3.2. Characterization and Adsorption Studies of Nonfunctionalized COFs
In order to elucidate on the formation of new linkage types, nonfunctionalized COFs were analyzed via FTIR. The spectrum of TpPa-COF (
Figure 2a, black line) was compared to those of its corresponding building monomers: TFP (
Figure 2a, purple line) and 4-phenylenediamine-Pa (
Figure 2a, blue line). This analysis allowed us to infer that the bands due to the C–H aldehyde stretching (2883 cm
–1) and N–H primary amine stretching (3375–3186 cm
–1) vibration modes, characteristic of TFP and Pa, respectively, are not present in the TpPa-COF spectrum, confirming the occurrence of the condensation reaction. Moreover, the presence in the spectrum of TpPa-COF (
Figure 2a, black line) of intense bands attributed to the C=C stretching (1578 cm
–1), C=O stretching (1600 cm
–1), and C–N stretching (1253 cm
–1) modes, and the absence of vibration modes due to the O–H stretching band (ca. 3000 cm
–1) and to the C=N stretching band (around 1650 cm
–1), corroborate the occurrence of the β-ketoenamine form of the COF. It should be stressed that both C=C and C=O bands appear at lower wavenumbers than expected probably on account of the extensive electronic conjugation of the COF, and its crystalline nature [
32]. Additionally, other COF bands emerge at 827 and 995 cm
–1, due to the
sp2 carbon C–H bending mode, and at 1520 cm
–1, possibly due to the N–H bending mode [
32]. Moreover, the FTIR spectra of the nonfunctionalized TpBd-COF (
Figure 2b, brown line) and TpBba-COF (
Figure 2b, orange line) samples proved to be very similar to TpPa-COF, with the aforementioned C=C, C=O, and C–N stretching bands, indicative of the β-ketoenamine tautomerization, appearing at the same wavenumber range.
The thermal stability of the COFs was evaluated by TGA. The TGA curves and the corresponding first-derivative curves of the nonfunctionalized TpPa-COF, TpBd-COF, and TpBba-COF are shown in
Figure 3. Comparison of the three curves allows the conclusion that the thermal degradation of all three materials occurs essentially in two steps, suggesting the breaking of the same type of chemical bonds and polymer interlayer interactions. The first degradation event occurs at 323 and 314 °C, for TpBd-COF and TpBba-COF, respectively. For TpPa-COF, however, the same degradation event happens at a significantly higher temperature (340 °C). Given that the linkage types are the same among all samples, the latter result strongly suggests a more robust interlayer packing and more favorable, higher-energy
orbital stacking interactions. In contrast, the lower stability observed for TpBba-COF may be correlated with the conformational freedom introduced in the reticulated structure by the presence of 4,4′-ethylenedianiline (Bba) as the starting monomer. Bba contains
sp3-hybridized carbons in its backbone, unlike the other diamines used, thus making the structure less thermally resistant overall. The second degradation event occurs at 462, 470, and 469 °C for TpPa-COF, TpBd-COF, and TpBba-COF, respectively. The proximity of these values once again suggests the structural similarities among the COF samples. Interestingly, the lowest degradation temperature was observed for TpPa-COF, which may indicate that the compound was the most significantly affected by the structural alterations introduced by the first degradation phenomenon [
32,
52,
56].
Specific surface areas for the nonfunctionalized COFs were obtained by nitrogen (N
2) adsorption and BET analysis.
Figure 4 shows a representative N
2 adsorption/desorption isotherm onto nonfunctionalized COFs. It can be observed that the N
2 adsorption follows a type II isotherm with a slight H1 hysteresis for all three polymers [
57]. This evidence suggests that all three COFs are mesoporous materials. In fact, by applying the BET method, we can find that the average pore diameter ranges from 7.6 to 20.8 nm, for TpPa-COF and TpBd-COF, respectively (see
Table 2). However, it should be noted that the effect of diamine size on COFs follows a different trend when the surface area is evaluated. In this case, the COF with the highest surface area—TpPa-COF—yields the lowest pore size.
BET surface area measurements suggest that the starting monomers of larger dimensions led to a less available surface area. TpPa-COF, prepared using the smallest diamine (Pa), exhibited the highest result (83 ± 2 m2 g–1), whereas TpBd-COF and TpBba-COF, built from larger diamines, exhibited smaller surface areas (69 ± 1 and 32.4 ± 0.8 m2 g–1, respectively). It is also interesting to note that there seems to be a correlation between the average pore size and the size of the starting diamine used, with a lengthier building block leading to bigger pore dimensions. However, for TpBba-COF, formed from the diamine with the largest dimensions, the lowest BET surface area and a relatively small average pore size (9.0 nm) were observed. Again, this may be due to the added conformational freedom introduced by the –CH2–CH2– linkages from Bba, resulting in a collapsed porous structure with a less accessible surface area.
The XRD patterns obtained for TpPa-COF, TpBba-COF, and TpBd-COF are shown in
Figure 5.
In the case of TpPa-COF, the most prominent peaks were observed at 4.8, 26.6, and 27.5° (
Figure 5, black line). The 4.8 and 27.5° reflections were attributed to the reflections of the (100) and (001) planes, respectively [
32]. Less intense peaks were detected at 8.8, 11.8, 12.8, and 14.7° (
Figure 5, black line). For TpBd-COF, a very strong, sharp peak was found at 5.9°, with less intense peaks emerging at 11.2, 13.2, and 27.5° (
Figure 5, blue line). Both these COFs appear to be more ordered than TpBba-COF. In fact, their XRD patterns show better-defined peaks than those seen in the XRD pattern of TpBba-COF (
Figure 5, red line). The latter sample produced an ill-defined intense peak at 5.6° and minor peaks peaking at 13.2, 26.2, and 28.4°. This difference in crystallinity may be due, in part, to the
sp3 carbon present in the Bba moiety, resulting in less rigid and, therefore, less planar 2D layers. The above XRD data obtained are in perfect agreement with the results discussed in the literature for TpPa-COF [
32], TpBba-COF [
56], and TpBd-COF [
52].
The surface morphologies of the nonfunctionalized COF materials were further evaluated by SEM.
Figure 6 shows the SEM images obtained for TpPa-COF, TpBba-COF, and TpBd-COF.
The texture of TpPa-COF (
Figure 6a) is characterized by small, homogeneous spherical aggregates (2–3 μm), sprouting from other structures of equivalent size, indicating that the growth process occurred by formation of independent polymer nuclei. The observed surface roughness is also in agreement with the high porosity, and the corresponding surface area of the material [
32]. TpBba-COF (
Figure 6b) shows varying morphology patterns, a result that suggests structural heterogeneity and mesoporosity. Different shapes are observed (from spherical and tubular to sheet-like aggregates) of varying sizes (up to 10 μm), with no apparent order. Morphology patterns for both COFs agree with the obtained BET surface areas: surface roughness and smaller average aggregate sizes lead to a higher available surface area. TpBd-COF (
Figure 6c) exhibits irregular aggregates of varying shapes and dimensions, with a highly disordered and porous surface.
The performance of nonfunctionalized COFs for the adsorption of two dyes with different charges, methylene blue (MB, cationic) and methyl orange (MO, anionic), was assessed. Based on preliminary results (not shown) and for a selective evaluation of all adsorbents, a solid/liquid ratio equal to 0.4 mg mL
−1 was chosen.
Figure 7 shows the removal efficiencies for the adsorption of the two dyes on TpPa-COF, TpBba-COF, and TpBd-COF.
TpBd-COF showed the highest removal efficiency from among the nonfunctionalized COFs, with a removal of approximately 70% toward MB. It was observed that the removal efficiencies for MO are significantly lower than those obtained for MB. Moreover, a linear relationship between the average COF pore diameters and dye removal percentage is observed; i.e., the removal efficiency increases by increasing the pore diameters of materials. This can be explained by the easier access of the pollutant to the polymer backbone by materials with wider pore lengths.
The effect of MB adsorption on the COF structure was also evaluated. SEM analyses confirmed the modification of the surface morphology of nonfunctionalized COFs after adsorption (
Figure 8).
Pre-adsorption TpPa-COF (
Figure 8a1) exhibits a “flower-like” morphology, with spherical aggregates crystallizing independently and growing “petals” from their centers. These petal-like shapes act as an anchor to redirect polymer growth [
32]. After adsorption (
Figure 8a2), the surface is significantly eroded, becoming, in general, more diffuse and less compact. A similar effect can be observed for the SEM images of TpBd-COF (
Figure 8c1,c2). Regarding TpBba-COF (
Figure 8b1,b2), no significant morphological changes seemed to occur upon adsorption.
Moreover, the TGA curve recorded for the TpPa-COF sample post-adsorption also confirms the existence of trapped MB adsorbate (
Figure S1), in particular, at 280 °C, where a slight mass loss is observed, due to MB degradation. The highest mass loss percentage also suggests that the adsorption process leads to a loss of thermal stability, which is in agreement with the loss of superficial integrity observed in SEM.
Nonfunctionalized COFs were further used as adsorbents for MB isotherm sorption studies. Two equations (Langmuir—Equation (1), and Freundlich—Equation (2)) were fitted to experimental values, and the fitting parameters are reported in
Table 3.
In general, the isotherm curves fitted the Langmuir model better, which suggests a tendentially homogeneous surface and a predominantly monolayer-controlled adsorption. The highest MB uptake was observed for TpBd-COF, with a maximum adsorption capacity of (36 ± 1) mg g
–1, according to the Langmuir model. Sorption kinetics fitting parameters can be found in
Table 4.
The sorption experiments in general were better described by the pseudo-second-order equation. This suggests that the adsorption process is mainly due to chemisorption, which means that chemical reactions between the adsorbate and adsorbent are taking place at the interface. It also suggests monolayer adsorption. Sorption isotherms and kinetics are detailed in
Figure 9.
3.3. Characterization and Adsorption Studies of Functionalized TpBd-Based COFs
TpBd-based functionalized COFs bearing –NO
2 and –SO
3H groups were prepared and characterized.
Figure 10 shows the FTIR spectra for the functionalized COFs, TpBd(NO
2)
2-COF [100%] and TpBd(SO
3H)
2-COF [100%], compared to the spectra of their corresponding starting diamines. As discussed in
Figure 2, the spectra of the COFs are characterized by the absence of diamine N–H stretching bands (3474–3360 cm
–1) (dark blue line and dark green line in
Figure 10, respectively). Comparing the nitrated COF and the corresponding starting diamine, the presence of the aromatic N–O symmetric and asymmetric stretching bands at 1337 cm
–1and 1508 cm
–1, respectively, indicate the presence of –NO
2 groups in the COF structure [
58]. Concerning the sulfonated COF (
Figure 10, dark green line) and its diamine (light green line—
Figure 10), both produce a set of bands ranging from 1247 to 1100 cm
–1 due to the S=O stretching vibration mode. The absence of the wide O–H stretching band in the COF spectrum, present in the diamine spectrum due to intramolecular hydrogen bonding, suggests an ordered polymer structure where pore wall functional groups are not mutually accessible [
49].
In order to evaluate the influence of the functionalization on the COFs’ thermal stabilities, the TGA curves of TpBd-COF and its nitrated and sulfonated derivatives were recorded and compared (
Figure 11). Interestingly, the results seem to suggest that a larger functionalization ratio (mol/mol) leads to an increase in thermal stability. The pattern found for TpBd(NO
2)
2-COF [50%] (
Figure 11a, light blue line) is very similar to that of the nonfunctionalized counterpart TpBd-COF (
Figure 11a, brown line), with degradation steps occurring at 324 and 466 °C, respectively. For fully functionalized TpBd(NO
2)
2-COF [100%] (
Figure 11a, dark blue line), the first event occurs at a much higher temperature (360 °C), resulting in a more extensive mass loss, and a second event is not observed up to 600 °C, the maximum temperature analyzed. A possible explanation is the polarization induced by the –NO
2 groups on the polymeric resonance structure, thus increasing interlayer interaction energies and consequently thermal stability. Similar conclusions can be drawn from the comparison between TpBd-COF and sulfonated COF derivatives (
Figure 11b).
A potentiometric acid–base titration was carried out to determine the pK
a values of sulfonated COFs (
Figure S2). For TpBd(SO
3H)
2-COF [100%], a mass percentage of the incorporated Bd(SO
3H)
2 monomer of 70.1% was determined (for 50.0 mg of COF sample), similar to the theoretical value (71.1%). Moreover, a pK
a of 3.88 was estimated based on the Henderson–Hasselbalch equation. For the TpBd(SO
3H)
2-COF [50%] sample, the Bd(SO
3H)
2 mass percentage of the incorporated monomer was only estimated at 22.9%, half of the expected amount (45.6%). This suggests that, during the synthesis and crystallization processes, nonfunctionalized benzidine was selectively integrated in the structure, in detriment of its sulfonated derivative. This can be attributed to the overall lower reactivity of Bd(SO
3H)
2: the bulky, electron-withdrawing –SO
3H groups make the diamine less nucleophilic and contribute to steric hindrance. A pK
a of 4.48 was obtained for the COF.
Functionalized COFs were used as adsorbents for the removal of MB and MO (
Figure 12). Removal efficiencies ranging from 73% to 96% were obtained, with –SO
3H-substituted COFs exhibiting the higher adsorption. The capture of MB, an anionic dye, increased with the degree of functionalization, whereas for MO, which is negatively charged at pH 6–7, a higher ratio of COF functionalization resulted in decreased removal efficiencies. These results point out that electrostatic interactions play a major role on the adsorption process [
59].
To have a deeper understanding on the mechanism of MB sorption onto functionalized TpBd-COF materials, the sorption isotherms and kinetics were evaluated and data are shown in
Figure 13.
The sorption isotherms were fitted by Langmuir and Freundlich equations, and data are shown in
Table 5. It is interesting to note that functionalized TpBd-COFs were more accurately described by the Freundlich model. This confirms the surface heterogeneity induced by the pore wall functionalization and the consequences it has on adsorption. The high
Freundlich parameters found additionally suggest chemisorption dynamics. The highest adsorption was determined for sulfonated TpBd(SO
3H)
2-COF [100%], with a Langmuir maximum adsorption capacity of 166 ± 13 mg g
–1, much higher than those obtained for the corresponding nitro counterparts (48 to 84 mg g
–1). In both cases, the sorption suggests the domination by chemisorption, in agreement with the pseudo-second-order best fitting to kinetics sorption data—
Table 6.
Physical properties and respective MB maximum adsorption capacities for similar COFs and related polymers found in the literature are described in
Table 7 and compared to the results observed in this work for TpBd(SO
3H)
2-COF [100%]. An overall comparison between the properties of the various adsorbents suggests that the presence of anionic groups within the porous structure is one of the key contributing factors for a high adsorption efficiency of MB, with the BET surface area of the polymer also representing an important, but less decisive parameter. For instance, TpBd(SO
3H)
2-COF [100%] exhibits a higher MB adsorption capacity than COFs with a much higher BET surface area but without anionic functionalization. In fact, the materials bearing cationic and uncharged groups exhibited the lowest adsorption results from all adsorbents [
47,
49,
60,
61]. A similar conclusion can be drawn for all other materials containing sulfonic or sulfonate groups within the porous structure [
49,
61]. Regarding nonfunctionalized polymers, a higher BET surface area seems to correlate, overall, with a higher removal efficiency. It is also worth noting the significant increase in efficiency reported by Dang and coworkers for TpBd(SO
3–) [
49]. The COF is analogous to the TpBd(SO
3H)
2-COF [100%] studied in this work—however, imidazolium salts were grafted onto the structure, and adsorption was tested at pH 9. Both modifications may explain the sharp contrast in the adsorption results reported.
In order to have further confirmation of the effect of electrostatic interactions on the adsorption process, the adsorption of different heavy metal ions (Cu(II), Pb(II), Ni(II), and Cd(II)) onto TpBd(NO
2)
2-COF [100%] and TpBd(SO
3H)
2-COF [100%], at pH 7, was further tested and data on removal efficiencies are shown in
Figure 14. From the analysis of the figure, it can be concluded that the strongest acid polymer showed a much higher efficiency overall than the nitro-substituted counterpart. Cu(II) removal percentages were similar for both materials, while Ni(II) and Pb(II) adsorption was much more significant for TpBd(SO
3H)
2-COF [100%], suggesting a higher affinity of sulfonate-bearing surfaces toward the metals. The lower results observed for the –NO
2 substituted COF may be attributed to the positive charge present in this group, partially repelling the metal ions. It is also relevant to note that, for both COFs, removal was the lowest for Ni(II) and Cd(II), possibly due to the higher ionic radii and, thus, lower charge densities.