The chemical modification of pristine Chi and Alg was achieved through a single-step reaction with methacrylic anhydride. In this context, the primary amine groups (−NH
2) of Chi or the hydroxyl groups (−OH) of Alg undergo a nucleophilic attack on the carbonyl group of methacrylic anhydride, resulting in the formation of a new amide or ester bond, respectively. To confirm and quantify the incorporation of methacrylic groups into the polysaccharides,
1H-NMR analyses were conducted. The
1H-NMR spectra used to determine the degree of methacrylation (MD%) are displayed in
Figures S1 and S2 (see Supporting Information). Signals that are useful for quantification are clearly visible, enabling the use of Equations (1) and (2). In the ¹H-NMR spectrum of MChi (
Figure S1), the methyl protons of the acetyl group of chitosan appeared as a singlet at 2.0 ppm, while glucosamine ring protons (H
2–H
6) were observed between 2.8 and 4.3 ppm. Additional peaks at 5.6 and 5.8 ppm corresponding to the introduced olefinic protons (H
a and H
b, respectively) and a distinct signal at 1.85 ppm attributed to the methyl (−CH₃) protons of the methacrylate moiety confirmed the success of the methacrylation reaction. In the ¹H-NMR spectrum of MAlg (
Figure S2), two anomeric protons of guluronic and mannuronic acid units were observed at 5.1 and 4.7 ppm, respectively. Similar to MChi, two signals at 5.8 and 6.2 ppm (H
a and H
b, respectively) corresponding to the olefinic protons and the methyl protons at 1.95 ppm of the methacrylate units were observed, corroborating again the success in the metacrylation reaction. Additionally, the degree of methacrylation (MD%) of Chi and Alg, as well as the guluronic acid content (G%) in the Alg chain, were calculated using Equations (1)–(3). The MChi sample exhibited a consistent MD% of 21%, whereas MAlg showed a significantly higher MD% of 40%, with a G% of 88%. This increase was attributed to the larger amount of methacrylic anhydride used during the methacrylation of Alg.
3.1. Electrospinning of Chitosan-Based Fibers
For the electrospinning process, different system parameters were optimized to ensure successful fiber formation. Voltage serves as a force counteracting viscosity, facilitating the formation of the Taylor cone and polymer jetting by modulating the applied electric field. Adjusting the flow rate controls the volume of solution passing through the syringe, influencing interactions within the Taylor cone and determining the polymer content in the electrospun jet. Increasing the distance between the syringe and collector enhances solvent evaporation, allowing the polymer fibers to solidify within the desired range. Additionally, variations in syringe size impact the flow rate, thereby influencing the amount of solution present in the Taylor cone [
33].
Initially, electrospinning attempts using both unmodified and methacrylated biopolymers failed to produce fiber formation (spherical particles of 0.4 ± 0.1 µm diameter). Consequently, PVA:biopolymer blend was introduced to enhance the electrospinning process and achieve successful fiber formation [
34]. The absence of fiber formation can be attributed to repulsive forces [
35]. Since Chi needed to be dissolved in an acidic environment, it formed a polycation, leading to repulsive interactions between the positive charges on the chains. These repulsive forces were stronger than the attractive forces of hydrogen bonding between hydroxyl groups, preventing the formation of fibers. Additionally, viscosity played a crucial role. In fact, unmodified Chi with high viscosity (5223 ± 612 cP) complicated the formation of a stable Taylor cone, hindering the homogeneous stretching required for fiber formation. In contrast, MChi presented a much lower viscosity (555 ± 27 cP). Despite achieving a semi-stable Taylor cone, the strength of the negative interactions was too high to allow for the fiber formation. Similarly, neither Alg nor MAlg yielded successful results due to strong repulsive forces. Based on these results, PVA was selected as a support material to enable fiber fabrication with biopolymers. To achieve this, the electrospinning process was first optimized using PVA alone. A 12.8%
w/
v PVA solution was prepared by dissolving 6.5 g of PVA in 50 mL of Millie Q water at 70 °C under constant stirring for 2 h. The solution was then continuously stirred for an additional 24 h at room temperature to ensure complete dissolution and homogeneity. Subsequently, polymer blends were prepared to obtain fibers. The SEM image of PVA is shown in
Figure S3A. To form fibers, sufficient positive interactions between the chains were necessary. In the case of PVA, these are mainly hydrogen bonds between hydroxyl groups, which need to extend in a continuous dimension (lengthwise).
Figure S3A revealed continuous, uniform, and smooth fibers with an average diameter of 0.25 ± 0.08 µm. Due to the chain lengths and the high number of hydroxyl groups, the chains can easily extend lengthwise. Moreover, the flexibility of the chains enabled a homogeneous distribution of interactions, leading to uniform fiber morphology.
In parallel, solutions containing 3.2% Chi and Alg were prepared. For this purpose, Chi was dissolved in 1 M acetic acid and Alg was dissolved in MilliQ water, and both solutions were stirred for 24 h to ensure proper dissolution. Different volumes of the PVA and Chi or Alg solutions were mixed and stirred for 24 h to achieve various mass ratios between the two components. The viscosities of the PVA:biopolymer blends highlighted a different trend: as the proportion of Chi or Alg increased, so did the viscosity due to the higher interaction density of these compounds. However, polymer concentration had a more significant effect on viscosity than their ratio. As the concentration decreased, the number of interactions and overall viscosity were reduced due to dilution.
Additionally,
Figure S3B presents the results for the PVA:Chi (2003 ± 110 cP) blend at an 8:2 ratio and 8% polymer concentration, where fibers with an average diameter of 0.19 ± 0.08 µm were obtained. These fibers showed significant diameter variations due to the stiffness of the chitosan chains, which affected the viscosity and limited homogeneity. However, with increased Chi concentration, fiber structure was lost, resulting in the formation of interconnected spheres with an average diameter of 0.41 ± 0.15 µm, along with areas lacking spherical structures. Due to the high viscosity of the solution (6492 ± 612 cP), droplets that were fully evaporated reached the collector, dissolving the spheres present in those regions. Subsequently,
Figure S3C presents the PVA:MChi blend (1112 ± 49 cP) at the same 8:2 ratio and 8% concentration, where fibers with an average diameter of 0.14 ± 0.04 µm were obtained. Using PVA:MChi blend at a 6:4 ratio, fiber structures covered with spheres with an average diameter of 0.16 ± 0.05 µm were observed. Although fibers were formed, the 6:4 ratio was not considered desirable due to the large quantity of spheres produced. Compared to the fibers, these spheres had a lower surface-to-volume ratio, reducing the number of potential interaction sites. Similar observations can be made from the trials using both Chi and MChi. As the proportion of Chi increased, the formation of fibers became more challenging due to electrostatic repulsion. In general, the effect of PVA hydroxyl groups must be enhanced to achieve sufficient attractive interactions for fiber formation.
As observed, the diameter and distribution of MChi fibers were smaller compared to those of Chi (0.14 ± 0.04 µm vs. 0.19 ± 0.08 µm). This allowed for a higher quantity of fibers to be obtained with the same polymer mass as the dispersion was higher across each fiber. Moreover, the solvent-induced voids were absent in the methacrylated product, and the number of spheres was reduced, which facilitated fiber formation. Methacrylate groups hindered amine protonation and enabled the formation of weaker hydrogen bonds since the basicity of the amide group is lower than that of the amine group. At the same time, the number of hydrogen bonds that amides can form decreased due to the steric hindrance caused by the methacrylate groups. Therefore, forming a strong polycation became more difficult, reducing ion-ion interactions and allowing the chains to come closer.
Given that MChi fibers exhibited superior morphological characteristics and the possibility to perform crosslinking, it was decided to use PVA:MChi at an 8:2 ratio with an 8% polymer concentration and vary the flow rate. The SEM images of these experiments are shown in
Figure S4 (see Supporting Information). At a flow rate of 0.2 mL·h
−1, the fiber diameter was 0.20 ± 0.06 µm; at 0.35 mL·h
−1, the diameter was 0.17 ± 0.05 µm; and at 0.45 mL·h
−1, the diameter was 0.14 ± 0.04 µm. Increasing the flow rate reduced both the number of spheres and the fiber diameter while also decreasing diameter variation. As the flow rate increased, the amount of solution moving through the syringe per unit of time also increased, intensifying the interactions within the solution. This intensification of interactions had two effects on the MChi system: (I) it increased the electrostatic repulsion due to the polycationic nature and (II) enhanced the hydrogen bonding attraction produced by PVA’s hydroxyl groups. As a result, the fibers became thinner due to the increased repulsions, but their structure remained stable during the process because of the attractive forces.
3.2. Electrospinning of Alginate-Based Fibers
Subsequently, Alg experiments were conducted. In
Figure S5A, the SEM image for PVA:Alg (602 ± 35 cP) at an 8:2 ratio and 8% of polymer concentration is presented, showing fibers with a diameter of 0.22 ± 0.05 µm. In
Figure S5B, the SEM image for PVA:MAlg (717 ± 32 cP) at same ratio and concentration is displayed, with fibers having a diameter of 0.18 ± 0.04 µm. As observed, the methacrylated product had a higher tendency to form spheres, even when using the same electrospinning parameters.
No successful results were achieved with different PVA:MAlg ratios. Instead of observing slow deposition of a film, explosive droplets or highly unstable Taylor cones were formed [
35,
36].The polyanionic nature of Alg, where the electrostatic repulsions between the carboxyl groups of the chains have sufficient strength to overcome the hydrogen bonding attractions with PVA’s hydroxyls, needed a higher proportion of PVA to achieve fiber formation.
Finally, the fibers from the same PVA:MAlg blend system using different flow rates were analyzed. Using 0.25 mL·h
−1 flow rate, fibers with a diameter of 0.21 ± 0.07 µm were obtained, while using 0.35 mL·h
−1 flow rate, the diameter of fibers diminished to 0.18 ± 0.04 µm (
Figure S6 in Supporting Information). In this case, results similar to those obtained with Chi were observed. As the flow rate increased, both the distribution of fiber diameters and the quantity of spheres decreased, while the fiber density increased. All of this occurred as the amount of polymer increased over time with increased flow, making more chains travel to the syringe tip per second, thus enhancing the number of interactions.
3.3. The Effect of Crosslinking on Electrospun Chitosan Fibers
Once fiber formation was achieved and optimized for each system and taking into account PVA’s high solubility in water, which could otherwise lead to fiber dissolution, crosslinking between fibers was performed to maintain structural integrity during water immersion. With the intended application of the membranes in mind, two different thermal initiators were used: AIBN (methanol-soluble) and V50 (water-soluble). For this purpose, only PVA with methacrylated biopolymers was analyzed as the methacrylate groups enable crosslinking, unlike the unmodified samples.
For this purpose, PVA:methacrylated biopolymer 8:2 8% solutions were treated with 5% by mass of AIBN and/or V50 related to the polymer mass to maintain a 1:2 initiator-to-methacrylate group molar ratio. In the case of AIBN, it was dissolved in a negligible volume of methanol, comprising less than 5% of the solution’s total volume. On the other hand, V50, being water-soluble, was directly dissolved with the polymers. The resulting membranes were placed in an oven to complete the reaction of the initiators: at 115 °C for AIBN and 65 °C for V50, over a period of 24 h. Additionally, crosslinking with GA was performed by exposing the thermally treated samples to the vapors of 6 mL of an aqueous GA solution for 7 days.
In
Figure 1, the crosslinked systems are observed. Adding AIBN to the PVA:MChi system and heating for crosslinking at 115 °C resulted in fibers with a diameter of 0.14 ± 0.03 µm (
Figure 1A). V50 was added and after being subjected to a thermal treatment at 65 °C for 24 h, fibers with a diameter of 0.15 ± 0.05 µm were obtained (
Figure 1B). As observed, the fiber diameter increased following thermal crosslinking. This can be explained by the structural rearrangement required by the chains. Since the radicals generated in the methacrylate groups have only one reaction site, they needed to interact with the double bonds of other methacrylate groups. Due to heat diffusion and the torsional stress of the chains, the distance between the chains increased to facilitate crosslinking.
After analyzing the impact of thermal crosslinking, the effects of chemical crosslinking using GA and dual crosslinking were examined. For this purpose, the obtained PVA:MChi and PVA:MChi + V50 fibers were exposed to GA vapor for 7 days.
Figure 1B displays the PVA:MChi 8:2 8% fibers mixed with V50 after thermal treatment. Conversely,
Figure 1C shows the PVA:MChi 8:2 8% fibers after exposure to GA vapor, with the majority of the fiber structure degraded. This degradation occurred because GA reacted with hydroxyl and amino groups, promoting crosslinking between PVA-MChi, PVA-PVA, and MChi-MChi. Given GA’s gaseous state and high diffusion capability, crosslinking within and between fibers led to a loss of overall structural integrity. On the other hand,
Figure 1D presents the fibers obtained via dual crosslinking (thermal treatment with V50 followed by GA vapor exposure) in PVA:MChi sample, resulting in fibers with a diameter of 0.27 ± 0.06 µm. It was evident that the fiber structure was maintained, alongside an increase in fiber diameter. The preservation of the structure, which did not occur with GA treatment alone, can be attributed to the initial thermal treatment. Through V50, the methacrylate groups reacted with each other, forming carbon–carbon bonds that restricted chain mobility, thereby limiting GA’s crosslinking effect to interactions between different fibers. The increase in diameter was due to crosslinking between adjacent fibers as GA promoted inter-fiber diffusion where methacrylate groups in MChi were not abundant.
3.4. The Effect of Crosslinking on Electrospun Alginate Fibers
Subsequently, the same process was applied to PVA:MAlg solutions.
Figure 2A shows the fibers obtained by adding AIBN to a PVA:MAlg 8:2 8% solution and after being subjected to thermal treatment at 115 °C for 24 h, with fibers having a diameter of 0.165 ± 0.02 µm. In this case, the morphology of the fibers was notably irregular, with spheres and melted areas visible throughout. This irregularity was due to the methanol used to dissolve AIBN, which complicated fiber formation since Alg was insoluble in methanol. The fiber diameters obtained before and after thermal treatment with AIBN showed significant similarities in both MChi and MAlg systems, with an increase in diameter and a decrease in distribution. This outcome could be attributed to the effect of temperature on diffusion: since the glass transition temperature of PVA ranges between 50 and 80 °C, the mobility of polymer chains was enhanced, facilitating their diffusion and promoting radical crosslinking between methacrylate groups. This process increased the distance between chains along the fiber due to the steric hindrance caused by the methacrylate groups. In order to use a lower temperature to form radicals, V50 was added.
Figure 2B shows the fibers obtained by adding V50 to a PVA:MAlg 8:2 8% solution, after being subjected to thermal treatment at 65 °C for 24 h with a resulting fiber diameters of 0.17 ± 0.02 µm. In this case, the theoretically expected increase in diameter was not achieved. Two different factors should be considered to explain this outcome. Firstly, a lower temperature was used for this crosslinking process compared to AIBN (65 °C vs. 115 °C), which reduced the energy available to the chains and limited their diffusion. Secondly, the initial fiber diameters before crosslinking were larger than in other cases, which may have required closer proximity between the chains to allow reactions between methacrylate groups, thereby reducing fiber diameter. On the other hand, GA vapor is used.
Figure 2C displays the fibers after exposure to GA vapor for 7 days, where significant blending between fibers was observed. Similar to the PVA:MChi fibers, the reactivity of GA with hydroxyl groups enables PVA-MAlg, PVA-PVA, and MAlg-MAlg crosslinking, resulting in crosslinking throughout the entire length of the fibers. In the case of MAlg, less structural loss was observed compared to MChi due to the higher number of methacrylate groups in MAlg, which reduced the likelihood of crosslinking via GA. Finally,
Figure 2D shows the fibers obtained through a dual crosslinking process (thermal treatment with V50 followed by GA vapor), where fibers with a diameter of 0.20 ± 0.05 µm were observed. In this case, the fiber structure is better preserved than in PVA:MChi system due to the higher degree of methacrylation in MAlg. This led to more crosslinking via V50, reducing diffusion and minimizing the impact of GA on fiber morphology. Adding GA with V50 slightly increased the diameter to 0.20 ± 0.05 µm, indicating that GA could contribute to thicker fibers due to crosslinking effects. GA alone did not yield measurable fiber diameters, likely due to insufficient fiber formation or unsuitable conditions for measurement. In summary, varying the biopolymer type, methacrylation, feed rate, and initiator type effectively controlled fiber diameter, enabling customization for specific applications.
3.5. The Effect of Water on Electrospun Membranes
After obtaining all different membranes and taking into account the aim of the study, the effect of water on the fibers was analyzed. For this purpose, the samples were placed in contact with Milli-Q water for 24 h. In all the PVA:MChi modified membranes when water contact extended to 24 h, the fibers were entirely lost. This phenomenon was attributed to the diffusion of the fibers. In fact, GA-based crosslinking did not provide significant rigidity, and the low methacrylation degree of MChi did not allow for high amount of crosslinking through V50. Consequently, the movement of the fibers induced by water was facilitated, leading to an easy loss of the overall structure.
The same procedure was followed for all PVA:MAlg membranes.
Figure 3A displays the fibers obtained through dual crosslinking (V50 and GA) after being exposed to water for 24 h. As observed, the fiber structure was preserved due to the increased rigidity provided by the dual crosslinking process. The high degree of methacrylation resulted in a significant amount of crosslinking through V50, which reinforced the fiber structure by creating crosslinking points between the fibers. Additionally, GA also formed crosslinking points between the fibers, further enhancing the structural rigidity. Moreover, the thermograms presented in
Figure 3B, obtained through differential scanning calorimetry (DSC) analysis, revealed that the membrane successfully retained the incorporated PVA, which was otherwise water-soluble, even after being immersed in water for 24 h because the fusion temperature of PVA at 200 °C was preserved. This observation underscored the effectiveness of the crosslinking process combined with the electrospinning technique, demonstrating its strong potential for developing membranes suitable for water-related applications.
3.6. Inclusion of Biocharcoal
After optimizing fiber formation and making the decision of using PVA:MAlg system, which showed generally better results, it was decided to incorporate biocharcoal at a 1% and 2% ratio relative to the polymer mass. Although the precise structure of this material was not well defined, it was observed to contain aromatic groups, as well as hydroxyl and carboxylic acid groups. Due to these features, the introduction of this product was expected to enhance the adsorption of various pollutants owing to the newly introduced interactions [
37].
Figure 4 shows PVA:MAlg 8:2 using biocharcoal as a filler. When incorporating 1% biochar without crosslinking, the biochar particles were clearly embedded within the fibers. However, upon crosslinking with V50, a more uniform distribution of fibers was observed, along with an increased presence of fibers extending across the entire particle surface. This effect was further amplified with dual crosslinking, leading to a significant enhancement in fiber distribution and density. With 2% biochar, all images revealed an improvement in fiber interconnection and an increase in the number of electrospun fibers. Notably, fiber density was higher both in the absence of a crosslinker and when using V50. However, under dual crosslinking conditions, no further enhancement was observed compared to the 1% biochar sample, suggesting a saturation effect in fiber formation.
For this reason, it was decided to study the mechanical properties of different PVA:MAlg systems using dynamic mechanical analysis (DMA). DMA results presented in
Figure 5 illustrate E′ and tan δ as a function of temperature for the alginate-based systems. The black curves correspond to crosslinker-free PVA:MAlg membrane, the red curves represent the sample subjected to dual crosslinking, and the blue curves show the performance of the sample containing 1% biocharcoal particles and subjected to dual crosslinking. All the samples exhibited a similar E′ of approximately 150–180 MPa at room temperature. The uncrosslinked sample had a slightly higher modulus, with a small decrease occurring when crosslinking the sample without or with biochar. In the case of the biochar addition, it was already reported [
38] that the addition of biochar resulted in a decrease of E’. As the temperature increased, as seen in
Figure 5, the E′ decreased due to the softening of the sample when passing from a glassy to a rubbery state. This caused an increase in tan δ at the peak of which the glass transition temperature (T
g) can be determined. Thus, the T
g of the neat Alg material was approximately 110 °C, with a rather broad peak in tan δ, while the dual crosslinked samples (red curves) tan δ peak shifted to ~160 °C. However, the pristine membrane (black curves) underwent melting at higher temperatures (around 180–200 °C), possibly due to the high PVA content. This melting disappeared when the sample was crosslinked, not only improving its thermal resistance but also, as already mentioned, making it insoluble in water.
The incorporation of 1% biochar (blue curves) into the Alg matrix did not significantly affect E′ but caused a decrease in Tg (110 °C). This decrease may be due to the incorporation of biochar affecting the crosslinking degree of the polymer. However, PVA melting was not observed due to the crosslinking effect. Comparing these systems, it was evident that dual crosslinking consistently enhanced the mechanical performance of the Alg matrix. These results highlighted the dual crosslinking method as the superior strategy for achieving high mechanical strength and thermal stability in biopolymer systems. Biocharcoal, while effective as a reinforcing filler, may be more beneficial when combined with crosslinking techniques to maximize its potential.
Additionally, DSC analysis was performed on the crosslinked samples with biochar addition (1%) to verify the effective incorporation of inorganic particles into the membranes (
Figure 6A). The appearance of new melting peaks was observed, likely due to interactions between the fibers and the biochar, demonstrating that the fillers were effectively integrated into the matrix. Furthermore, SEM analysis of the biochar-containing samples exposed to water for 48 h (
Figure 6B) revealed partial degradation of the fibers, although their presence remained noticeably evident. This effect could be attributed to biocharcoal: as the fibers formed around the particles, the diffusion of the polymer chains was hindered, reducing the efficiency of the crosslinking process and diminishing the water resistance that would otherwise be achieved in the fiber structure.
The first transition observed in both cases was due to the evaporation of water molecules trapped in the structure. The subsequent distinguishing transition was the melting temperature of PVA, which occurred at 193 ± 1 °C in the PVA:MAlg 8:2 system without biocharcoal. This temperature was lower than the typical melting temperature of PVA with an 88% hydrolysis level, which was 220 °C [
39]. This phenomenon occurred due to the interaction with Alg where the PVA-MAlg interactions weakened the PVA-PVA interactions, thus weakening the crystalline structure [
40]. Concurrently, the incorporation of methacrylate groups introduced steric hindrances during the formation of crystalline regions, further compromising the structure. In the case of the PVA:MAlg 8:2 with 1% biocharcoal, the melting temperature of PVA was observed in two stages. Initially, most of the crystalline structure was lost at 168 ± 1 °C, with subsequent melting occurring at 200 ± 1 °C. This can be attributed to the influence of biocharcoal particles, which acted as nucleation points in the fibers, transforming and weakening the crystalline structure that polymer chains could have, leading to melting at 168 ± 1 °C [
38].
Additionally, both samples (PVA:MAlg 8:2 without biocharcol and PVA:MAlg 8:2 with biocharcoal 1%) showed similar thermal degradation profiles in thermogravimetric analysis (TGA) and the derivative of weight loss (DTG) curves with slight differences in peak intensities and exact temperatures (
Figure S7 in Supporting Information). This could indicate that while they share comparable components, minor compositional or structural differences affected their thermal stability. In fact, both samples underwent multiple stages of decomposition, with primary degradation occurring in the 200–400 °C range, a secondary stage near 450–500 °C, and a stable residue forming after 500 °C. Moreover, an initial weight loss at lower temperatures was observed in both samples, which was commonly attributed to the loss of absorbed water or volatile compounds. This was observed as a minor peak in the DTG curve around 100–150 °C in both plots. This was an expected behavior in materials containing PVA and Alg, which were hydrophilic and retained some water in their structure. The main degradation was around 200–400 °C for both samples. These peaks corresponded to significant mass losses, likely due to the breakdown of the main polymeric structure. The main degradation of PVA and Alg occurred at this temperature as both structures decomposed at moderate temperatures [
41]. The presence of peaks in this range in both samples suggested the breaking of the PVA and Alg chains.
Additional DTG peaks were observed in both samples after the primary decomposition, around 450–500 °C. This could indicate the degradation of remaining high-stability fractions or more crosslinkedstructures. The sample with biochar exhibited a second peak in the region of 450–500 °C, which could indicate higher thermal stability or an additional phase of degradation. Biochar is known for its high thermal stability, and its inclusion can delay or modify the decomposition of the material, acting as a barrier and possibly increasing the amount of residue at the end of the analysis. In addition, biochar could facilitate the formation of carbonized structures that were more resistant to high temperatures. Both samples reached a plateau after 500 °C, suggesting the formation of a stable residue. The biochar sample likely had a higher residue at the end of the test (after 500 °C), which was consistent with its presence, as it is a stable form of carbon that cannot decompose easily. This elevated residue was consistent with the expected thermal behavior of materials with strong carbon content.
3.7. Adsorption of Methylene Blue
Given the intended application of these membranes for the removal of water pollutants, a crucial step in their evaluation involved assessing their adsorption and desorption capacities. After a comprehensive characterization of their morphology using SEM analysis, along with their mechanical and thermal properties, the next phase of this study focused on evaluating their ability to adsorb MB, a model contaminant commonly used in water treatment research. Subsequently, desorption experiments were conducted to determine the extent to which the membranes can be regenerated and reused. These findings provided essential insights into the feasibility of employing these electrospun biopolymer-based membranes as efficient and sustainable adsorbents for wastewater remediation. MB adsorption performance of the developed materials over time is depicted in
Figure 7A, comparing three different systems: (i) PVA:MAlg 8:2 + V50 + GA (black), (ii) PVA:MAlg 8:2 + V50 + GA + biochar 1% (red), and (iii) PVA:MAlg 8:2 + V50 + GA + biochar 2% (green). The adsorption capacity (mg/m
2) was monitored for up to 6 h, providing insights into the influence of biochar content on the adsorption efficiency.
During the initial adsorption phase (t = 1 h), the biochar free sample (black) exhibited an adsorption capacity of approximately 125 mg/m2, significantly outperforming the biochar-containing samples, which showed values around 75 mg/m2 for both 1% and 2% biochar loadings, respectively. This trend suggested that the presence of biochar initially hinders adsorption, possibly due to changes in the surface area or active site availability caused by the filler. Over time, all systems showed an increase in adsorption capacity, with the sample without biochar maintaining the highest values throughout the experiment. After 3 h, the biochar-free sample reached 250 mg/m2, while the red (1% biochar) and green (2% biochar) samples exhibited lower adsorption capacities of approximately 150 mg/m2 and 100 mg/m2, respectively. The incorporation of biochar, particularly at 2%, consistently resulted in reduced adsorption performance. After 6 h, the baseline system achieved the highest adsorption capacity, peaking at ~320 mg/m2, whereas the 1% biochar sample reached ~200 mg/m2 and the 2% biochar sample only ~150 mg/m2. The plateau observed in all samples suggests that adsorption equilibrium was reached, with the filler-free material demonstrating superior performance.
The negative correlation between biochar content and adsorption capacity might be attributed to a reduction in the active sites or possible diffusion limitations within the matrix. While biochar is generally known for its high surface area, its integration into the PVA:MAlg matrix may alter the porosity or block functional groups necessary for effective adsorption. Additionally, higher biochar loadings (2%) did not translate to improved adsorption, reinforcing the notion that the interaction between biochar and the polymeric matrix may not be fully optimized for adsorption applications.
The results indicated that while dual crosslinking (V50 + GA) enhanced the adsorption capacity of the material, the inclusion of biochar, contrary to expectations, decreased performance. Future work could explore the optimization of biochar dispersion or surface modification strategies to enhance the synergy between the biochar and the polymer matrix, potentially unlocking higher adsorption efficiencies.
The desorption performance of MB at pH 2 over 2 h from the developed materials is shown in
Figure 7B, comparing three systems: (i) PVA:MAlg 8:2 + V50 + GA (black), (ii) PVA:MAlg 8:2 + V50 + GA + biochar 1% (red), and (iii) PVA:MAlg 8:2 + V50 + GA + biochar 2% (green). The percentage of desorption capacity was monitored to evaluate the release efficiency of the previously adsorbed MB. The filler-free system exhibited a gradual increase in desorption capacity over time, reaching a maximum of 90% in 2 h, demonstrating its desorption. Alg component demonstrated a pH-dependent behavior due to its functional groups. Under acidic conditions, protonation of these groups occurred, weakening their interaction with MB as stronger interactions with the abundant H
+ ions in the medium dominated. This shift in acidity reduced the affinity between Alg and MB, improving the desorption capacity of the system. The system with 1% biochar (red) showed similar desorption behavior.
When contrasted with the adsorption performance from
Figure 7A, the 1% biochar system balanced moderate adsorption with partial desorption, offering a compromise between capacity and release control. Meanwhile, the non-filler addition system showed both high adsorption at neutral pH and high desorption at pH 2, indicating a more dynamic but less retentive behavior. At acidic pH, MB was not released from the membrane containing biochar, indicating that biochar integration could be beneficial when desorption is not desired. This makes biochar-containing membranes suitable for short-term applications where the material is intended for single use and subsequent disposal. Conversely, if the goal is to reuse the membrane, the presence of biochar may not be advantageous. Overall, these findings highlight that the incorporation of biochar, particularly at higher concentrations, enhanced the binding strength of MB to the polymer matrix, effectively preventing desorption. This characteristic is particularly valuable in applications requiring strong dye capture and stability, such as in single-use filtration systems or scenarios with a low risk of contamination. However, for applications where controlled desorption is necessary, biochar-free systems would provide a more effective solution.