Open Access Article
Andres F. Prada
*, 
Jaemin Kim
, 
Linduo Zhao
, 
Fangyu Li
, 
Lee Green
 and 
John W. Scott
Illinois Sustainable Technology Center, Prairie Research Institute, University of Illinois at Urbana-Champaign, 1 Hazelwood Dr., Champaign, IL 61820, USA. E-mail: pradase2@illinois.edu; jaemin@illinois.edu; zhao117@illinois.edu; seanl6@illinois.edu; leegreen@illinois.edu; zhewang@illinois.edu
First published on 27th October 2025
Mechanochemical methods such as ball milling offer a solvent-free and non-thermal approach for PFAS remediation, enabling not just separation but actual destruction of PFAS through defluorination. In this study, we demonstrate that effective PFAS defluorination using ball milling critically depends on the presence of a co-milling catalyst, in this case piezoelectric catalysts such as boron nitride (BN), which showed the highest performance among other tested piezoelectric materials. While BN has already proven effective for defluorination of pure PFAS compounds, PFAS in sediments, and aqueous film-forming foam (AFFF), prior studies have been limited by the small amounts of PFAS they can treat inside another medium. To overcome these limitations, we present as an alternative the coupling of BN with activated carbon as a pre-concentration medium for PFAS. By leveraging activated carbon's high sorption capacity, we were able to destroy nearly 100 times higher mass of PFOA in less than one-third of the time compared to previous studies on sediments or AFFF. These results suggest that the design of larger-scale ball milling systems for PFAS destruction should incorporate the use of high-capacity sorbents to concentrate contaminants, thus destroying higher amounts more effectively. While in the case of activated carbon the chances of reusing it after milling are minimal, it could be safely disposed of without the risk of releasing PFAS back into the environment.
To manage PFAS contamination, several technologies have been developed and applied for their physical separation from water, including activated carbon adsorption, anion exchange resins, nanofiltration, reverse osmosis, ozonation, and foam fractionation.8,9 Some of these methods have achieved over 90% removal efficiency for long-chain PFAS.10,11 However, there is the potential risk of PFAS release from disposed materials as confirmed from landfill leachate data which show some of the highest PFAS concentrations among environmental and industrial water streams,12 highlighting the need to destroy PFAS laden in materials prior to their disposal. As a result, there is growing interest in treatment technologies that go beyond separation and focus on the actual destruction of PFAS compounds—specifically, through defluorination.
Incineration has been identified by the U.S. EPA as the only currently viable solution for PFAS destruction,13 as it is capable of full defluorination of PFAS compounds.14,15 However, concerns remain regarding the volatilization of shorter-chain PFAS and the potential emission of toxic organic fluorine byproducts or perfluorinated carbons. In response, the U.S. Department of Defense has emphasized that incineration of PFAS-laden materials should only be applied under strictly controlled conditions, following detailed protocols aligned with Clean Air Act requirements.16 As alternatives, several non-incineration approaches have been developed for treating solid-phase PFAS, including supercritical water oxidation,17 UV-advanced reduction processes,18 non-thermal plasma,19 hydrothermal alkaline treatment,20 electrochemical oxidation,21 or mechanochemical degradation.22 Among these, mechanochemical methods—such as ball milling—offer a promising, solvent-free, and energy-efficient strategy for PFAS destruction in solid matrices, and are increasingly viewed as a more sustainable option.23
Mechanochemical degradation of PFAS, particularly using ball milling systems, was first introduced by Zhang et al.24 In their study, various co-milling reagents—including CaO, SiO2, Fe–SiO2, NaOH, and KOH—were tested to enhance the defluorination efficiency of solid-phase PFOS and PFOA. Among these, KOH proved to be the most effective, achieving over 90% fluoride recovery after 4 to 8 hours of treatment.24 Yang et al. (2023), however, argued that the high chemical loading required for KOH—exceeding a 20
:
1 weight ratio—posed limitations for practical applications and disposal of treated materials (caustic residues), highlighting the need for more efficient co-milling reagents.25 They proposed boron nitride (BN) as a promising alternative. BN is a piezoelectric material traditionally used as an electrical insulator due to its wide band gap (∼6.0 eV), but it is increasingly regarded as a wide band gap semiconductor.26 For PFAS treatment, BN's crystalline structure and piezoelectric properties enable the generation of localized electric potentials upon mechanical impact, which can cleave the strong C–F bonds.25 Yang et al. (2023) demonstrated that BN, used at a BN to solid-phase PFAS weight ratio of 5 to1, could mineralize over 90% of pure PFOA and PFOS within 2 to 4 hours, and over 80% of 21 PFAS species detected in 2 grams (g) of sediment samples after 6 to 10 hours of treatment.25
Zhu et al. (2025) later used similar techniques to destroy up to 2 mg of PFOS adsorbed in different types of anion exchange resins under more than 3 hours of treatment with the assistance of BN as well.27 Additionally, Yang et al. (2025) applied similar principles and parameters to demonstrate complete defluorination of 100 to 1000 μL of undiluted aqueous film-forming foam (AFFF) under ambient conditions, using a combination of boron nitride (BN) and quartz sand (SiO2).28 However, a major barrier to further implementation of piezoelectric ball milling strategies is the small scale at which this technology has been developed, suitable only for treating limited quantities of contaminated liquids or solids. To address this, Yang et al. (2023) proposed using larger equipment, such as tumbler ball mills, to enable treatment of greater volumes of undiluted AFFF.28
Here we demonstrate an alternative, and potentially more practical, approach involving pre-treating contaminated liquids by filtering them through activated carbon, followed by ball milling the PFAS-laden activated carbon. Activated carbon has proven to be an effective sorbent, particularly for long-chain PFAS, with adsorption capacities ranging from 100 to 400 milligrams of PFAS per gram of carbon.29,30 In their study, Yang et al. (2025) worked with AFFF containing a total organic fluorine concentration of 9080 mg L−1.28 At this concentration, one gram of activated carbon could concentrate PFAS from nearly 50 mL of AFFF, adsorbing up to 400 mg of PFAS, and representing a 50-fold increase in the volume treated using the same ball milling setup and energy input, compared to the direct treatment of only 1 mL. This approach highlights the potential to scale up PFAS remediation of high concentrated solid materials without the need of scaling the equipment or increasing the energy consumption, and offers an alternative to incineration or reactivation practices for PFAS-laden activated carbon.
In this study, we demonstrate the effectiveness of piezoelectric ball milling for mineralizing nearly 90% of PFOA adsorbed onto activated carbon. The high level of defluorination was achieved after just 2 hours of treatment, using the optimized dosage of boron nitride (BN) previously shown to be effective for pure, solid-phase PFAS.25 By first adsorbing PFAS from aqueous solutions onto activated carbon, this approach lays the groundwork for a simple, scalable, and practical remediation strategy—operable at ambient temperature and pressure, and producing no harmful by-products aside from clean defluorination. Although we found that activated carbon cannot be reused due to a roughly 50% reduction in surface area from repeated mechanical impacts, the high fluoride recovery confirms that the treated carbon can be safely disposed of, mitigating long-term environmental risks.
:
1 relative to the PFOA, corresponding to 500 mg. This catalyst dosage was maintained in both experiments involving pure PFOA and 1 g of PFOA-laden activated carbon, as the adsorbed PFOA content was standardized at 100 mg.
For sorption onto activated carbon, 100 mg of PFOA were dissolved in 100 mL of nanopure water (>18.0 MΩ cm; Labconco Water Pro Plus system, Kansas City, MO, USA) in 125 mL glass vessels. One gram of activated carbon was then added to each vessel. The vessels were sealed with Parafilm and placed on a temperature-controlled reciprocal shaker, operated at 200 rpm and maintained at 25 ± 0.5 °C for 24 hours. After shaking, the vessels were left undisturbed on a countertop to allow the activated carbon to settle. Then, 1 mL of the supernatant was collected from the center of each vessel for PFAS analysis to verify sorption.
PFAS analysis was conducted using a Shimadzu 8050 Ultra High-Performance Liquid Chromatography tandem Mass Spectrometry (LC-MS/MS) system (Kyoto, Japan). Detection used electrospray ionization (EIS+) and multiple-reaction monitoring (MRM) modes. Prior to each assay, the instrument was calibrated using seven calibration standards made with reference standards obtained from Wellington Laboratories (Guelph, Ontario, Canada), for a detection range of 1–100 parts-per-billion (ppb). Quality control measures included the use of isotope-labeled surrogates and internal standards, as well as continuing calibration blanks, reagent blanks, and independently prepared check standards. Final PFAS concentrations were calculated using the isotope dilution method, which corrects native PFAS levels based on surrogate recoveries. Reported values represent the average of multiple sample preparations and analyses. Associated errors were determined using either the relative percent difference (%RPD) or relative standard deviation (%RSD) across replicate measurements.
For the experiments on activated carbon, after sorption, the PFAS-laden activated carbon was collected and dried in an oven at 60 °C overnight prior to ball milling treatment. Once dried, each gram of activated carbon was added along with 500 mg of one of the previously described catalysts and placed into stainless steel jars containing stainless steel balls (100 mL jars, 16 Ø 1.0 cm large balls and 100 Ø 0.6 cm small balls, 160 g in total). Each jar was sealed with a rubber gasket and lid, then clamped into a planetary ball mill (PQ-N04, Across International), which accommodates four jars. All four jars were milled simultaneously for 1 to 4 hours at 580 rpm (Fig. S-1). At this operating speed, the mill consumes 0.14 kWh per hour, as measured using a plug-in power meter. Therefore, the total energy consumption for the milling process ranges from 0.14 to 0.56 kWh, depending on the treatment duration.
After ball milling, the contents of each jar were rinsed with nanopure water into pre-cleaned 200 mL glass beakers. The beakers were previously washed, fired at 450 °C for 4 hours, and triple-rinsed with methanol, toluene, and ammonium hydroxide. A 5 mL aliquot of the rinse water was collected to quantify fluoride ion yielded and thus confirm the cleavage of C–F bonds and, consequently, the defluorination of PFOA. Defluorination efficiency was calculated as the percentage of measured fluoride ions relative to the total fluorine content of the initial PFOA. The instrument used was an ion chromatography system (Dionex ICS-2100, Thermo Scientific, Waltham, MA), calibrated with fluoride reference standards obtained from SPEX CertiPrep (Metuchen, NJ), covering a detection range of 1–100 parts per million (ppm). Fluoride measurement alone may miss partially degraded fluorinated organic compounds, including shorter-chain PFAS or other fluorine-bearing byproducts that retain C–F bonds but are not mineralized.31
The milled activated carbon was then dried overnight at 60 °C for subsequent analysis of Brunauer–Emmett–Teller (BET) surface area, scanning electron microscopy (SEM), and energy-dispersive X-ray spectroscopy (EDS). BET surface area measurements were performed using a Micromeritics Gemini VII analyzer (Norcross, GA), based on 11-point adsorption isotherms over a relative pressure (P/P°) range of 0.05–0.3. SEM analysis was conducted using a Hitachi S-4800 High-Resolution SEM (Tokyo, Japan), and elemental characterization via EDS was performed using a Shimadzu EDX-7000 Energy-Dispersive X-ray Fluorescence Spectrometer (Tokyo, Japan).
Defluorination of over 80% of pure PFOA was observed with the addition of BN as a catalyst, for all milling times, on both our results and those presented by Yang et al. (2023)25 (Fig. 1A). Our results showed a uniform defluorination trend with no increase over time confirmed by Analysis of Variance (ANOVA) and Tukey post hoc with no significant differences in defluorination efficiency among the 1-, 3-, and 4-hour treatments (p > 0.05, Table S-2). Notably, the 2-hour treatment yielded significantly higher defluorination, representing a 6–10% improvement compared to the other durations. This non-monotonic behavior suggests that the catalytic activity of BN may become depleted or less effective over time, limiting further degradation beyond the initial 80–90%. Yang et al. (2023) reported a similar trend, observing slightly lower efficiency after 4 hours of milling compared to 2 hours, although their efficiencies were nearly 10% higher than ours.25 Additionally, as previously established, mechanical effects alone account for only ∼1% defluorination, further reinforcing that prolonged milling without fresh catalyst input does not substantially enhance performance. The electric potentials generated by BN during ball impacts are likely responsible for the rapid mineralization of pure solid-phase PFAS within the ball milling system.
When PFOA was adsorbed onto activated carbon, a clear linear increase in defluorination occurred between the 1-hour (46%) and 2-hour (89%) treatments (Fig. 1B), which contrasts with the behavior observed for pure PFOA. However, similar to the pure PFOA experiments, no further increase in defluorination efficiency was observed beyond the 2-hour treatment as ANOVA and Tukey post hoc tests revealed no significant differences among the 2-, 3-, and 4-hour treatments (p > 0.05, Table S-3). The lower defluorination observed at the 1-hour mark in the activated carbon experiments may be attributed to the physical distribution of PFOA: although the total mass of PFOA was kept constant, its dispersion across the porous matrix of the activated carbon likely diluted and spatially separated the molecules compared to the dense solid-phase form used in the pure PFOA trials. In this more dispersed form, the efficiency of the ball milling treatment appears more sensitive to treatment time, until, once again, the catalytic activity of BN diminishes after approximately 2 hours of milling.
Additional 2- and 4-hour tests were conducted using alternative catalysts, specifically aluminum nitride (AlN) and silicon dioxide (SiO2), to explore potential substitutes for BN. However, both alternatives resulted in defluorination efficiencies of no more than 20% (Fig. 1B). These results are consistent with previous studies evaluating SiO2 for pure PFAS compounds, which also reported defluorination below 20%.24,28,32,33 Gobindlal et al.32 suggested that the low efficiency could be attributed to the formation of unextractable fluorinated species and provided evidence from solid-state nuclear magnetic resonance (NMR) spectroscopy indicating the formation of insoluble Si–F bonds. These bonds likely hindered fluoride ion recovery during solvent extraction. We attribute the observed differences in catalytic efficiency primarily to the varying piezoelectric properties of the materials, specifically their piezoelectric strain coefficients under longitudinal mode activation (33-mode, d33). Table 1 shows the d33 coefficients (in picocoulombs per newton, pC/N) for the three catalysts evaluated in this study, illustrating that BN exhibits a piezoelectric strain approximately 3.5 to 8 times higher than that of AlN and SiO2, correlating well with the higher defluorination performance observed.
We further examine the activated carbon before and after treatment. The morphology of untreated activated carbon exhibits a rough surface with minimal deposition of fine particles, heterogeneous texture with prominent pits, elevations, and irregular contours—features that contribute to its porous structure and high surface area (Fig. 2B top). This morphology enables effective exposure of adsorption-active sites, which is critical for maintaining adsorption capacity, particularly for contaminants such as PFAS. In contrast, the ball-milled activated carbon displays a markedly altered morphology, with absence of the original pit-and-peak topography (Fig. 2B bottom). Instead, the surface is densely covered with fine particulates, likely occluding the pore structure and significantly reducing the accessible surface area. This observation is supported by the BET surface area analysis, where a nearly 50% reduction of surface area after ball milling was measured (Tables S-4 and S-5). This masking effect is believed to contribute to the reduced adsorption performance observed in subsequent treatment cycles.
The ball milling process was performed using stainless steel components, which typically contain iron (Fe), chromium (Cr), and nickel (Ni). The presence of fine surface deposits in Fig. 2B (bottom) is likely caused by the abrasion of milling equipment, resulting in Fe, Cr, and Ni fragments embedding onto the activated carbon surface during processing. This is further supported by the EDS spectrum of untreated and treated activated carbon (Fig. 2C, and Tables S-6 and S-7), as well as the elemental mapping of the treated sample (Fig. S-2).
The EDS spectrum of the untreated control (Fig. 2C top) primarily displays peaks for C and O, the main components of activated carbon, along with minor peaks for S, Mg, Si, and Ca, likely from residual mineral debris. In contrast, the EDS spectrum of the ball-milled sample (Fig. 2C bottom) reveals a marked increase in Fe, Cr, and Ni content, alongside the original elements. Importantly, elemental mapping of the ball-milled sample (Fig. S-2), collected from the area shown in Fig. 2B (bottom), shows that fine particles containing Cr, Fe, and Ni are evenly distributed and closely correspond to the surface contours of the activated carbon, further indicating their origin from stainless steel abrasion during the milling process.
One potential approach to minimize the shedding of stainless steel particles during ball milling is to use jars and balls made from materials with higher surface hardness and therefore higher resistance to abrasion. Commercial options available for the ball milling system used in this study include zirconium oxide and tungsten carbide, both of which are significantly harder than stainless steel. Zirconium oxide approaches the hardness of advanced ceramics,37 while tungsten carbide is among the hardest known materials, second only to diamond.38 These alternatives are more expensive than stainless steel. But future studies should evaluate whether using them could reduce the pore clogging on activated carbon, thereby increasing its potential for reuse in at least one additional adsorption cycle and potentially offsetting the higher upfront costs. However, even in the absence of material shedding, the high-energy ball impacts still deform the activated carbon structure, reducing pore space and overall surface area, which ultimately compromises its sorption performance.
At the 580 rpm used in our experiments, the impact force is approximately 57 N.25 Reducing the speed to 500 rpm and 400 rpm lowers the force to about 45 N and 30 N, respectively, representing reductions of 21% and 47%.25 While this suggests a gentler treatment, it raises the question of whether extended treatment times might still compromise the carbon's physical integrity. Reported evidence also suggests that prolonged milling, even at reduced speeds, can still degrade the surface area and porosity of activated carbon. For example, Yuan et al. (2023) showed that at 500 rpm, after 5 hours of milling the degradation notably increased with drops in surface area and porosity of 40% by 8 hours and more than 85% by 24 hours.39 These findings may indicate that while lowering the milling intensity can reduce the immediate mechanical damage, extended milling durations needed to compensate for the lower energy input could still result in substantial degradation.
Even in the case of a one-time use of activated carbon, our methodology remains more cost-effective in the per-gram-of-PFAS basis than previously reported ball milling approaches. By leveraging the high sorption capacity of activated carbon, we successfully destroyed nearly 100 times higher mass of PFOA in less than one-third of the time compared to other studies that tested their defluorination in different media. For instance, prior studies showed that it required 6 to 10 hours of ball milling to destroy much smaller PFAS amounts, such as 93% of 0.3 mg in 2 g of sediment25 or 90% of 9 mg in 1 mL of AFFF.28 This demonstration highlights a scalable and efficient strategy for PFAS destruction, not only through the use of larger ball mills, but also by concentrating substantial PFAS loads into small amounts of activated carbon that can be processed with the same system described in this study.
One potential advantage over incineration, however, is that the ball milling reaction takes place in a sealed, enclosed environment, which inherently minimizes the risk of vapor-phase emissions during treatment, unlike incineration, where volatilization and atmospheric release are more likely. However, determining whether volatile short-chain PFAS were released upon opening the sealed jars after treatment was beyond the scope of this study, primarily due to the significant analytical challenges involved in reliably sampling and quantifying volatile fluorinated species in the post-milling headspace. We recommend that future studies consider this, or alternatively, analyze the total organic fluorine content in the rinsed water following milling, which indirectly may help estimate the fraction of fluorine potentially present in the gas phase.
| This journal is © The Royal Society of Chemistry 2025 |