Open Access Article
Panagiota
Bika
a,
Nadia
Todorova
a,
Theopisti
Lymperopoulou
b,
Lamprini-Areti
Tsakanika
b,
Maria-Anna
Gatou
b,
Elias
Sakellis
ac,
Nikolaos
Zacharopoulos
a,
Vassilis
Psycharis
a,
Apostolos
Kalafatis
a,
Thomas
Stergiopoulos
a,
Dimitrios
Tsoukleris
d,
Evangelia A.
Pavlatou
b and
Panagiotis
Dallas
*ae
aInstitute of Nanoscience and Nanotechnology, NCSR Demokritos, 15341, Athens, Greece. E-mail: pdallas@eie.gr; p.dallas@inn.demokritos.gr; Tel: +302107273812
bLaboratory of General Chemistry, School of Chemical Engineering, National Technical University of Athens, Zografou Campus, 15772, Athens, Greece
cDepartment of Physics, National and Kapodistrian University of Athens, Athens, Greece
dNanoViis Innovative Nanotechnologies 21 El. Venizelou Str., Melissia, 15127, Athens, Greece
eTheoretical and Physical Chemistry Institute, National Hellenic Research Foundation, 11635, Athens, Greece
First published on 8th April 2026
In this work, a multi-step approach for the fabrication of a unique sponge-based platform with multiple functionalities and applications in water-remediation technologies under dynamic conditions is presented. Commercial melamine sponges were rendered hydrophobic through decoration with vinyl-terminated silane and subsequently functionalized in situ through a two-step process with a thiol-terminated covalent organic framework (COF). The materials were extensively characterized and applied for the removal of dissolved oil from emulsions and mercury cations under dynamic conditions, namely in a batch reactor under constant stirring for oil adsorption and in a flow reactor with constant metal concentration for Hg adsorption. The chemical and structural stability of the COF networks were evaluated via FTIR, EDS, and SEM analysis, respectively. An oil-removal study was conducted using a 100 ppm solution with a volume of 100 mL, was evaluated through UV-vis measurements and the results demonstrated a first-order kinetics fitted with the Elovich model, which provided the initial rate α = 0.307 mg cm−3 min−1 and desorption constant β = 0.323 g cm−3 for the active sites of the thiol-terminated sponges. The competitiveness of a series of elements against mercury adsorption was examined through dynamic absorption experiments and inductively coupled plasma optical emission spectrometry (ICP–OES). Mercury removal efficiencies of 96–99% were achieved over 300 minutes of continuous flow of a 10 ppm solution, while 77–96% removal was achieved over a subsequent 90 minutes for a 100 ppm mercury solution. The characterization analysis and the environmental remediation studies between the efficiencies of COF-modified sponges without and with the –SH terminal groups revealed the crucial role of the thiol pendant groups in the removal of both dissolved oil and mercury. The versatility of the functional material enables its dual functionality in heavily polluted aqueous environments.
Increased industrialization is also leading to pollution of aqueous resources with heavy metals such as mercury, lead, copper and zinc. Mercury is one of the most toxic heavy metals, with strict regulations for maximum contaminant levels in both water and soil. Soil can be heavily contaminated with mercury due to industrial activities, with concentrations ranging from less than 1 mg kg−1 (background levels) up to approximately 10
000 mg kg−1 in some cases.10 Modified sponges are well established as candidates for the removal of heavy metal ions (Hg2+, Pb2+, As3+, and Cd2+) from water.11 Sponges that were functionalized with biogenic methionine resins have reduced the mercury levels to 1.8–4.4 ppb from 200–400 ppb in only 15 minutes as was outlined in the work by Ali et al.12 A super-amphiphilic silicon sponge was reported to adsorb a high amount of mercury cations with concentrations at the level of 63–6231 ppm. The efficiency of the sponge is related to its porosity and the strong affinity between mercury and sulfur.13 Furthermore, a polyurethane sponge modified with reduced graphene oxide was suggested for both oil–water separation and the removal of divalent copper from wastewater.14 This nanocomposite exhibited an ∼100% removal within 2 h at a divalent copper concentration of 6 ppm. Finally, magnetic nanoparticles embedded in melamine sponges have effectively adsorbed Pb2+ and Cr6+ through electrostatic mechanisms.15
Recently, we demonstrated the ultra-efficient removal of copper cations from water using a melamine sponge decorated with a triazine-based covalent organic framework (COF) bearing terminal 4,4′-bipyridine units.16 This work was based on our previous identification of the reaction mechanism and coordination in divalent copper absorbed by COFs in their powder form.17 However, these COFs suffer from small porosity, as evidenced by BET measurements. To this end, imine-linked COFs appear as optimum systems for heavy metal removal. This subclass of covalent organic frameworks has found applications in gas storage and separation, environmental remediation and catalysis.18–20 Their organic pendant groups can be further modified with a terminal thiol that presents extraordinary ability for mercury and lead removal.21 Furthermore, by incorporating vinyl silane groups, the sponges were endowed with superhydrophobic properties, and they have been presented as an ideal system for crude oil removal,22 substantially changing the initial wetting properties and behavior of the commercial melamine sponges.23
In this work, we present a facile synthesis of an imine-based COF functionalized on hydrophobic sponges for ultra-efficient removal of heavy metals and oil from water. The in situ reaction is easily scalable with a straightforward modification of more than two (2) grams of melamine sponges in a single batch. The materials absorb crude oil dissolved in water and demonstrate an extraordinary capacity for selective mercury sorption. The former is evidenced by UV-visible spectroscopy and the latter by ICP–OES. The crucial role of the terminal thiol groups in endowing the materials with amphiphilic properties for both oil and heavy metal remediation is investigated. The complete removal of mercury cations and dissolved oil in a short period of time was explained using a first-order kinetic model of oil removal and an accurate fitting with the Elovich equation.
| Functional material | Application | Capacity | Ref. |
|---|---|---|---|
| Imine COF | Various oils | For silicone oil 150 g g−1; for toluene 125 g g−1 | 4 |
| Organosilane | Various oils | 70–120 g g−1 | 7 |
| MnO2/wood | Heavy metals | — | 11 |
| Silicone sponge | Mercury | 941.3 mg g−1 | 13 |
| Reduced graphite oxide | Copper | — | 14 |
| Triazine COFs | Copper | 0.293 mg cm−2 | 16 |
| Magnetic NPs and vinyl-terminated silica | Crude oil and heavy metals | 60–100 g g−1 for crude oil; 20.3–20.5 g g−1 for mercury and arsenic | 22 |
| Vinyl-terminated silica | Oil | 60–100 g g−1 | 24 |
X-ray diffraction was initially employed to prove the formation of a covalent organic framework on the surface of sponges. The two distinctive structures of the COF, before and after the thiol–ene coupling reaction are presented in Fig. 2a. To obtain a direct comparison with the imine COF, we performed the polycondensation reaction in the absence of sponges, which yielded the pristine powder (Powder_ctrl) and additionally a scaled-down reaction was performed employing a heating time of 24 hours in toluene (sample: Sp_ctrl). The XRD patterns of Sp_h_COF and Sp_h_COF_SH are presented in Fig. 2b, alongside the diffraction patterns of the control samples and to obtain a direct comparison with the imine COF powder (Powder_ctrl) and sponge (Sp_ctrl). The functionalized sponge Sp_h_COF exhibits the (100) reflection at 2θ = 2.73°, which corresponds to the one-dimensional channel with a 32.4 Å diameter.28 This peak is more pronounced in the two control samples, especially in the Powder_ctrl, due to the hindering effect of the sponges in the formation of a highly ordered, crystalline, framework. In comparison, the Sp_h_COF_SH samples did not demonstrate any pronounced diffraction peaks at low angles, due to a symmetry collapse after the thiol functionalization. The 28.73° peak arises from the melamine sponge.16
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| Fig. 2 (a) The chemical structure of the covalent organic framework with the pendant thiol groups and (b) the XRD patterns of Sp_h_COF, Sp_h_COF_SH and the control samples. | ||
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| Fig. 3 Images of the sponges during the 1st oil adsorption cycle in a batch reactor under constant stirring with a magnet. | ||
| Density (mg cm−3) | Sponge | COF-functionalized sponge | COF–thiol functionalized sponge |
|---|---|---|---|
| Initial | 8.5 | 51.5 | 114.0 |
| After cycle no. 1 | N/A | 34.9 | 37.3 |
| After cycle no. 3 | N/A | 24.8 | 23.4 |
The morphology of the modified sponges was evaluated through SEM analysis. The SEM images of the hydrophobic sponge (Sp_h) are published in our previous work.16 The SEM captures of the Sp_h_COF sample are presented in Fig. 4a at three different magnifications. The characteristic fibrillar network of the melamine sponge appears covered with the organic framework, while the dense network forms large agglomerates, intercalated between the fibers of the sponge. After three cycles of dissolved oil removal and clean-up procedure, it is qualitatively observed that a minor part of the weekly bound physisorbed COFs is removed (Fig. 4b), which is additionally supported quantitatively by the decline in density. A similar pattern is observed between the Sp_h_COF_SH and Sp_h_COF_SH_3c samples as well. After the functionalization with the 1,2-ethanedithiol, their morphology remained the same with the network lined up in large aggregates, intercalated between the channels of the melamine sponge (Fig. 4c). However, Sp_h_COF_SH_3c clearly demonstrates a reduced loading of the organic framework agglomerates (Fig. 4d). This indicates that after the oil adsorption and the subsequent purification process, the thiol-modified frameworks that were physiosorbed on the melamine are removed. These findings coincide well with the calculations performed for the reduced density values, outlined in Table 2.
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| Fig. 4 SEM images of (a) Sp_h_COF (i) and Sp_h_COF_3c (ii); (b) Sp_h_COF_SH (i) and Sp_h_COF_SH_3c (ii). | ||
EDS was employed to qualitatively and quantitatively identify the composition of the adsorbers. The focus is shed upon the thiol-terminated sponges before and after the oil adsorption process, since this is the system with the superior performance in the water remediation tests, as it will be discussed in the following sections of the present work. The representative EDS spectra can be seen in Fig. 5a, while the atomic and weight percentages derived from two different regions are shown in Fig. 5b and c and summarized in Table S1. The weight and atomic percentages of sulphur are reduced from 14.92 and 6.73% to 7.88 and 3.34%, indicating that a fraction of weakly physisorbed COFs is removed during the sorption cycles. However, it unambiguously proves that the thiol groups remain in a reasonably large percentage even after three oil removal cycles, which demonstrates the potential of the material in real-life applications.
To further evaluate the influence of the adsorption and desorption oil procedures upon the material, we examined the functionalized sponges through diffuse reflectance and UV-visible spectroscopy. Their respective diffuse reflectance spectra are demonstrated in Fig. S1 and by considering a direct band gap29 for the covalent organic frameworks, the Tauc-plots are obtained and presented in Fig. 6, along with the derived energy band gaps. The Sp_h_COF exhibits a band gap of 2.38 eV, which remains practically the same after the 3rd cycle of adsorption, with Sp_h_COF_3c at 2.43 eV. An important enhancement of the gap from 2.38 eV of the Sp_h_COF to 2.46 eV with the successful thiol termination in Sp_h_COF_SH is demonstrated due to the presence of non-conjugated aliphatic chains of the thiol. Finally, only a minor increase in the band gap till 2.56 eV is observed for Sp_h_COF_SH_3c, most likely due to the presence of the non-conjugated oil contaminants. These values greatly match those reported in the literature for imine-linked COFs.30 A similar increase of the band gap upon methylation of the side chains has been previously observed by Dautzenberg et al. for a series of COFs,30 where their band gaps fluctuated in the range of 2.54–2.93 eV. These observations prove that the COF remains intact during the multi-cycle oil adsorption process.
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| Fig. 6 Tauc-plots derived from the diffuse reflectance spectra of Fig. S1 for the following samples: Sp_h_COF; Sp_h_COF_3c; Sp_h_COF_SH_3c. The band gaps are indicated in the plot. | ||
The wetting behavior of the functionalized sponges was carefully evaluated through contact angle measurements. Representative images of the three samples with a water drop on their surface can be seen as an inset in Fig. 7, showing their intense orange-brown color and their texture. In Fig. 7, the contact angle images are presented for the Sp_COF and Sp_COF_SH samples before and after the first and third cycle of oil adsorption and desorption. The as-made Sp_h_COF and Sp_h_COF_SH samples demonstrate a strikingly different behavior, with the former having a hydrophobic character with a contact angle of 129°, while the latter has a hydrophilic behavior. However, a superhydrophilic response after a modification with an –SH bond has already been demonstrated in fabrics due to a combination of change of the roughness, van der Waals forces, and weak hydrogen bonding with water. Li et al. compared the wetting behavior of water droplets on a pristine fabric and a thiol–ene/silica hybrid-decorated fabric.31 The water droplets on the pristine fabric had a WCA of 86.4°, while on the thiol–ene/silica hybrid fabric, water permeated and spread out completely, notably, within 0.36 s. Similarly, in ref. 27 a drastic decline of hydrophobicity was observed, due to changes in the micro- and nano-roughness of their system. It is known that sulfur has a hydrophobic character, while –SH is more hydrophilic and polar due to its capacity to form H-bonds with water. Depending on the environment, redox conditions can convert the wetting behavior of –S-containing groups.32 Thus, an amphiphilic character, dependent on the surrounding environment and protonation/deprotonation processes (from thiol to thiolate) may be activated. Following the oil adsorption and desorption cycles in this study, the sponges demonstrate hydrophobic behavior, with a contact angle reaching the value of 140.45° for the Sp_h_COF_SH_3c sample and 131.60° for Sp_h_COF_3c (Fig. 7c). In that case, the abundant hydrophobic characteristics of the interior layer in synergy with strongly adsorbed aliphatic or aromatic molecules from the crude oil led to the water-repelling characteristics, observed in the water drop experiments.33 To further evaluate the hydrophobic/hydrophilic properties of the materials, a control experiment was conducted, where the COF powders were removed from the sponges with and without thiol groups, and were dispersed in water. The striking difference between a profound hydrophobic behavior in the powder without the thiol and a stable suspension in the powder with the thiol groups can be seen in Fig. S2.
Vibrational spectroscopy was applied to identify the structure of organic precursor molecules and polymers. The FTIR spectra of the synthesized Sp_h_COF and Sp_h_COF_SH samples before and after oil removal experiments are presented in Fig. S3 to demonstrate the successful synthesis and the chemical stability of the covalent organic frameworks on the hydrophobic sponges, and the spectra of the Tab and Dva precursors are presented in Fig. S3c. In Fig. 8, the spectra of the COF-functionalized sponges, Sp_h_COF, Sp_h_COF_SH, and Sp_h_COF_SH_3c are presented alongside the spectrum of the pristine sponge. The COF-functionalized sample demonstrates new peaks assigned to the –C
N– and –C
C– double bonds at 1591 and 1517 cm−1 (ref. 34) and the disappearance of the N–H (peaks at 3432 and 3352
cm−1) related to the Tab as well as the modes at 2700–2780 cm−1 characteristic of the aldehyde hydrogen of Dva.4 The peak at 1683 cm−1, which is characteristic of the aldehyde carbon–oxygen double bond, is also present in the pristine sponge. In Fig. S3c, we compare the FTIR spectra of the pristine Tab and Dva precursors with that of the Sp_h_COF sample. While the peak intensity increases in the Sp_h_COF material, which signals some unreacted aldehyde, the rest of the spectrum is markedly different with the precursor molecules. After their functionalization with dithiol, the vibration peak of the –S–H bond rose in the 2500–2600 cm−1 region (Fig. S4) with a weak intensity. It is important to note that the characteristic peak of the S–H group is notoriously elusive35 and, in general, exhibits a very low intensity due to the low polarity of the thiol group. In the case of the thiol-functionalized sample, after the third oil removal cycle, a significant intensity loss of the characteristic peaks assigned to the COF molecules is observed in the FTIR spectrum, which is in accordance with the fewer population of the agglomerates observed in SEM. The Raman spectra at green light excitation showed a fluorescence from all samples.
![]() | (1) |
In Fig. 9a, the decrease of the A/A0 with time is presented for the Sp_h_COF and Sp_h_COF_SH samples, while the data regarding the pristine sponge are presented in Fig. S8. The visible light absorbance was recorded at selected time intervals for a period of 350 minutes, and the final measurement took place after 1440 minutes (24 hours). The Sp_h_COF_SH sample completely removed all the dissolved oil, in contrast to the Sp_h_COF sponge. The quantitative analysis clearly demonstrates the crucial role of the thiol functional group for effective oil adsorption. The pristine sponge absorbs mainly water and minor fractions of oil, while the COF-functionalized, hydrophobic sponge, removes oil following a linear decrease of the absorbance value. In contrast, the thiol-modified sponge demonstrates a rapid, exponential decrease of visible light absorbance, related to the oil removal. The Sp_h_COF_SH adsorption curve shown in Fig. 9b follows a first-order kinetic model and the fitting model using eqn (2).
ln Ct = −k·t + ln C0 | (2) |
The linear fit, with an excellent adj-R-square = 1, results in a rate constant k = 0.01037 min−1 and an initial concentration C0 = 92.5 ppm. The first-order kinetic model of the process indicates that all adsorption sites have equal energy and chemical properties.
In Fig. 9c, the adsorption capacity, qm in mg cm−3, of the Sp_h_COF and Sp_h_COF_SH samples for three subsequent oil adsorption and desorption cycles is demonstrated. Clearly, the exponential increase of qm for the thiol-terminated COF is gradually reduced to a linear response after subsequent cycles. At the third cycle, both the pristine and the thiol-terminated samples present an identical behavior, which coincides well with the lower percentage of sulfur as demonstrated by the EDS analysis. In order to explain these results, we examine the composition of the crude oil. Crude oil itself contains sulfur, thiols, as well as metals that have a high affinity with the –S–H group.37,38 Furthermore, the functionalization with 1,2-ethanedithiol inherited the sponges with two additional hydrocarbon groups. Hence, we assign the high efficiency of the Sp_h_COF_SH sample to the combination of the above-mentioned factors.
Additionally, the kinetics of the adsorption were described through a widely used equation, which represents the Elovich model. The equation of the Elovich kinetic model is described using the following equation:
![]() | (3) |
In general, crude oil sorption is a complex process involving physisorption through weak van der Waals forces, strong chemical interactions (i.e. chemisorption) through the functional groups of the organic molecules and sulfur and metal components and pore diffusion, with the latter being in general the rate-determining step.41,42
The linear fitting using the Elovich model provides the following values: α = 0.307 mg cm−3 min−1 and β = 0.323 g cm−3. The α parameter represents the initial adsorption rate and indicates how quickly the adsorption process begins, while the β constant is related to the extent of surface coverage and the activation energy for the sorption.43 Additionally, the data were fitted using the Bangham model, a diffusion kinetic model of substances within the pores of the adsorbent while a reaction happens at the liquid/solid interface. The Bangham model with an adj-R square = 0.9, in Fig. S10, indicates that the mass transfer is limited and diffusion is not the rate-determining step.
333 mL g−1) have been observed for functionalized metal–organic frameworks such as the well-known MOF 808.44
The metal removal capacity of the composite sponges was evaluated under dynamic adsorption experiments, which are considered closer to real-life applications compared to static experiments. As a control experiment, the functionalized sponge with the imine COF was studied initially prior to the thiol modification. These nitrogen-rich COFs have been previously demonstrated to be efficient absorbers for mercury cations.45 For the experiments of this study, an aqueous solution of mercury nitrate and a multielement standard solution that contains 27 different elements were utilized. The pH of mercury nitrate and of the multielement solution was 3.5 and 1, respectively. It is considered that the pH greatly influences mercury behavior and its solubility in water. At very low, acidic pH levels, mercury is predominantly in the form of “free” divalent cations, i.e. Hg2+. As the pH levels increase, the hydroxide HgOH− form dominates. Thus, the dominant mercury species in the solution are Hg2+ at pH < 3.0, and Hg(OH)2 at pH > 5 and both species alongside HgOH+ co-exist between pH 3 and pH 5.46,47 This is outlined in the chemical equations that can be seen below.
| Hg2+ + OH− ↔ HgOH+ K3 = 1010.6 | (4) |
| HgOH+ + OH− ↔ Hg(OH)2 K4 = 1011.2 | (5) |
| Hg(OH)2 + OH− ↔ Hg(OH)3− K5 = 10−0.9 | (6) |
In dilute solutions, the mercury species at different pH values are calculated according to the above equilibrium constants, and are denoted as
,
,
and
. They represent the percentages of Hg2+, HgOH+, Hg(OH)2 and Hg(OH)3−, respectively, following the trend seen in Fig. 10a.
![]() | (7) |
![]() | (8) |
![]() | (9) |
![]() | (10) |
In the experiments, we observed a drastically different behavior of the Sp_h_COF sample, where almost no mercury uptake was observed in the mercury nitrate solution, while a rapid and more efficient removal was achieved at the multielement solution (Fig. 10b). As the pH of the mercury nitrate solution is 3.5 and of the multielement solution is highly acidic with a pH = 1, and we assign this discrepancy to the inactivity of the nitrogen moieties to the successfull coordination with HgOH+ in contrast with the divalent cation. The efficiency of the system in sequestering mercury is determined by the delicate balance between metal speciation and the protonation state of the imine linkages. At pH 1, mercury exists primarily as the free mercuric ion Hg2+, which acts as a potent and “soft” Lewis acid. Due to its high polarizability, Hg2+ tends to withdraw electron density from the imine N
C bond, even when the nitrogen is already protonated RN
CR–H+. At pH 1, complete protonation of the imines strongly polarizes the N
C bond, creating an electronic environment conducive to Hg2+ entry. Mercury coordinates with nitrogen, while the framework architecture keeps the carbon protected from water-induced hydrolysis. The free, “softer” Hg2+ form allows interaction with the double bonds of the COF. These interactions stabilize the metal within the lattice. Conversely, at pH 3.5, the emergence of [Hg(OH)]+, a “harder” Lewis acid, and the lack of full imine protonation limit the binding affinity.48
Following the soft and hard acid–base theory, sulfur-containing groups are excellent candidates for the removal of mercury from aqueous solutions. Mercury, particularly in forms like Hg2+ and methylmercury, is classified as a soft Lewis acid. This large cation with a low charge density is highly polarizable. Sulfur-containing compounds, such as sulfides (S2−) and thiolates (SH−), are highly polarizable with a low electronegativity, and thus are classified as soft Lewis bases. With respect to the above, mercury has a high affinity for sulfur, leading to the formation of very stable, insoluble complexes. The reaction thermodynamics prove the high affinity of mercury to sulfur (i.e., log
K ≈ 52.7–53.3) compared to that for Hg to organic matter (i.e., log
K
=
22–28).49 Under the dynamic, continuous flow conditions the Sp_h_COF_SH samples presented a complete removal of mercury for 300 minutes when the solution had a concentration of 10 ppm (Fig. 10c). We then switched to a 100 ppm solution where a partial saturation of the capacity was observed. The material reached saturation much earlier when a multielement solution was applied (Fig. 10d) due to competition from other metal cations. Specifically, we identified the removal of lead during the experiments with the multi-element solution. A detailed study focusing on the competition between the different heavy metals, specifically on the Pb2+, would be a subject of a separate work.
In Fig. 10e, we present the images of the sponges after the dynamic experiments, where it is worth noting that the Sp_h_COF_SH sample retained its hydrophilicity with the water droplet readily spreading on its surface. The thiol-terminated sponges obtained a darker color after mercury adsorption in both single element and multi-element systems. Additionally, EDS analysis proved the presence of both sulfur and mercury, with the characteristic Hg L peaks appearing at high energies, while the Hg M and the S K peaks overlap, as expected (Fig. 10f). In the inset graph added in Fig. 10f-i, the deconvolution reveals the two distinctive peaks at 2.2 keV for the Hg and 2.3 keV for the S element. Fig. 10f-ii demonstrates the respective quantitative analysis and reveals an atomic percent of 4.29% for the sulfur element and 2.36% for mercury (see also Table S2). Before Hg(II) adsorption, the system contains higher percentages of C, N, and S elements than after the adsorption experiments, which is consistent with the physisorbed quantities drifted by the flow of the solution. Although Sp_h_COF_SH contains lower amounts of O and Si in comparison to the aftermath values of the dynamic adsorption experiment, Si values may be increased due to the exposure of the hydrophobic layer following the removal of the physisorbed molecules by solution flow, while O has its source from the Hg(NO3)2 aqueous solution. The SEM images of the three systems after the heavy metal removal application are presented in Fig. 11. It appears that the materials remained practically the same, which further strengthens their positive aspects for everyday and industrial applications. The Sp_h_COF_SH after mercury adsorption (Fig. 11b) presents a more continuous bonded network in comparison to the initial agglomerates.
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| Fig. 11 SEM images of the sponges after the heavy metal dynamic adsortion (a) Sp_h_COF/multielement solution (b) Sp_h_COF_SH/mercury solution (c) Sp_h_COF_SH/multielement solution. | ||
Supplementary information (SI): Fig. S1: diffuse reflectance spectra. Fig. S2: COF powders with and without thiol were removed mechanically from the sponges and dispersed in water. Fig. S3: video and photo of the preparation of the oil/water emulsion using a high-share emulsifier. Fig. S4: FTIR spectra. Fig. S5: image and video of the preparation of the emulsion. Fig. S6: The reference emulsions and the corresponding calibration curve. Fig. S7: video of the first oil removal cycle using the thiol-functionalized sponge. Fig. S8: Oil adsorption curve of the pristine sponge. Fig. S9: Second order kinetic model. Fig. S10: Bangham model graph. Tables S1 and S2: Quantitative EDS analysis data. See DOI: https://doi.org/10.1039/d6ma00413j.
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