 Open Access Article
 Open Access Article
      
        
          
            Jingya 
            Pang
          
        
      ab, 
      
        
          
            Huixin 
            Qiu
          
        
      c, 
      
        
          
            Scott 
            Berggren
          
        
      d, 
      
        
          
            Himanshu 
            Tanvar
          
        
      e, 
      
        
          
            Brajendra 
            Mishra
          
        
      e and 
      
        
          
            Maricor J. 
            Arlos
          
        
      *ab
      
aDepartment of Civil and Environmental Engineering, University of Alberta, 9211-116 St. NW, Edmonton, Alberta T6G 1H9, Canada
      
bDepartment of Civil and Environmental Engineering, University of Waterloo, 200 University Avenue West, Waterloo, Ontario N2L 3G1, Canada. E-mail: mjarlos@uwaterloo.ca
      
cDepartment of Food Science & Technology, National University of Singapore, 2 Science Drive 2, Singapore 117542, Singapore
      
dGRÖN Holding Corporation, 40 King St. West, Suite 5800, Toronto, Ontario M5H 3S1, Canada
      
eMaterial Science and Engineering, Worcester Polytechnic Institute, Worcester, MA 01609, USA
    
First published on 26th September 2025
Per- and polyfluoroalkyl substances (PFAS) are synthetic organic compounds characterized by strong C–F bonds and various functional groups, which contribute to their persistence and mobility in the aquatic environment. Bauxite residue (or red mud) is a highly alkaline waste from the aluminum industry, often stored in large quantities in tailing ponds. Recently, growing interest in sustainable waste management has highlighted the potential of bauxite residue to remove organic pollutants from water. This study investigates the use of activated bauxite residue (ABR) (produced via a reduction roasting process) as an adsorbent for a mixture of 10 PFAS substances in water. Bench-scale testing demonstrated that long-chain PFAS can be effectively removed by ABR (up to 100%) whereas the short-chain ones achieved 20–100% removal. PFAS removal using ABR follows a pseudo-second-order kinetic model, indicating that chemisorption may play a role during adsorption. This is further supported by the XPS analysis that shows the presence of metal–F bond. Isotherm study further indicated that at its current material characteristics (pore volume = 0.14 cm3 g−1, BET surface area = 25 g m−2, point of zero charge of ∼pH 5), high dosage of ABR (∼10 g L−1) is required to reach >85% removal for ∑PFAS (n = 10). Cytotoxicity results supported the use of <10 g L−1 ABR to minimize ABR toxicity and maximize PFAS removal. Although further material optimization is needed to lower dosage requirements and improve competitiveness with established adsorbents (e.g., powdered activated carbon), our preliminary results highlight the potential of ABR as a promising sorbent for PFAS removal.
| Environmental significanceActivated bauxite residue (ABR) is a waste material from aluminum industry which can be repurposed as an adsorbent to remove organic pollutants from water (i.e., promoting circular resource use). Here, we assessed the use of ABR to remove a mixture of per- and polyfluoroalkyl substances (PFAS), a diverse group of persistent and bioaccumulative chemicals that are challenging to remediate. We observed that ABR can remove PFAS (especially the long-chain ones) without introducing relevant toxicity by ensuring operation is at neutral pH. This study indicates that ABR is a promising solution to remove PFAS from the water column, offering opportunities to re-use waste materials. Further material improvements and pilot-scale testing are needed to enhance ABR adsorption performance. | 
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 tons.4 Although PFAS are essential components in many products, they are hard to remove from or decompose in the environment5 due to their amphiphilic and stable characteristics.6,7 Given their potential to impact human health, many jurisdictions have implemented guidance/regulation for PFAS levels in drinking water.1,6,8,9 PFAS remain highly recalcitrant to existing wastewater treatment technologies,10 with precursors transforming into PFAS after biological treatments.11,12 Adsorption has been regarded as effective for PFAS removal,13,14 and many conventional and novel adsorbents have been evaluated for their efficiency in removing PFAS from the water column at bench- and pilot-scales.15–18
000 tons.4 Although PFAS are essential components in many products, they are hard to remove from or decompose in the environment5 due to their amphiphilic and stable characteristics.6,7 Given their potential to impact human health, many jurisdictions have implemented guidance/regulation for PFAS levels in drinking water.1,6,8,9 PFAS remain highly recalcitrant to existing wastewater treatment technologies,10 with precursors transforming into PFAS after biological treatments.11,12 Adsorption has been regarded as effective for PFAS removal,13,14 and many conventional and novel adsorbents have been evaluated for their efficiency in removing PFAS from the water column at bench- and pilot-scales.15–18
      Generated as a by-product from alumina extraction,19,20 bauxite residue (red mud) has attracted increasing attention in waste reuse due to its high abundance, with approximately 1–2.5 tonnes of bauxite residue produced per tonne of alumina19 and a global generation of ∼150 million tonnes per year.21 This waste material has a low utilization rate (<5% worldwide)22 mainly due to its potentially hazardous properties, including highly alkaline pH (pH 10–13 (ref. 23)) and risk of metal leaching.24 Much research has focused on exploiting its recovery and reuse values in construction (bricks, tiles), road aggregates, and pigments.19,20 Due to its small particle size (diameter of 5–75 μm for about 90% of the particles), high specific surface area and high chemical reactivity,25 bauxite residue has also been tested as an adsorbent to remove a wide variety of wastewater pollutants such as dyes, phenols, and nutrients.25–29
Others have modified bauxite residue to further improve its adsorbent properties (e.g., thermal treatment, acid treatment).30,31 Using the approach developed by our research team,32 bauxite residue underwent physiochemical modification via a solid-state reduction roasting process, leading to enhanced adsorption capacity and minimal toxic metal leaching potential. This work further demonstrated that this activated bauxite residue (ABR) is capable of removing acid-extractable organics (AEOs) from oil sands process-affected water (OSPW) and other constituents of primary, secondary and tertiary treated municipal wastewater.28
The main objective of this study is to evaluate the potential of ABR for removing PFAS from water. The ABR properties were first characterized using several material characterization techniques to gain insights into its adsorption behaviour. A series of bench-scale experiments were then completed to evaluate its performance (adsorption kinetics and isotherms) in removing 11 PFAS (long/short-chain, sulfonic/carboxylic) in environmentally relevant mixtures. Given the potential for ABR to introduce toxicity, cytotoxicity was monitored throughout the experiments to assess potential mitigation options should it be found to contribute to toxicity. The performance of ABR was compared with a commercially available powdered activated carbon (PAC) as a benchmark of ABR's treatment efficiency.
| Full name – short (S) or long (L) chain | Abb | Chemical formula | MW (g mol−1) | pKa (strongest) | Solubility (pH = 7) (g L−1) | Concentration applied | 
|---|---|---|---|---|---|---|
| a Use in the following experiments: removal efficiency of powdered activated carbon (PAC). b Removal efficiency at different dosages and exposure duration. c XPS. d Zeta potential. e Adsorption kinetics and isotherm. f Cytotoxicity test. g EDX. h BET surface area analysis. | ||||||
| Perfluorobutanoic – S | PFBA | C4HF7O2 | 214.04 | 0.37 | 214.039 | 500 ng L−1a, 600 ng L−1b, 100 μg L−1c,d,e,f, 100 mg L−1c,g | 
| Perfluoropentanoic – S | PFPeA | C5HF9O2 | 264.05 | 0.34 | 264.047 | 500 ng L−1a, 600 ng L−1b, 100 μg L−1c,d,e,f, 100 mg L−1c,g | 
| Perfluorohexanoic – S | PFHxA | C6HF11O2 | 314.05 | 0.32 | 314.05 | 500 ng L−1a, 600 ng L−1b, 100 μg L−1c,d,e,f, 100 mg L−1c,g | 
| Perfluoroheptanoic – S | PFHpA | C7HF13O2 | 364.06 | 0.31 | 364.062 | 500 ng L−1a, 600 ng L−1b, 100 μg L−1c,d,e,f, 100 mg L−1c,g | 
| Perfluorooctanoic – L | PFOA | C8HF15O2 | 414.07 | 0.30 | 414.07 | 500 ng L−1a, 600 ng L−1b, 100 μg L−1c,d,e,f, 100 mg L−1c,g | 
| Perfluorononanoic – L | PFNA | C9HF17O2 | 464.08 | 0.29 | 262.6829 | 500 ng L−1a, 600 ng L−1b, 100 μg L−1c,d,e,f, 100 mg L−1c,g,h | 
| Perfluorodecanoic – L | PFDA | C10HF19O2 | 514.08 | 0.4 | 44.521 | 500 ng L−1a, 600 ng L−1b, 100 μg L−1c,d,e,f, 100 mg L−1c,g | 
| Perfluoroundecanoic – L | PFUnA | C11HF21O2 | 564.09 | 0.4 | 10.3686 | 500 ng L−1a, 600 ng L−1b, 100 μg L−1c,d,e,f, 100 mg L−1c,g | 
| Perfluorotetradecanoic – L | PFTEDA | C14HF27O2 | 714.11 | 0.4 | 0.2194 | 500 ng L−1a, 600 ng L−1b, 100 μg L−1c,d,e,f, 100 mg L−1c,g | 
| Perfluorobutanesulfonic – S | PFBS | C4HF9O3S | 300.1 | −3.31 | 300.09 | 500 ng L−1a, 600 ng L−1b, 100 μg L−1c,d,e,f, 100 mg L−1c,g | 
| 6 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 Fluorotelomer sulfonic – L | 6 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 PTSA | C8H5F13O3S | 428.16 | −2.72 | 428.16 | 100 mg L−1h | 
The porosity of ABR was investigated through the Brunauer–Emmett–Teller (BET) surface area test using the AS-iQ-MP-XR (Anton-Paar GmbH) based on the adsorption and desorption curves of N2 gas. Before exposing the sample to N2 at 77 K, virgin and spent ABR were outgassed for 4 h at 200 and 170 °C, respectively. During the BET test, ABR was oversaturated with two long-chain PFAS (PFNA and 6![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 PTSA) representative of carboxylic and sulfonic PFAS. The elemental composition and mapping were obtained using the energy-dispersive X-ray (EDX) analysis at 20 kV (Zeiss Sigma FeSEM) with ABR sample affixed to stubs by carbon tapes. The element concentrations and specific atomic structures on the ABR surface were determined by X-ray photoelectron spectroscopy (XPS) (Kratos Axis Ultra spectrometer). ABR samples were also sent to the University of Calgary (Research Instrumentation and Technical Support Lab) for zeta potential measurements to determine the surface charge. Since our batch experiments utilized environmental concentrations that are typically lower (0.5–100 μg L−1), the PFAS adsorbed on the ABR surface could not be clearly observed by material characterization techniques. Hence, our characterization experiments utilized high concentrations of PFAS (100 mg L−1) (Table 1). Other ABR specifications including purity, specific gravity and density are found in SI-B.
2 PTSA) representative of carboxylic and sulfonic PFAS. The elemental composition and mapping were obtained using the energy-dispersive X-ray (EDX) analysis at 20 kV (Zeiss Sigma FeSEM) with ABR sample affixed to stubs by carbon tapes. The element concentrations and specific atomic structures on the ABR surface were determined by X-ray photoelectron spectroscopy (XPS) (Kratos Axis Ultra spectrometer). ABR samples were also sent to the University of Calgary (Research Instrumentation and Technical Support Lab) for zeta potential measurements to determine the surface charge. Since our batch experiments utilized environmental concentrations that are typically lower (0.5–100 μg L−1), the PFAS adsorbed on the ABR surface could not be clearly observed by material characterization techniques. Hence, our characterization experiments utilized high concentrations of PFAS (100 mg L−1) (Table 1). Other ABR specifications including purity, specific gravity and density are found in SI-B.
Given the exploratory nature of this study, a single replication and corresponding recovery studies was used to assess the feasibility of using ABR for PFAS removal. Data derived here will direct studies on optimal conditions for future studies with more controlled replication. Limitations in sample volumes required for chemical analyses also contribute to this decision. Error bars were representative of ±20% measurement uncertainty and were adopted to represent typical variability in analytical measurements.
The adsorption isotherm experiments were conducted by mixing different dosages of ABR (0, 0.1, 0.5, 1, 5, 10 g L−1) with 200 mL 100 μg L−1 PFAS solution at 120 pm using the jar tester for 24 hours. All the samples were then prepared and analyzed as previously. The data were fit to (1) Langmuir (one of the widely used adsorption isotherm models, assuming homogenous surface and monolayer, reversible adsorption), (2) Freundlich (suggesting a multilayer adsorption process on a heterogeneous surface), (3) Redlich Peterson and Langmuir-Freundlich (Sips) (an empirical model combining Langmuir and Freundlich approaches), and (4) Toth models (an extension of Langmuir model to describe a heterogenous surface and more widely used as a supplement). All the equations are described in SI-C.
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1 methanol
1 methanol![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) ethyl acetate (v/v) by gravity. The eluates were collected and evaporated to complete dryness in a water bath at 35–40 °C with a gentle blow of nitrogen. The dried extracts were then reconstituted in methanol to reach an extraction factor of 1000 (SI-C), then transferred into 2 mL amber vials and stored with parafilm at −20 °C until in vitro bioassay analysis.
ethyl acetate (v/v) by gravity. The eluates were collected and evaporated to complete dryness in a water bath at 35–40 °C with a gentle blow of nitrogen. The dried extracts were then reconstituted in methanol to reach an extraction factor of 1000 (SI-C), then transferred into 2 mL amber vials and stored with parafilm at −20 °C until in vitro bioassay analysis.
        The determination of cytotoxicity utilized the same reagents, data analysis, and procedure with slight modifications as.33 Briefly, cytotoxicity was determined by the percent inhibition of Aliivibrio fischeri bacteria after exposure to the samples using the BioTox LumoPlate kit (Environmental Bio-detection Product Inc). The concentration that could cause 10% light inhibition of exposure after 15 minutes (IC10,15min) was determined and represented as 1/IC10 in this study.
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 fluorotelomer sulfonic acid (6
2 fluorotelomer sulfonic acid (6![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2-FTSA) (100 mg L−1 each). This result suggests that a substantial portion of the ABR surface area remains available for further sorption. The density functional theory (DFT) pore size distribution also indicates the heterogeneity in ABR pore sizes (Fig. 1a), which enhances its ability to adsorb a wide range of substances, especially PFAS with their varied molecular sizes. Molecules are preferentially adsorbed into pores that closely match their size, as this increases the number of interactions between the adsorbate (i.e., pollutants) and the adsorbent. According to the adsorption free energy concept, as the number of contact points between the adsorbates and the adsorbent's surface increases, adsorption becomes more favorable. This is because multiple contact points along the pore walls create stronger attractive forces compared to adsorption on a two-dimensional surface.34
2-FTSA) (100 mg L−1 each). This result suggests that a substantial portion of the ABR surface area remains available for further sorption. The density functional theory (DFT) pore size distribution also indicates the heterogeneity in ABR pore sizes (Fig. 1a), which enhances its ability to adsorb a wide range of substances, especially PFAS with their varied molecular sizes. Molecules are preferentially adsorbed into pores that closely match their size, as this increases the number of interactions between the adsorbate (i.e., pollutants) and the adsorbent. According to the adsorption free energy concept, as the number of contact points between the adsorbates and the adsorbent's surface increases, adsorption becomes more favorable. This is because multiple contact points along the pore walls create stronger attractive forces compared to adsorption on a two-dimensional surface.34
        The pore size distribution additionally suggests that ABR predominantly contains mesopores (pore diameter between 2 and 50 nm (ref. 35)), which can be further advantageous for PFAS adsorption. Punyapalakul et al. observed a faster adsorption rate of PFOA and PFOS on mesoporous adsorbents than microporous ones (pore diameter <2 nm), with interparticle diffusion being the primary adsorption mechanism.36 Additionally, meso- and macroporous adsorbents were shown to have higher adsorption capacity for long-chain PFAS as larger molecules can easily access adsorption sites and avoid pore blockage.37 Also, larger PFAS molecules have a preference to aggregate in bigger structures, which leads to a higher removal via adsorption.2 Note that in terms of total pore volume, ABR is better than raw bauxite residues reported in the literature but incomparable to activated carbon-based adsorbents (Table S2). However, while activated carbon has a larger surface area than ABR, it is predominantly microporous, which may be limited for adsorbing smaller molecules.38
Although the surface area was unchanged, there were small differences observed between the total pore volumes of virgin and spent ABR, with virgin ABR pore sizes ranging from 2–46 nm and spent ABR with 2–76 nm. This observation indicates that PFAS may have filled or blocked the pores.34 This result is further supported by XPS and EDX analysis, which detected the presence of fluorine atoms (F) on the surface when ABR was exposed to a mixture of 10 PFAS (100 mg L−1 each) (Fig. 1b). Although XPS and EDX provided different relative atom contributions, both analyses were able to detect F, strongly indicating PFAS adsorption by ABR. The main difference in the approaches is their analysis depth, with XPS being more surface-sensitive than EDX. More specifically, XPS is minimally destructive and typically probes the top 1–10 nm of a sample, with elemental sensitivity in the order of 0.1 atomic percent.39,40 Therefore, XPS is ideal for the analysis of surface chemistry, thin films, and surface adsorption. By contrast, EDX provides information over a larger volume compared to XPS. It can assess relative atom contribution in samples ranging from 1 μm to a few μms (up to 5000 nm) and analyze the bulk material at an analysis depth of 100–3000 nm.41,42 Therefore, XPS analysis showed relatively higher concentrations of F atoms which are mostly present on the ABR surface.
XPS analysis further revealed the high atom contribution of metallic elements (Al, Na, Fe, Table 2) at low PFAS concentration (0.1 mg L−1 PFAS). This result was expected given that the bulk ABR primarily consists of metallic oxides (e.g., Fe2O3, Al2O3, SiO2).28 However, F was at levels higher than the background (i.e., virgin ABR), indicating adsorption of PFAS when added into the mixture. To further investigate PFAS sorption, the PFAS concentration was increased 1000-fold (100 mg L−1 each PFAS) in 3 g L−1 ABR (Table 2). At this high PFAS concentration, the relative atom contribution shifted to ∼58% F, confirming that ABR treatment facilitated PFAS removal from the water column and its subsequent adsorption onto the ABR surface.
| PFAS conc | Virgin ABR | 0.1 mg L−1 | 100 mg L−1 | ||
|---|---|---|---|---|---|
| ABR dose | N/A | 2 g L−1 | 6 g L−1 | 10 g L−1 | 3 g L−1 | 
| F | 1.37 | 4.60 | 2.00 | 2.07 | 57.69 | 
| Na | 22.17 | 20.54 | 20.63 | 21.45 | 2.97 | 
| Fe | 19.65 | 18.05 | 17.78 | 19.09 | 4.88 | 
| Ti | 2.31 | 2.13 | 2.17 | 2.21 | 1.11 | 
| Ca | 4.73 | 4.42 | 5.10 | 5.31 | 3.01 | 
| Si | 16.18 | 15.41 | 16.86 | 15.50 | 7.88 | 
| Al | 33.60 | 34.86 | 35.46 | 34.36 | 22.46 | 
XPS analyses further provided detailed spectra of each element, allowing for qualitative identification of F-bond types. This feature is particularly useful as it identifies whether C–F bonds are present or if F interacts with other surface elements (i.e., metal–F bonds). No C–F or metal–F bonds were observed on virgin ABR (Table 3). Although the F relative concentration is low (4.6%) for 0.1 mg L−1 PFAS concentrations (Table 2), both C–F and metal–F bonds were detected (Table 3). The presence of C–F was expected (i.e., main PFAS bond), but the appearance of metal–F bonds in the spectra suggests that F may interact with other metallic elements on the surface. Given the diverse elemental composition of ABR,28 it can prove to be a distinct advantage over other emerging adsorbents as it allows additional surficial interactions for diverse types of adsorbates.
| ABR dose (g L−1) | PFAS conc (mg L−1) | Fluorine bond energy position (eV) | Bond type detected | 
|---|---|---|---|
| 0 | 0 | N/A | N/A | 
| 100 | 0.1 | 685.0, 688.5 | Metal bond, carbon bond | 
| 0.1* | 685.5 | Metal bond | |
| 3 | 100 | 688.93 | Carbon bond | 
When ABR was further oversaturated with 100 mg L−1 PFAS (ΣPFAS = 1 g L−1), the C–F bond was more visible while the metal–F bond was no longer observed (Table 3). The result suggests that at high PFAS concentrations, C–F bonding (likely through physisorption) is more favourable than chemical bonding with surficial elements. As a preliminary experiment to determine whether C–F bonds remain after thermal treatment, XPS analysis of thermally treated (550 °C) spent ABR revealed only metal–F bonds (Table 3), suggesting that the thermal treatment can break C–F bonds on the surface. Although some bonds can be broken down at this temperature, complete thermal degradation of PFAS can be accomplished when heated at elevated temperatures (>1000 °C), providing a potential pathway for adsorbent regeneration.43 Note that evaluating the regeneration and reuse potential of spent ABR is beyond the scope of this study but is an avenue that can be explored further.
SEM and EDX analyses were also completed for spent ABR (exposed to 100 mg L−1 PFAS, ΣPFAS = 1 g L−1) to map the distribution of F from two random sites on the surface. The results show that F is present across the surface, though not uniformly distributed (Fig. 1c). Some areas exhibit higher concentrations of F atoms, indicating that these sites may be more conducive to PFAS adsorption. While it is challenging to correlate F elemental map with those of other abundant elemental maps such as C, Fe, Al, Si, Ti, and Na (Fig. S2), the findings nonetheless reiterate the surface heterogeneity of ABR, which can enhance its ability for adsorbing for a wide variety of substances ranging from inorganic anions (e.g., nitrate, fluoride, phosphate), oxides (sulphur, nitrogen, carbon), metal (e.g., arsenic, chromium, nickel, copper, cadmium), and other organic substances (phenols, dyes, acid extractable organics in oil sands processed water) as already observed by others.26,28
The zeta potential measurements of ABR at various pH conditions show the surface charge properties of virgin and spent ABR (Fig. 1d). The point of zero charge (PZC) (at which equal numbers of positive and negative charges are present on the surface) is determined to be at ∼ pH 5 (Fig. 1d). Also, the surface charge decreased with increasing pH (11.1 mV to −30 mV), suggesting stronger electrostatic repulsion by negatively charged substances at higher pH conditions, which makes ABR adsorption less favourable for these substances. The PZC of spent ABR was observed at ∼ pH 6, and with zeta potentials more negative than the virgin ABR. This shift was expected as PFAS exist as anions in the water column, and their adsorption onto ABR may have led to a negative net charge on the surface. At higher pH, the ABR surface charge becomes more negative, leading to stronger electrostatic repulsion (i.e., weaker attractions) with anionic PFAS.2 Therefore, it is beneficial for ABR to be operated at pH near its PZC, where electrostatic interactions are more favorable (acidic pH conditions are generally avoided, as pH is typically maintained in neutral to mildly alkaline conditions for further treatment or discharge of wastewater). Cheng et al. evaluated the leaching of aluminum ions at different pH levels from ABR and found that a pH range of 7–8 reduces aluminum leaching from ABR.28 This pH range also corresponds to a less negative charge on the ABR surface, which may be more amenable for PFAS adsorption on the ABR surface. Therefore, the bench-scale batch experiments described subsequently below were completed at this pH to reduce the leaching of metallic ions from ABR while maximizing the adsorption of PFAS.
Electrostatic interactions may also play a role in PFAS adsorption by ABR. The PFAS mixture in this study has carboxylic and sulfonate functional groups, which impart a negative charge to the molecules at environmental pH conditions (pKa ranging from −3.31 to 0.4). This negative charge may then lead to electrostatic repulsions between the negatively charged ABR (zeta potential of −6.68 mv at pH 7) and PFAS, but these may have been mitigated by more dominant hydrophobic interactions, especially for the long-chain ones.46 By contrast, short-chain PFAS are more soluble (due to shorter carbon backbones) and are more likely to be influenced by electrostatic attraction or repulsion.48 As can be observed here, electrostatic repulsion is likely greater for PFBA (#C = 4) than those with C > 7, which can explain its relatively poor removal by ABR. Despite this, ABR still shows some ability to remove short-chain PFAS (Fig. 2a), suggesting that the positive charges present on the ABR surface can promote some electrostatic attraction, particularly for these smaller, more polar PFAS compounds. As mentioned previously, long-chain PFAS also have a preference to form molecular/colloidal aggregates in the adsorbent surface pores.37 Their large molecular weights enable adsorbate–adsorbate interactions that eventually form micelle/hemimicelle (small aggregates).48,49 This further suggests that cooperative adsorption is at play and may be a contributing factor to overall PFAS adsorption to adsorbents.
Our batch experiments further indicate that both short- (1 h) or long-term (24 h) exposure periods were effective for removing long-chain PFAS (∼100% removal) (Fig. 2b) and also suggest that equilibrium adsorption could be reached relatively quickly (potentially <1 h for some). However, a longer adsorption period may be required to maximize the removal of short-chain PFAS such as PFPeA. For PFBA, however, lower removals were observed during the 24 h sorption period compared to 1 h experiments. Similar findings were reported by Nakazawa et al., where they observed PFBA desorption from a granular activated carbon (GAC) filter operated at full-scale at a drinking water treatment plant.50 Many suggest that the formation of small aggregates by long-chain PFAS can displace the already adsorbed short-chain PFAS, eventually leading to the desorption of small-chain PFAS from the adsorbents.37,48,49
Additional experiments comparing the performance of a commercially available PAC with ABR showed that for the same initial PFAS concentration (500 ng L−1), the removal efficiency of 10 g L−1 ABR was comparable to that of 0.1 g L−1 PAC (Fig. 2c). When ABR dosage was lowered to 0.1 g L−1, very low removals were observed for individual and ∑PFAS. This result supports our preliminary hypothesis that, to match the performance of commercially available adsorbents such as activated carbon, larger dosages are required due to ABR's lower surface area.
In general, a PSO model assumes low initial concentration, abundant active sites for the adsorbate, and adsorbates react with adsorbents irreversibly.52 Irreversibility is of importance to ensure recirculation of PFAS back into the treated wastewater is avoided. Given that chemisorption involves higher energy interactions than physisorption,53 binding of these five PFAS to ABR is therefore stable. Potential chemisorptive processes are illustrated further by the presence of metal–F bonds on the ABR surface after adsorption (XPS, see Section 3.1). Although it cannot be determined exactly what types of metal–F bonds were formed, it can be hypothesized that PFAS molecules can interact with the metallic elements/oxides present in ABR.
|  | ||
| Fig. 4 The adsorption isotherm for PFAS by ABR fitting via (a) Langmuir, (b) Freundlich, and (c) Sips isotherm model based on equilibrium concentrations derived dosages ranging from 0.1 to 10 g L−1. | ||
| PFAS | Langmuir | Freundlich | Sips | |||||||
|---|---|---|---|---|---|---|---|---|---|---|
| K L (L μg−1) | Q m (μg g−1) | R 2 | K F | 1/n | R 2 | K S | b | Q m (μg g−1) | R 2 | |
| PFHxA | 0 | 4.11 × 1011 | 0.515 | 0.009 | 2.050 | 0.966 | — | |||
| PFHpA | — | 1.523 | 1.416 | 0.998 | — | |||||
| PFOA | 0.029 | 188.679 | 0.963 | 5.958 | 0.834 | 0.950 | 0.001 | 2.433 | 198.793 | 0.982 | 
| PFNA | 0.005 | 3333.333 | 0.977 | 20.469 | 0.791 | 0.881 | — | |||
| PFDA | 0 | 5.380 × 109 | 0.523 | 60.632 | 0.693 | 0.641 | — | |||
| PFBS | 0 | 2.288 × 1012 | 0.802 | 0.009 | 1.887 | 0.915 | 1.24 × 10−12 | 6.123 | 106.729 | 0.973 | 
Although the goodness-of-fit is a good metric for isotherm model choice, others caution choosing the isotherm solely on this criterion as it may not always provide meaningful or practical insights.53,54 For instance, the heterogenicity of ABR surface and potential aggregation of PFAS during adsorption49,55 conflict with the monolayer assumption of the Langmuir model. Hence, although PFNA fit well via Langmuir, Freundlich isotherm (multi-layer adsorption) is more applicable despite the lower R2 value (i.e., 0.977 vs. 0.881). Additionally, since PFAS adsorption follows the PSO kinetic model which implies irreversibility challenges the choice of Langmuir model where reactions are assumed to be reversible.53
As for Freundlich isotherm, the 1/n value provides insights related to the adsorption mechanism, where a value of 1/n > 1 indicates that additional sorbates are bound to the adsorbent by weaker and weaker free energies.56 As an indicative of affinity, 1/n > 1 also suggests that the adsorption tendency increased as the surface concentration of PFAS increased.56,57 Therefore, the cooperative adsorption among the adsorbates is an important mechanism for substances behaving this way (i.e., sorbed sorbates bring in more sorbates via attractive interactions). This aligns with the assumption that the interactions between PFAS molecules can create micelle/hemimicelle formation (i.e., surfactant aggregates),37,39,40 further influencing their multilayer adsorption on adsorbents.
Sips model is a hybrid of Langmuir and Freundlich (mathematically) and can represent adsorption equilibrium for a wide range of adsorbate concentrations, whether the surface is homogeneous or heterogeneous.53 The good fit of experimental data to Sips model also indicates PFOA adsorption on ABR can reduce to the Freundlich isotherm as the concentration decreases.55
Important information derived from isotherm experiments is the maximum adsorption capacity (Qm) of the material (for Langmuir and Sips), and the opportunity to determine the desired dosage of adsorbent when operated in a completely mixed flow reactor system (CMFR) (for the case of Freundlich isotherm). This is illustrated in eqn (S13) and (S14), and depending on the target removal requirements, the ABR dose to reach the target efficiency could be estimated. For instance, to remove 50–95% of PFHpA via ABR, doses ranging from 0.1 to 6.4 g L−1 are required (Table S6). From here, it appears that a concentration of up to 10 g L−1 ABR is suitable to remove most of the substances (ΣPFAS removal of >85%), substantially reducing the ABR dosage from earlier experiments (100 g L−1).
Although it was observed here that PFAS removals were improved at higher ABR dosages (Fig. 2a), the result further suggests that there is a potential for increased toxicity at higher dosages. Hence, the results support the use of <10 g L−1 ABR dosage as suggested from the isotherm data (see Section 3.3) as both removal efficiency is maximized, and the potential toxicity is minimized. This result is also useful for future ABR operation as cytotoxicity can be tracked and compared to effects-based trigger values for ecosystem protection should the treated water be discharged into a receiving environment (i.e. if 1/IC10REF < 20 after dilution is considered). If this is not possible, further material modification (e.g., heat or acid treatment) may be required to reduce toxicity.
In the future, further improvements in ABR characteristics can be made, and optimization of ABR dosage and treatment conditions can be assessed on a pilot- or full-scale and promote the comprehensive evaluation of the combination of ABR with existing WWTP processes. Finally, spent ABR (i.e., after wastewater treatment) allows for the extraction of metals and subsequent reuse processes (e.g., construction material/roadway aggregates). Given the large amounts of source material and ABR use, there is a potential for ABR to be utilized as an economically and environmentally friendly adsorbent material to remove PFAS and as a supplement to the existing treatment process.
The processed data supporting this article have been included as part of the supplementary information (SI). Supplementary information: pre-experiment preparations, material specification and characterization, equations used within the article, PFAS concentration data, and optimal dosage calculations. See DOI: https://doi.org/10.1039/d5va00101c.
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