by the volume of N2 adsorbed at low relative pressures (Figure S1b, Supporting Information).
All the supports exhibit type I–IV isotherms according to the IUPAC classification,[34] which are characteristic of micro- and mesoporous samples with a well-defined capillary condensation step at p/p0 above 0.5, which is indicative of a well-developed mesoporosity, consistent with uniform cylindrical mesopores and greater pore connectivity. This is confirmed by the pore size distribution (PSD), which shows that the porosity is made up of uniform mesopores ranging from 2 to 10 nm. The presence of a hysteresis loop also suggests a similar mesoporous structure across the samples. The carbonization process (i.e., heat treatment under an inert atmosphere) removes volatile matter in CX, resulting in the development of microporosity, which is reflected in higher adsorbed volumes at low p/p0 compared to the original polymer OX. The activation process used during the synthesis of AX further enhances this microporosity, as indicated by the increased adsorption at low relative pressures in Figure S2b, Supporting Information. This increase in microporosity contributes to a higher specific surface area (SBET), as summarized in Table 1, following the trend OX < CX < AX (226, 619, and 1597 m2 g−1, respectively).
Incorporation of Fe into these samples partially blocks the pores, leading to a decrease in SBET compared to the pristine samples: 158, 523, and 1325 m2 g−1 for OXFe(g), CXFe(g), and AXFe(g), respectively. A slight increase in the SBET is observed when these samples undergo heat treatment to convert goethite to hematite, as seen in CXFe(h) and AXFe(h). However, this increase is not observed for OXFe(h), where a notable change in morphology occurs. The low thermal stability of the OX sample may induce secondary reactions with the Fe precursors, further blocking the porosity, as indicated by the reduction in both microporosity and SBET. Additionally, the N2 adsorption–desorption isotherm shifts to type II (Figure S2, Supporting Information), indicating the loss of mesopores. Accordingly, OXFe(h) is completely different from OXFe(g), not only in terms of its chemistry but also in porosity of the resultant material, with a denser structure clearly reflected by the increase of helium density and the decrease of the porous characteristics (Table 1).
The morphologies of Fe-impregnated samples were examined using scanning electron microscopy (SEM) (Figure 1). Iron species predominantly appeared as polyhedra and nanorods. However, the distribution of these iron species was more uniform in the CXFe and AXFe samples compared to OXFe (Figure 1a–c). For the OXFe material, a lower surface coverage was observed, with noticeable agglomeration of nanorods forming in certain areas (Figure 1a).

Figure 1
The analysis by X-ray diffraction (XRD) (Figure S3a, Supporting Information) revealed the presence of goethite in the samples synthesized by oxidative hydrolysis (OXFe(g), CXFe(g), and AXFe(g)). The subsequent heat treatment at 300 °C led to the transformation of goethite into hematite (OXFe(h), CXFe(h), and AXFe(h)) (Figure S3b, Supporting Information). Notably, the original polyhedral and nanorod morphologies of the iron species were preserved after this thermal transformation (Figure 1c,d).
As observed in previous studies conducted by the authors,[35] the type of iron species present on the surface of carbon materials significantly impacts mercury adsorption performance. This performance is also influenced by the textural properties of the material and, distinctly, by the presence of SO2.
2.2 Mercury Retention: The Role of Porous Texture
Figure 2 shows the mercury retention capacity alongside the surface area for all the carbon materials studied. As previously discussed, these materials exhibit variable textural characteristics but were designed with hierarchical porosity to enable a comprehensive evaluation of their effects on mercury removal and SO2 resistance. It is worth noting that OX and CX samples have comparable total pore volumes and mesopore sizes but differ in micropore volume, leading to differences in SBET (Table 1). In contrast, the AX samples have a more developed porosity with higher pore volumes across the entire porosity range. The mercury retention capacity varies according to the type of carbon material and the iron species present.

Figure 2
Similar mercury retention capacities (1–2 μg g−1) were observed in the raw materials and the OX sample loaded with iron species (OXFe(g) and OXFe(h)), regardless of their textural properties (Figure 2, Table 1). This suggests that the carbonaceous matrix itself lacks significant activity for mercury capture and serves mainly to provide a support with appropriate porosity for the active phase. Additionally, the limited textural properties of the OXFe samples reduce the accessibility of Fe active sites, leading to low mercury removal activity irrespective of the type of iron species present.
Impregnation of the CX and AX with Fe had a significant impact on Hg capture efficiency, with the highest retention observed in CX and AX samples containing hematite (20 and 21 μg g−1 for CXFe(h) and AXFe(h), respectively). Previous studies have shown that the outer layer of Fe3+ in the iron oxide (αFe2O3), which has an empty orbital structure, enhances the Fe/Hg0 interaction .[36] In fact, earlier research by the authors on carbon foams demonstrated that αFe2O3 enhances mercury capture efficiency compared to other iron oxides and hydroxides under similar conditions.[35] The results obtained in this work corroborate these findings, as both CXFe(h) and AXFe(h) exhibit higher mercury retention values than CXFe(g) and AXFe(g), respectively, reinforcing the role of αFe2O3 in Hg removal.
In terms of textural properties, it is notable that CXFe(h) and AXFe(h) exhibit similar mercury retention capacities, despite CXFe(h) having a considerably smaller surface area than AXFe(h) (Table 1, Figure 2). In contrast, for samples loaded with goethite (CXFe(g) and AXFe(g)), mercury retention is higher in AXFe(g) than in CXFe(g). Both samples have the same iron morphology, characterized by nanorods and polyhedral particles (Figure 1), but AXFe(g) benefits from a more developed microporosity, which likely enhances the availability of active sites and thus contributes to its superior Hg retention.
The results suggest that 1) the formation of αFe2O3 on the surface of carbon materials creates active sites for the chemisorption/oxidation of elemental mercury, but the critical factor is the overall porosity of the material, rather than solely the microporosity, as commonly suggested in most studies carried out so far; and 2) when FeOOH is the iron species, which results in fewer active sites available for Hg0 oxidation,[36] a more developed pore structure with a higher surface area in AXFe(g) compared to CXFe(g) (Table 1) enhances mercury retention (Figure 2). The findings also indicate that a carbonization process alone may suffice, eliminating the need for activation and thus potentially lowering the cost of this technology.
2.3 Mercury Retention: The Role of SO2
Inhibition of mercury capture could occur because carbon material is a catalyst for the oxidation of SO2 to sulfuric acid or through adsorption of SO3 (which can hydrolyze to sulfuric acid), with SOx competing with mercury for the same adsorption sites, specifically the Lewis base sites, on the carbon surface. Two carbon materials with differing pore structures were subjected to varying SO2 concentrations to assess the effect on Hg0 adsorption, specifically focusing on those materials that exhibited the highest mercury retention capacity, that is, those loaded with αFe2O3 (CXFe(h) and AXFe(h)). Figure 3 displays the mercury retention capacity of CXFe(h) and AXFe(h) at different SO2 concentrations, highlighting their contrasting textural properties. For CXFe(h), mercury retention remained relatively stable across the SO2 concentration range. In contrast, AXFe(h), characterized by a more developed porosity, showed a progressive decrease in mercury removal as SO2 concentration increased (Figure 3). This suggests that SO2 competes with Hg0 for surface and lattice oxygen active sites, thereby reducing Hg0 adsorption in the material (M) via the well-known Mars–Maessen mechanism.[35, 37, 38]
()
()
()
()
Figure 3
It is generally assumed that the first step, namely, the physisorption process (I), is favored by a higher surface area, as seen in AXFe(h) (Table 1). However, unlike CXFe(h), a more developed microporosity preferentially promotes the adsorption of SO2 over Hg0 on the same active sites, supporting a mechanism of competitive adsorption between SO2 and Hg0[32] (Figure 3). Therefore, the findings of this study demonstrate that in flue gas atmospheres, an adsorbent with increased microporosity does not necessarily achieve higher Hg retention efficiency or better tolerance to acidic gases like SO2, which is critical for designing a cost-effective technology optimized for mercury capture.
Although evaluating this effect is not the primary objective of this study, as it has already been investigated in various sorbents, it is important to note that hematite active sites may be consumed during retention experiments. However, this deactivation can be counteracted by the presence of O2 in the gas stream, which facilitates the regeneration of the sorbents.[29, 35, 39]
3 Conclusions
The development of a model material with hierarchical porosity enabled an assessment of the impact of textural properties on both Hg capture and SO2 resistance, a task that has proven challenging for most materials studied to date.
The similar total pore volumes in samples OX and CX suggest that this parameter does not play a crucial role in Hg adsorption. The higher Hg removal observed with CX and AX compared to OX supports the idea that a well-developed microporosity enhances Hg retention capacity. However, contrary to common assumptions, microporosity is not the only textural parameter to consider. This is illustrated by the similar retention capacities of CXFe(h) and AXFe(h), highlighting the importance of considering porosity as a whole. It should also be noted that sorbents with more developed porosity were more affected by the presence of SO2.
The comparable mercury retention capacities observed between the CX and the AX also indicate that an activation process, which is more costly and tedious, is not always required. Therefore, the findings of this study not only improve the understanding of the Hg/SO2/texture relationship but also contribute to the development of the best available techniques and the best environmental practices for Hg control in relevant emissions sources, such as coal combustion processes.