Le Tanga,
Paul Schweng
ab,
Joseph J. Dale
a and
Robert T. Woodward
*a
aInstitute of Materials Chemistry and Research, Faculty of Chemistry, University of Vienna, Währinger Straße 42, 1090, Vienna, Austria. E-mail: robert.woodward@univie.ac.at
bVienna Doctoral School in Chemistry, University of Vienna, Währinger Straße 42, 1090, Vienna, Austria
First published on 4th August 2025
The selective removal of oil and oil-based contaminants from water remains a critical challenge in environmental remediation. Here, we report a series of hypercrosslinked polymers with high surface areas and tuneable chemistries, achieving exceptional adsorption capacities for a variety of organic solvents, with a maximum capacity of >15 g g−1 for chlorinated solvents. We describe how the adsorption capacities of the materials in pure organic solvents are governed by porosity rather than sample fluorine content and its associated hydrophobicity, challenging conventional design strategies. Oil/water separation tests of the most promising networks demonstrated the effective removal of toluene from water, achieving separation efficiencies of >99%. The polymers also exhibit exceptional stability in organic solvents, allowing repeated use. This work establishes hypercrosslinked polymers as robust, scalable materials for efficient oil–water separation and advanced wastewater treatment.
Current oil remediation technologies face numerous limitations, particularly in separating immiscible oil from water. Skimmers and dispersants are commonly used, yet are energy-intensive, limited in effectiveness, and often cause secondary pollution.1 Adsorbent materials capable of selectively capturing large amounts of bulk-phase oils have garnered attention as attractive alternatives. Ideal sorbents should exhibit high uptake capacity, hydrophobicity, rapid adsorption, structural durability, and reusability. Achieving all these features simultaneously, while ensuring scalability and economic viability, remains a major challenge for adsorbent material design. Efforts have focused on developing various hydrophobic porous frameworks, including sponges,4,5 membranes,6,7 fabrics,8,9 and aerogels,10 However, many such systems are hampered by complicated synthesis routes, lack of durability, or challenging regeneration procedures.
Hypercrosslinked polymers (HCPs) may represent a promising alternative platform for oil sorption and water remediation. These amorphous polymer networks possess high surface areas, tuneable pore structures, swellability, and exceptional chemical stability, and can be synthesised from inexpensive, commercially available monomers.11–13 HCPs have shown excellent performance in both gas phase adsorption, such as atmospheric water harvesting,14,15 CO2 capture,16 and the capture of volatile organic compounds,17,18 as well as in the adsorption of dissolved pollutants.19,20 However, their potential for bulk-phase organic solvent uptake and direct oil/water separation remains relatively underexplored. Superhydrophobic monolithic adsorbents used for oil/water emulsion separation and oil recovery have been produced via the coating or anchoring of HCPs onto melamine formaldehyde sponges.5,21,22 The coated sponges showed ultrahigh separation efficiency and outstanding durability. Elsewhere, Lin et al. fabricated hypercrosslinked microporous polymers via emulsion-templating, demonstrating that the incorporation of fluorine substantially enhanced both hydrophobicity and oil adsorption capacity.23
Powdered or particulate adsorbents are particularly efficient in cleaning high viscosity or large-area thin oil spills when compared with monolithic adsorbents, however, the oil adsorption capacities of powders remain limited in comparison24 A powdered superhydrophobic covalent organic framework showed a crude oil uptake capacity of almost 12 g g−1 after post-functional hydrophobisation via silane grafting.25 Activated carbons have also shown promise for oil sorption, with lauric acid decorated biochar achieving an oil uptake capacity of 11 g g−1 (ref. 26) and magnetite-loaded carbons offering facile separation using magnetic fields.27 However, further work is needed in order to improve uptake capacities and unveil simpler routes to effective adsorbents.
In this work, we synthesise both non-functional and fluorine-containing HCPs by the simple self-polycondensation of 4,4′-bis(chloromethyl)biphenyl (BCMBP) and α,α′-dichloro-p-xylene (pDCX).28 To investigate the impact of chemical composition on adsorption and separation performance, the fluorine-containing monomer 4-fluorobenzyl chloride (pFBC) is incorporated into the HCP structure in varying ratios. Given the hydrophobic nature of fluorine, its incorporation was expected to enhance oil adsorption and improve oil/water separation. The resulting materials are evaluated for their chemical composition, porosity, organic solvent uptake, and separation efficiency, offering insights into structure–property relationships in these HCP-based adsorbents.
Network | Monomer feedstock composition | |||
---|---|---|---|---|
Monomer 1 | n (mmol) | Monomer 2 | n (mmol) | |
BP-HCP | BCMBP | 3 | — | — |
BP-HCP-25F | BCMBP | 3 | pFBC | 1 |
BP-HCP-50F | BCMBP | 3 | pFBC | 3 |
X-HCP | pDCX | 3 | — | — |
X-HCP-25F | pDCX | 3 | pFBC | 1 |
X-HCP-50F | pDCX | 3 | pFBC | 3 |
Thermogravimetric analysis (TGA) was conducted using a Discovery TGA (TA instruments). Between 3 to 10 mg of sample was placed into a platinum sample pan, equilibrated at 30 °C, then heated to 800 °C at a ramp rate of 10 °C min−1 in air. Samples were held at the target temperature for 5 min before being allowed to cool. The TGA data were recorded and analysed using the Discovery TGA@Lab program in TRIOS software.
X-ray photoelectron spectroscopy (XPS) was performed on a Nexsa Photoelectron Spectrometer (Thermo Scientific). All measurements were performed using Al-Kα X-rays with a spot size of 400 μm. The survey spectra were taken at a pass energy of 200 eV from 1350 to 0 eV with a resolution of 1 eV. The high-resolution C 1s, O 1s, F 1s, and Cl 2p spectra were collected at a pass energy of 50 eV with a resolution of 0.1 eV. C 1s was collected in the range from 298 to 279 eV, O 1s from 545 to 525 eV, F 1s from 698 to 678 eV, and Cl 2p from 210 to 190 eV.
The N2 adsorption–desorption isotherms were measured at −196 °C using a 3Flex (Micromeritics), or a TriStar II (Micromeritics) for sample repeats. Before the measurement, 50 to 100 mg of sample was degassed at 120 °C under N2 flow for 14 h using a FlowPrep 060 (Micromeritics). The networks’ specific surface areas (SSA) were determined via the Brunauer–Emmett–Teller (BET) method in the relative pressure P/P0 range 0.05 to 0.3. Pore size distributions (PSDs) were determined from the N2 adsorption branch of the isotherm using quenched solid density functional theory (QSDFT) and a carbon model with slit/cylindrical pores. The total pore volume VP, micropore volume VMic, and mesopore volume VMes were determined from the cumulative pore volumes calculated using QSDFT in the relevant pore width ranges. When calculating VP and VMes, isotherm points from P/P0 > 0.97 were excluded to avoid the effects of bulk N2 condensation.
Dynamic vapour sorption (DVS) experiments were performed on a DVS-Discovery (Surface Measurement Systems). Approximately 10 mg of sample was weighed into a quartz crystal pan. Each experiment was performed at 25 °C and either deionised water (HPLC grade) or toluene (HPLC grade) was used to generate the desired relative pressure. Each analysis commenced at a relative pressure of 0.0 P/P0 and was increased to the desired P/P0 for sorbate uptake. Isotherms were recorded up to 0.9 P/P0, using a step increment of 0.1. Each step was equilibrated until the weight change was below 0.005% min−1 prior to data point collection.
![]() | (1) |
For comparison, the adsorption capacity kB based on the dry weight of the sample before adsorption was calculated according to eqn (2), following previous reports:5,22,23,27
![]() | (2) |
![]() | (3) |
![]() | (4) |
The FTIR spectra of BP-HCPs (Fig. 1c) displayed the characteristic absorption peaks of the 4,4′-dimethylbiphenyl framework, with BP-HCP-25F and BP-HCP-50F exhibiting three additional peaks at 1228, 1157 and 501 cm−1. The peaks at 1228 and 1157 cm−1 were assigned to C–H in-plane bending vibration in the fluorinated aromatic ring, and the peak at 501 cm−1 was assigned to the characteristic CAr–F bending vibration, confirming the incorporation of fluorine. The CAr–F stretching vibration expected at around 1330 cm−1 was likely overlapped by other signals and was not observed. Increasing pFBC content led to a greater intensity of peaks associated with fluorine, indicative of BP-HCP-50F containing the highest fluorine content of the BP-HCPs. A similar trend was observed in the X-HCP series (Fig. 1d), where X-HCP-25F and X-HCP-50F exhibited the same three additional peaks at 1233, 1157 and 501 cm−1, relative to X-HCP, confirming successful pFBC incorporation. Again, peaks associated with fluorine increased with expected pFBC content, indicating X-HCP-50F contained the highest fluorine content of the X-HCPs. The FTIR spectra of the BP-HCPs after 6 months storage in ambient conditions were almost the same as their corresponding pristine spectra (Fig. S1), confirming the excellent stability of HCPs.
XPS was conducted to understand the surface chemistry and relative fluorine content of all HCPs. Survey spectra (Fig. 1e and f) confirmed the presence of fluorine in all networks produced from monomer feeds containing pFBC, as well as the presence of residual terminal chlorine. The pFBC was incorporated effectively with increasing pFBC monomer ratios, with BP-HCP-50F and X-HCP-50F reaching fluorine contents of 6.0 ± 0.4 at% and 7.1 ± 0.1 at%, respectively. The fluorine content of all networks was in slight excess of the theoretical value (Table S1), likely due to the molecule's ability to effectively stabilise the carbocation formed upon the loss of Cl, aiding crosslink formation to the BCMBP monomer. However, the fluorine substituent is weakly deactivating toward electrophilic aromatic substitution and likely suppresses further propagation upon incorporation into the polymer. The presence of oxygen in all HCPs was ascribed to the attack of trace water at the carbocation generated during the Friedel–Crafts reaction. In the fluorine-decorated HCPs, the high-resolution F 1s spectra displayed a peak at 687.5 eV, assigned to the CAr–F in the pFBC (Fig. S2). An additional peak at ∼694 eV was observed, which does not correspond to known C–F species but is close to the binding energy of SF6 (693.5 eV).30 A plausible explanation for this feature may be residual sulfur contamination, a common impurity in organic materials originating from crude oil cracking.
The high-resolution C 1s spectra of BP-HCPs and X-HCPs were deconvoluted into three peaks ∼284.8 eV, 287.0 eV and 291.4 eV, corresponding to sp2/sp3 C, the combination of C–O and C–Cl, and a low-intensity π → π* shake-up feature,30 respectively (Fig. S3). In fluorine-functionalised HCPs, C–F was expected to produce a peak at 286.0–286.5 eV but was not clearly distinguishable due to spectral overlap with C–O and C–Cl.
The TGA curves of all HCPs showed similar thermal stability (Fig. S4). All networks increased in weight at around 240 to 260 °C, indicative of oxidation,15 before the onset of thermal decomposition at around 340 to 360 °C. All samples were decomposed completely at approximately 580 to 600 °C. The introduction of fluorine into the HCP networks did not noticeably alter their thermal stability.
N2 adsorption–desorption isotherms of all samples were collected at −196 °C. According to IUPAC classification,31 all networks displayed a combination of type I and type IV isotherms (Fig. 2a and b), consistent with typical HCPs.14,32 The type I behaviour demonstrated by a steep uptake at low P/P0 indicates microporosity, while the type IV component identified by hysteresis during desorption reflects mesoporous capillary condensation.
With increasing pFBC content, BP-HCPs exhibited a steady decline in porosity. The BET-specific surface areas (SSABET) decreased from 1748 ± 78 in BP-HCP to 960 ± 114 m2 g−1 in BP-HCP-50F, with corresponding reductions in the total pore volume VP, micropore volume VMic, and mesopore volume VMes (Table 2). On the other hand, porous properties remained relatively unchanged between X-HCP and X-HCP-25F, with SSABET of 1089 ± 105 m2 g−1 and 1140 ± 94 m2 g−1, respectively, and an apparent increase in VMes from 0.61 cm3 g−1 to 0.84 cm3 g−1 was observed. However, at the highest pFBC loading (X-HCP-50F), porosity declined significantly, resulting in a SSABET of 691 ± 69 m2 g−1 and VMes of 0.40 cm3 g−1. Overall, X-HCP networks derived a larger portion of their VP from micropores than their BP-HCP counterparts (Table 2). Pore size distributions were determined using the QSDFT model, displaying an abundance of ∼1 nm wide micropores and broad mesoporosity in all networks (Fig. 2c and d).
Sample | SSABET (m2 g−1) | VP (cm3 g−1) | VMic (cm3 g−1) | VMes (cm3 g−1) | VMic/VMes |
---|---|---|---|---|---|
BP-HCP | 1748 ± 78 | 2.85 | 1.40 | 1.45 | 1.0 |
BP-HCP-25F | 1403 ± 182 | 2.38 | 1.31 | 1.07 | 1.2 |
BP-HCP-50F | 960 ± 114 | 1.66 | 0.99 | 0.67 | 1.5 |
X-HCP | 1089 ± 105 | 2.73 | 2.12 | 0.61 | 3.5 |
X-HCP-25F | 1140 ± 94 | 2.14 | 1.30 | 0.84 | 1.6 |
X-HCP-50F | 691 ± 69 | 1.43 | 1.03 | 0.40 | 2.6 |
Adsorption capacity was calculated using two methods; the first, kB, follows conventional literature approaches and considers the initial sample weight before adsorption. However, as the powdery HCPs in this work were recovered by vacuum filtration, some sample loss during filtration led to an underestimation of adsorption capacity. To correct for this loss, a second adsorption capacity, kD, was calculated using the dry sample weight after adsorption, ensuring fairer comparison between networks. The kD values were consistently only slightly higher than the corresponding kB values (Table S2) and, therefore, remain comparable to kB values in the literature. As such, kD is used in the following discussion as a measure of adsorption capacity.
The adsorption capacities of the HCPs were compared with their SSABET and VP (Fig. 3 and Table S2). In the BP-HCP networks, adsorption capacities toward toluene and methanol decreased in line with SSABET and VP. Specifically, adsorption dropped from 9.89 ± 0.49 to 3.55 ± 0.29 g g−1 for toluene and from 8.92 ± 1.52 to 3.99 ± 0.45 g g−1 for methanol, when comparing BP-HCP and B-HCP-50F. However, kD did not follow the same trend for n-heptane and DCE; although both BP-HCP-25F and BP-HCP-50F exhibited lower adsorption than BP-HCP, a slight increase in uptake was observed in BP-HCP-50F. The higher fluorine content in BP-HCP-50F may enhance DCE adsorption via halogen interactions, while also improving n-heptane uptake due to its strong hydrophobicity. The hydrophobicity of BP-HCP-50F was assessed and compared to BP-HCP by the collection of dynamic vapour sorption isotherms of both toluene and water (Fig. S5). Although BP-HCP displayed a higher total uptake capacity for both water and toluene, the ratio of toluene:
water total uptake was significantly larger in BP-HCP-50F (20
:
1) compared to BP-HCP (6
:
1), indicating increased hydrophobicity with the inclusion of fluorine.
![]() | ||
Fig. 3 Adsorption capacities kD of HCPs for different organic solvents compared to their BET-specific surface area SSABET and fluorine content. |
Among the X-HCP polymers, the adsorption capacities for all four solvents again correlated closely to SSABET and VP (Table S2), remaining similar across X-HCP, X-HCP-25F, and decreasing for X-HCP-50F. In the X-HCPs, no positive effect on adsorption capacity was observed with the inclusion of fluorine. Overall, adsorption capacities correlated more closely with porosity rather than fluorine content, reinforcing the importance of pore structure in organic solvent uptake. The solvent adsorption capacity of our best performing material, BP-HCP, is compared with various oil adsorbents in the literature in Table S3.
The adsorption capacities kD of BP-HCP and BP-HCP-25F toward distilled water were 7.89 ± 0.52 and 1.36 ± 0.23 g g−1, respectively (Fig. 4a). The water adsorption performance of BP-HCP-25F was significantly lower than that of BP-HCP, caused by the combination of a reduction in SSABET and VP, as well as the hydrophobicity of the introduced p-fluorobenzyl groups, which may hinder water infiltration into the HCP pores.24,26 Due to good apparent oil/water selectivity in isolated systems, BP-HCP and BP-HCP-25F were selected for testing in toluene/water separation experiments.
To visualise the oil/water separation process, Sudan III dye was added to toluene, and a model oil/water mixture was prepared by adding 0.5 mL of dyed toluene to 20 mL of distilled water. Both BP-HCP and BP-HCP-25F successfully adsorbed and removed the toluene from the water (Fig. 4b), demonstrating their applicability as adsorbents for oil/water separation. The adsorption efficiencies (AE) of BP-HCP and BP-HCP-25F reached up to 49.5% and 95.1%, respectively. The improved AE of BP-HCP-25F suggests that the increased hydrophobicity of the network improves efficiency in the toluene/water separation; however, this is more likely due to the addition of excess BP-HCP. It should be noted that this experiment was conducted as a proof of principle to observe oil/water separation visually. We will seek to determine the limits of oil/water separation in future work.
The separation efficiencies (SE) of BP-HCP and BP-HCP-25F were determined by measuring the weight difference of the aqueous phase before and after separation, with both samples achieving 96% (Fig. S6). To account for potential water loss, a control experiment was conducted using water alone, allowing for the calculation of the actual separation efficiencies (SEa) according to eqn (5):
SEa = 100% − SEc + SEm | (5) |
Despite the difference in oil/water selectivity between BP-HCP and BP-HCP-25F in isolated systems, the SEa was unchanged in the two-phase system, likely due to the general preference of both networks for the organic phase over water, as well as differences in experimental conditions compared with the ideal adsorption measurements.
To more thoroughly assess the impact of fluorine incorporation on oil adsorption in pure solvent systems, we also produced HCPs using trifluorotoluene (BTF) in place of pFBC in a BP-HCP series of networks (reaction scheme shown in Fig. 5a). A similar trend was observed in these networks to those discussed herein, with respect to their characterisation, adsorption of organics (Fig. 5b), and regeneration (complete data set shown in section 2 of the SI). In the BTF series, the strongly electron-withdrawing –CF3 significantly reduces electrophilic reactivity, resulting in significantly reduced incorporation into the network compared to theoretical values (Table S5). Nevertheless, fluorine incorporation into HCPs again did not appear to benefit organic adsorption and, overall, BP-HCP remained the most promising candidate for oil/water separation.
The SI includes additional experimental data, tables, and figures supporting the main text. It provides XPS-derived surface elemental compositions, FTIR spectra after long-term storage, and detailed XPS core-level spectra for all polymers. Additional TGA curves, N2 adsorption–desorption isotherms, pore size distributions, and adsorption capacity data are presented, along with dynamic vapour sorption isotherms and oil/water separation efficiency measurements. Recovery studies are detailed through FTIR and porosity analyses of reused adsorbents. Comparative adsorption performance with literature materials is tabulated. Section 2 presents synthesis, characterisation, porosity, adsorption, and recovery data for trifluorotoluene-derived HCPs, BP-HCP-BTFs. See DOI: https://doi.org/10.1039/d5lp00081e.
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