Open Access Article
Bitupan Mohan
ab,
Rahul Sonkar
ab,
Sakyabmani Bharalia and
Devasish Chowdhury
*ab
aMaterial Nanochemistry Laboratory, Physical Sciences Division, Institute of Advanced Study in Science and Technology, Paschim Boragon, Garchuk, Guwahati-781035, Assam, India. E-mail: devasish@iasst.gov.in; Fax: +91 361 2279909; Tel: +91 361 2912073
bAcademy of Scientific and Innovative Research (AcSIR), Ghaziabad-201002, India
First published on 4th March 2026
The development of high-efficiency, selective, and regenerable adsorbents for simultaneous remediation of toxic heavy metals and greenhouse gases remains a growing challenge. This work reports the synthesis of a biofunctionalized graphitic carbon nitride composite (BSA-CN) through stepwise oxidation, epoxide activation, and covalent immobilization of bovine serum albumin (BSA) onto 2D g-C3N4 nanosheets. Comprehensive structural, chemical, and morphological analyses (FTIR, XRD, TGA, Raman, SEM-EDX, TEM, and BET) confirmed successful protein immobilization, enhanced surface roughness, increased porosity, and the introduction of protein-derived functional groups that significantly improve surface reactivity and adsorption capacity. The BSA-CN composite exhibited exceptional adsorption performance toward Pb2+ ions, achieving a high monolayer capacity (292.9 mg g−1), rapid uptake within 30–60 min, and strong pH-dependent interactions governed by surface charge modulation. Kinetic modeling indicates that adsorption follows a mixed physicochemical adsorption process dominated by surface complexation, best described by the pseudo-second-order and Elovich models, while equilibrium behavior fits the Redlich–Peterson and Freundlich isotherms, indicating heterogeneity and multilayer sorption. Thermodynamic analysis revealed a spontaneous and endothermic adsorption process (ΔG° < 0, ΔH° = +45.03 kJ mol−1), accompanied by increased interfacial entropy. The composite demonstrated excellent selectivity for Pb2+ over Cu2+, Cd2+ and Mn2+ and retained over 70% efficiency after five regeneration cycles, confirming strong operational durability. In addition, it was able to remove Pb2+ from real samples (lake water and surface water). Additionally, BSA-CN displayed measurable CO2 adsorption capacity that increased at lower temperatures, attributed to enhanced interactions with its hierarchical porous architecture. Overall, this study highlights the potential of protein-functionalized g-C3N4 as a versatile, bio-derived, and dual-functional adsorbent for integrated heavy-metal remediation and low-temperature CO2 capture.
Various advanced treatment methods have been applied to eliminate toxic metal ions from water including chemical precipitation, coagulation–flocculation, ion exchange, electrochemical oxidation, advanced oxidation process, membrane filtration, photocatalysis and adsorption.7–11 Although these techniques can achieve high removal efficiencies, they often suffer from several intrinsic limitations. Ion exchange resins, for instance, provide good selectivity but are expensive and sensitive to solution chemistry.12 Membrane-based processes achieve high removal efficiency but are hindered by membrane fouling and energy demands while AOP-based methods require significant operational cost and often generate secondary pollutants.13,14 These drawbacks restrict large scale applicability. In contrast, adsorption techniques have emerged as one of the most effective methods for heavy-metal removal due to their operational simplicity, cost-effectiveness, high removal efficiency, potential for adsorbent regeneration and ability to work across a wide concentration range.15–17 The performance of adsorption processes largely depends on the physicochemical properties of the adsorbent, particularly its surface area, active functional groups and structural stability.18 So far, a large number of adsorbents such as activated carbon, metal oxides, clays, and biochar have demonstrated considerable success.15,19–22 However, their limited selectivity, low surface charge tunability, and poor regeneration often hinder their long-term applicability. Moreover, enhancing the selective separation of Pb2+ is not only conducive to environmental protection but also allows the recovery of lead metal.23 These shortcomings highlight the urgent need for next-generation functional materials engineered with tailored binding sites, abundant heteroatoms, and strong chemical affinity to Pb2+.
In recent years, two-dimensional (2D) nanomaterials such as graphene oxide, transition metal dichalcogenides (TMDs) and metal–organic frameworks (MOFs) have been widely investigated.24–27 Despite their potential adsorption capacities, many of these materials involve complex synthesis routes, high production costs, and poor chemical stability under harsh conditions. In this context, graphitic carbon nitride (g-C3N4), a metal-free and nitrogen-rich polymeric semiconductor, has recently drawn significant research attention in the fields of photocatalysis, energy conversion and environmental remediation due to its nitrogen rich backbone.28–32 Its intrinsic advantages include low-cost synthesis from abundant nitrogen rich precursors, excellent chemical and thermal stability and structural tunability.33 Compared to other advanced nanomaterials, g-C3N4 offers superior stability, low toxicity risk and scalable preparation, making it suitable for sustainable water treatment applications. However, pristine g-C3N4 suffers from limited accessible active sites, moderate surface area, and strong interlayer stacking restricting its adsorption capacity. Various modification approaches have been reported to enhance the adsorption performance of g-C3N4, such as thermal exfoliation, heteroatoms doping, introducing oxygen-containing groups, and surface functionalization.30,34,35 Oxidation of g-C3N4 can produce hydroxyl and carboxyl functionalities on its surface, thereby increasing hydrophilicity and metal-binding ability.35,36 Further functionalization of pre-carboxylated or oxidized g-C3N4 surfaces introduces new chemical moieties on its surface via amide linkage or epoxidation reactions.35,37,38 Among different functional strategies biofunctionalization using biomolecules offers unique advantages because biological macromolecules inherently possess diverse functional groups capable of strong, selective bindings with metal ions.35,39,40
Biomolecules such as bovine serum albumin (BSA), collagen, casein, or engineered peptides offers a rich distribution of amine (–NH2), carboxyl (–COOH), hydroxyl (–OH) and thiol (–SH) functional groups, which can strongly interact with metal ions through complexation, electrostatic attraction, and coordination bonding.40–42 Importantly, proteins may also contribute to enhanced hydrophilicity, increased surface heterogeneity, and improved biocompatibility of the adsorbent. Bovine serum albumin (BSA), in particular, is an inexpensive, stable, and readily available protein with a molecular structure rich in amino acid residues that can act as active sites for metal adsorption.42 Its three-dimensional conformation provides a variety of binding domains, enabling selective interaction with soft and borderline Lewis's acids such as Pb2+. The immobilization of BSA onto nanomaterials can therefore significantly enhance their adsorption capacity and selectivity.44,45 In addition to metal binding, proteins also exhibit notable potential for CO2 adsorption. In biological systems, proteins such as hemoglobin naturally bind and transport CO2, forming carbamino complexes, demonstrating the inherent ability of amino groups to react with CO2.46 Beyond biological systems, emerging studies show that solid-state proteins are also capable of interacting with CO2, indicating their promise as bio-based sorbents.47 For instant, Mitsuda et al. showed that solid proteins including casein, raw silk, and gelatin can adsorb significant amounts of CO2 with high selectivity compared to other gases.46 Although several studies have modified g-C3N4 with inorganic dopants or polymers, protein-based functionalization remains largely unexplored, especially regarding how protein–polymer interactions modify surface chemistry, charge distribution, and their mechanistic effect on Pb2+ uptake and performance under varying environmental conditions (pH, dosage, temperature, and competing ions). Additionally, few reports address the broader implications of such materials in relation to CO2-driven environmental challenges or evaluate their regeneration potential over repeated use. Therefore, understanding how such biomolecular functionalization influences adsorption kinetics, isotherm behavior, and thermodynamic feasibility is essential for designing materials suited for real wastewater systems.
This study aims to develop a BSA biofunctionalized g-C3N4 composite (BSA-CN) adsorbent for efficient and selective adsorption of Pb2+ from aqueous systems. The work focuses on controlled oxidation and epoxy mediated protein immobilization onto exfoliated g-C3N4, thereby introducing abundant amino, carboxyl, and peptide coordination sites for enhanced metal binding. Comprehensive physicochemical characterization, including FTIR, XRD, Raman spectroscopy, TGA, TEM, SEM-EDX, BET surface area analysis and zeta potential measurements was performed to confirm successful structural modification and to elucidate changes in functional groups, morphology, surface area and charge distribution. Adsorption performance was systematically evaluated under varying pH, concentration, temperature, and contact time conditions, while the mechanism was elucidated using non-linear kinetic and isotherm modeling supported by thermodynamic analysis. Beyond its aqueous metal remediation, the protein modified g-C3N4 also demonstrates significant CO2 adsorption at low pressure, highlight its viability as a dual-function materials for environmental remediation.
The synthesized g-C3N4 was oxidized by using a previously reported method.25 In this technique, 1 g of g-C3N4 powder was combined with 30 mL of HNO3 in a single-neck flask and stirred magnetically for 30 minutes. After progressively adding 3.5 g of KMnO4 to the flask, the mixture was kept in an ice bath and vigorously stirred for 2 hours. The mixture was blended with 90 mL of deionized water and ultrasonically treated for 2 hours. The mixture was then stirred at room temperature for another 8 hours. To neutralize leftover KMnO4, 20 mL of a 30% hydrogen peroxide (H2O2) solution was carefully added. The white product was separated by centrifugation at 6000 rpm and washed with DI water until the pH was approximately neutral. Finally, the oxidized g-C3N4 (Ox-CN) nanosheets were produced as a white powder.
:
1 (v/v) ethanol–deionized water mixture (40 mL) using ultrasonication for 30 min to ensure uniform dispersion. The pH of the suspension was adjusted to ∼9–10 by adding 0.1 M NaOH dropwise under continuous stirring. Subsequently, 2 mL of epichlorohydrin was added dropwise to the alkaline suspension under a nitrogen atmosphere, and the reaction mixture was stirred at 50 °C for 8 h. Upon completion, the mixture was cooled to room temperature and neutralized using dilute HCl (0.1 M). The product was separated by centrifugation (6000 rpm, 10 min), washed thoroughly with ethanol and deionized water to remove unreacted epichlorohydrin, and finally freeze-dried to obtain the epoxide-functionalized nanomaterial (designated as Ep-CN).
For covalent immobilization, 100 mg of Ep-CN was redispersed in 25 mL of phosphate buffer (0.05 M, pH 8.5) containing the target protein BSA (100 mg). The reaction mixture was stirred at 37 °C for 24 h to facilitate nucleophilic attack of the primary amine group on the epoxy moieties, leading to ring opening and covalent bonding. The resulting biofunctionalized nanomaterial was collected by centrifugation, washed multiple times with deionized water to remove unbound residues, and dried under vacuum at 40 °C. The final product was designated as BSA-CN.
The adsorption capacity (Qt, mg g−1) and percentage removal (R%) were calculated using the following equations:
![]() | (1) |
![]() | (2) |
| Qt = Qe(1 − e−k1t) | (3) |
![]() | (4) |
![]() | (5) |
Equilibrium isotherm experiments were conducted by varying the initial Pb2+ concentration (10–70 mg L−1), while maintaining the adsorbent dosage at 0.2 g L−1 and pH at 7. The suspensions were agitated for 180 min to reach equilibrium. After equilibration, the adsorption data were fitted using four non-linear isotherm models: Langmuir, Freundlich, Temkin, and Redlich–Peterson (R–P) models which are expressed as follows:
![]() | (6) |
| Qe = KFCe1/n | (7) |
Qe = B ln(KTCe)
| (8) |
![]() | (9) |
All isotherm parameters were estimated using non-linear curve fitting to minimize error and avoid distortions associated with linear transformations.
![]() | (10) |
The Gibbs free energy change was calculated using
| ΔG° = ΔH° − TΔS° | (11) |
The activation energy of the adsorption process was calculated by using the Arrhenius equation as follows
![]() | (12) |
![]() | (13) |
N heterocycles. Additionally, a prominent peak was observed at 811 cm−1, attributed to the out-of-plane bending vibration of the s-triazine units. A broad absorption band centered at 3100–3300 cm−1 was also observed, resulting from terminal –NH2 and –OH groups as well as adsorbed water, which is consistent with previous reports on polymeric carbon nitride.30,36 Following nitric acid–KMnO4 oxidation (Ox-CN), significant spectral changes were observed. A new broad band in the 3050–3500 cm−1 region appeared, corresponding to the stretching vibrations of –OH groups introduced during oxidation, confirming successful incorporation of oxygenated groups.36 After epichlorohydrin-treatment (Ep-CN), the characteristic oxirane bands expected around 910–925 and 840–855 cm−1 were not clearly resolved. This absence can be attributed the inherently weak intensity of epoxy vibrations compared to the dominant heptazine breathing band at ∼810 cm−1 and partial ring-opening of epoxides under aqueous alkaline conditions, which generates chlorohydrin or diol-type linkages that do not display sharp oxirane features.48 Despite the lack of these distinct peaks, other spectral changes confirm successful surface modification. Specifically, new aliphatic C–H stretching bands appeared near 2920 cm−1, the C–O stretching region (1000–1200 cm−1) became more intense, and the broad O–H absorption diminished, consistent with consumption of hydroxyl groups. These features collectively indicate that epichlorohydrin was covalently grafted onto CN, producing a mixture of epoxy, and ether linkages. Importantly, such functionalities remain highly reactive toward nucleophiles such as amines, thereby enabling the subsequent conjugation of BSA to the nanosheets. Although the protein's vibrational modes partially overlap with the intrinsic framework peaks of g-C3N4, distinct signatures of BSA can still be discerned in the BSA-CN spectrum. The most prominent evidence comes from the amide I band (∼1632 cm−1), arising from C
O stretching of peptide linkages, while a weaker feature around 1543 cm−1 corresponds to the amide N–H bending coupled with C–N stretching.43 These characteristic features unambiguously confirm the successful conjugation of BSA onto the surface of the epoxide-functionalized g-C3N4.
The crystalline structure of the samples was investigated using X-ray diffraction (XRD), and the results are shown in Fig. 2(b). The pristine g-C3N4 exhibited two characteristic reflections at 2θ ≈ 12.9° and 27.7°, corresponding to the (100) in-plane structural packing of tri-s-triazine units and the (002) interlayer stacking of the aromatic conjugated layers, respectively (JCPD Card No. 00-066-0813). From the card number the phase of the nanomaterials was confirmed to be orthorhombic in nature. The intense peak at 27.7° indicates well-ordered stacking of the graphitic planes, while the weaker diffraction at 12.9° corresponds to the periodic arrangement of heptazine motifs.49 Upon oxidation (Ox-CN), the (002) peak becomes broader and shifts, indicating partial disruption of the π–π stacking due to the introduction of oxygen-containing functionalities, which expand the interlayer distance.36 The (100) diffraction at 13° was further weakened, supporting the loss of in-plane periodicity following oxidative treatment. The broadening of the peaks indicates that the crystallinity of the materials decreases. The intensity of the peaks slightly decreases compared to the pristine material, indicating a change in crystallite size. These results are consistent with FTIR evidence of oxygen-containing groups, which disrupt the ordered conjugated network. Notably, after BSA immobilization, the (002) reflection remained at 27.7°, suggesting that protein attachment occurs primarily through surface binding rather than significant intercalation between the g-C3N4 layers. This retention of the (002) position, together with peak broadening, supports successful BSA immobilization while maintaining the layered framework of CN. The peaks remain at the same positions, indicating that the phase of the material has not changed after modification.
Furthermore, the surface charge evolution of g-C3N4 during successive functionalization steps was monitored by zeta potential measurements (pH 7 ± 0.1) and is shown in Fig. S1. Pristine g-C3N4 exhibited a moderately negative zeta potential of −11.9 mV, arising from deprotonated edge nitrogen sites. Upon oxidative treatment (Ox-CN), the zeta potential decreased markedly to −18.2 mV, confirming the successful incorporation of oxygenated moieties (–COOH and –OH) that dissociate under neutral conditions. Subsequent activation with epichlorohydrin (Ep-CN) resulted in partial neutralization of these surface charges, reflected by a positive potential of 6 mV, as the epoxy linkers masked carboxyl/hydroxyl functionalities. Following BSA immobilization (BSA-CN), the zeta potential further decreased to −23.3 mV, consistent with the presence of BSA, which carries a net negative charge at physiological pH due to its low isoelectric point (∼4.7).50 These systematic shifts in surface charge confirm the successful stepwise modification of g-C3N4 and highlight the dominant contribution of protein adsorption to the final colloidal stability.
Subsequently, the thermal stability and organic content of the materials were examined by TGA under a nitrogen atmosphere as shown in Fig. 2(c). The pristine CN exhibited excellent thermal stability, showing negligible weight loss below 500 °C. The main decomposition occurred in the range of 540–700 °C, corresponding to the breakdown of the heptazine framework, leaving a small char residue of 5.5% beyond 700 °C.51 In contrast, the epoxide-functionalized sample (Ep-CN) displayed additional weight loss between 200 and 400 °C, corresponding to the grafted epichlorohydrin moieties introduced during the process. The overall weight loss was significantly higher than that of pristine CN, confirming the successful introduction of organic linkers onto the nanosheets. The major degradation of the g-C3N4 backbone still occurred at ∼500 °C, although with a slightly lower onset temperature, indicating that surface modification reduced the thermal stability of the framework. For the protein-functionalized sample (BSA-CN), a two-step decomposition profile was observed. The initial weight loss below 150 °C was associated with the release of bound water, followed by a clear degradation stage between 200 and 400 °C, which can be ascribed to the thermal decomposition of immobilized BSA. The subsequent mass loss at 500–650 °C corresponded to the decomposition of the underlying g-C3N4 matrix. Compared to Ep-CN, BSA-CN exhibited intermediate thermal stability, with higher residual mass at 700 °C due to the contribution of proteinaceous carbonaceous residues.
Raman spectra of pristine CN and BSA-immobilized g-C3N4 (BSA-CN), collected under 633 nm excitation, are presented in Fig. 2(d). The spectrum of pristine CN exhibits a distinct band at 690 cm−1, which corresponds to the characteristic breathing vibration of the tri-s-triazine (heptazine) units, confirming the structural integrity of the g-C3N4 framework.52 Additionally, broad features between 1550 and 1700 cm−1 can be attributed to C–N and C
N stretching vibrations within the conjugated network. Following BSA immobilization, several new Raman-active modes emerge. Peaks at 707 and 770 cm−1 arise from protein-related skeletal vibrations, while the band at 1236 cm−1 is characteristic of amide III (C–N stretching coupled with N–H bending).53 A strong and broad feature in the 1600–1700 cm−1 range is attributed to the amide-I band, arising primarily from C
O stretching of the peptide backbone. These new vibrational signatures confirm the successful immobilization of BSA on the CN surface.
The morphological changes on the surface of CN after BSA immobilization were observed by SEM and the corresponding elemental composition was confirmed through EDX analysis. SEM images of pristine CN, oxidized CN (Ox-CN), and BSA-CN are presented in Fig. 3. As illustrated in Fig. 3(a), the pristine CN displays the characteristic aggregated, layered, and crumpled nanosheet-like morphology, typical of polymeric carbon nitride obtained through thermal polymerization. The corresponding EDX spectrum (Fig. 3(a')) shows dominant signals of carbon (32.04 wt%) and nitrogen (62.19 wt%), along with a small amount of oxygen (5.77 wt%), which likely originates from surface hydroxylation or adsorbed moisture. The high nitrogen atomic percentage (59.45%) confirms the presence of tri-s-triazine frameworks containing abundant amine and imide nitrogen. Upon oxidative treatment, the Ox-CN sample (Fig. 3(b)) displays a more fragmented and rough morphology. The increase in structural roughness and agglomeration indicates partial oxidation, exfoliation damage, and formation of defect sites. This morphological evolution is consistent with the introduction of hydrophilic –OH and –COOH groups, as also confirmed by the increased oxygen content from 5.77 wt% to 10.11 wt%, in the EDS profile, confirming successful surface oxidation. Additionally, the AFM topographic image of Ox-CN (Fig. S2) shows well-dispersed, exfoliated sheets without severe restacking and the corresponding height profile indicates thickness variations in the range of ∼1.5–2.4 nm. Subsequent BSA immobilization (Fig. 3(c)) produces a further change in surface texture, with the appearance of more irregular, clustered aggregates, suggestive of protein adsorption onto the CN framework. The EDS spectrum (Fig. 3(c')) further reveals a pronounced increase in oxygen content (11.39 wt%), accompanied by the appearance of sulphur (0.31 wt%), which can be attributed to the cysteine and methionine residues in BSA. This compositional shift, together with the attenuation of the C/N ratio, provides direct evidence of protein attachment on the CN surface. These observations correlate strongly with the zeta potential results, where surface charge reversals (from −11.9 mV for CN to −23.3 mV for BSA-CN) confirmed successful stepwise functionalization. The elemental mapping images further validate the homogeneous distribution of carbon, nitrogen, oxygen, and sulphur across the BSA-CN surface. The uniform sulphur distribution is especially strong evidence of successful and consistent protein immobilization, confirming that BSA is not merely adsorbed in isolated patches but forms a uniform coating around the CN framework.
To further verify the nanoscale surface modifications induced by BSA functionalization and to complement the morphological features observed in SEM, TEM analysis was performed. As shown in Fig. S3 pristine CN exhibits stacked plate-like nanosheets with relatively smooth surfaces. The TEM micrographs of BSA-CN shown in Fig. 4 reveal aggregated, sheet-like domains with irregular edges, consistent with the layered morphology of graphitic carbon nitride. At lower magnification (Fig. 4(a), 200 nm scale), BSA-CN appears as loosely packed agglomerates of ultrathin flakes, indicating the presence of nanosheet-like structures. Increasing magnification (Fig. 4(b)) highlights the crumpled and wrinkled surface textures, which can be ascribed to both the inherent layered nature of CN and the adsorption of BSA macromolecules, leading to increased surface roughness and partial aggregation. The HRTEM image reveals that the lattice fringes of CN become less distinct, and the material exhibits diffuse contrast rather than well-ordered crystalline planes, suggesting that BSA immobilization introduces a degree of surface amorphization and disrupts the stacking order of CN nanosheets. This interpretation is supported by the selected area electron diffraction (SAED) pattern (inset, Fig. 4(c)), which displays diffuse concentric rings instead of sharp diffraction spots, confirming the polycrystalline to semi-amorphous character of BSA-CN.
![]() | ||
| Fig. 4 TEM images of BSA-functionalized g-C3N4 (BSA-CN) at different magnifications: (a) 200 nm, (b) 100 nm and (c) HRTEM image with the inset showing the SAED pattern. | ||
The nitrogen adsorption–desorption isotherms of pristine CN and BSA-CN are presented in Fig. 5. We recorded the N2 adsorption–desorption isotherms of two samples possessing different nanoparticle sizes at 80 °C under a continuous nitrogen flow for 18 hours. Both materials exhibit a characteristic type-II isotherm with a pronounced H3-type hysteresis loop at higher relative pressures (P/P0 > 0.8), which is typical of mesoporous structures originating from slit-shaped pores and irregular interparticle voids. This confirms that the fundamental mesoporous architecture of graphitic carbon nitride is retained even after protein immobilization.54 Pristine CN shows a moderate adsorption volume at low relative pressures, indicating the presence of limited micropores, followed by a gradual increase in the mid-pressure region, which corresponds to capillary condensation within the mesoporous channels. In contrast, BSA-CN exhibits substantially higher nitrogen uptake over the entire pressure range. The enhanced adsorption at low P/P0 suggests an increase in accessible surface area or pore exposure due to partial exfoliation or loosening of CN layers during BSA functionalization. The specific surface area versus pore radius for each sample is represented as a histogram in Fig. 5(b). We have obtained specific surface areas of 75.885 m2 g−1 and 132.424 m2 g−1 together with pore radii of 1.7 nm and 1.9 nm, respectively, for CN and BSA-CN samples. This enhancement is consistent with the morphological observations from TEM and SEM, where BSA deposition introduced surface roughness and disrupted the dense stacking of CN nanosheets. Such structural modifications create additional adsorption sites.
![]() | ||
| Fig. 5 (a) Nitrogen adsorption–desorption isotherms of pristine CN and BSA-CN, and (b) comparison of their BET specific surface areas and average pore radii. | ||
The influence of various initial Pb2+ concentrations (10, 30, 50 and 70 mg L−1) was investigated to evaluate the initial aqueous solution concentration as illustrated in Fig. 6(b). It was revealed that the adsorption capacity increased steadily from 49.6 to nearly 292.1 mg g−1 as the initial Pb2+ concentration increased from 10 to 70 mg L−1. Conversely, the removal efficiency declined from nearly 99.3% at 10 mg L−1 to 83.4% at 70 mg L−1. This behavior could be ascribed to progressive saturation of available active sites and high concentration of adsorbate per unit mass of adsorbent.
The adsorption capacity as a function of pH (Fig. 6(e)) mirrors the zeta potential trend. Under strongly acidic conditions (pH 3), equilibrium adsorption capacity was relatively low (∼118 mg g−1), mainly due to the protonation of carboxylate and amine groups, which weakens their ability to coordinate with positively charge Pb2+. In addition, high concentrations of H+ ions competed directly with Pb2+ for the available adsorption sites.57 With an increase in pH to 7–9, the equilibrium adsorption capacity of Pb2+ remarkably increased, raising Qe to 158.2 mg g−1. This improvement can be attributed to the deprotonation of carboxylate/amine groups and stronger coordination between Pb2+ and electron-rich donor sites in BSA (–COO−, –NH2, and –C
O). At pH 10, a decrease in Qe is observed, which is likely due to the hydrolysis and precipitation of Pb(OH)2, reducing the contribution of true adsorption. Thus, pH 6–8 represents the optimal range for BSA-CN and Pb2+ interactions.
| Kinetic models | Parameters | Values |
|---|---|---|
| Pseudo first order | Qe, exp (mg g−1) | 144.58 |
| Qe (mg g−1) | 135.61 | |
| K1 (min−1) | 5.191 × 10−2 | |
| R2 | 0.941 | |
| χ2 red | 124.48 | |
| Pseudo second order | Qe (mg g−1) | 148.42 |
| K1 (g mg−1 min−1) | 5.64 × 10−4 | |
| R2 | 0.988 | |
| χ2 red | 27.66 | |
| Elovich kinetic model | α (mg g−1 min−1) | 62.10 |
| β (g mg−1) | 0.043 | |
| R2 | 0.994 | |
| χ2 red | 13.01 |
The correlation coefficient (R2), theoretical Qe and reduced chi-square (χ2-red) parameter values were used to assess model suitability. Among the three models, the Elovich model exhibited the best agreement with the experimental data when considering R2 = 0.994 and a significantly lower value of χ2-red (13.01), followed closely by the PSO model (R2 = 0.998, χ2-red = 27.66), whereas the PFO model showed a slightly lower correlation and χ2-red (R2 = 0.941, χ2-red = 124.48). The PFO model yielded Qe = 135.61 mg g−1 and R2 = 0.941, underestimating the experimental value and suggesting that physisorption alone cannot adequately describe the system. Instead, the excellent fit of the PSO and Elovich models reflects the chemical nature and heterogeneity of the BSA-CN surface. The Qe value predicted by the PSO model (148.42 mg g−1) was closest to the experimental value. The PSO rate constant (k2 = 5.64 × 10−4 g mg−1 min−1) indicates that the adsorption process primarily follows a chemisorption mechanism, involving surface complexation or coordination between Pb2+ ions and the surface functional groups (–COOH, –NH2, and –C
O) of the BSA-modified CN nanosheets.59 The Elovich model fitting reveals notable correlations, characterized by best fit (R2 = 0.994) a significantly higher adsorption rate constant (α = 62.1 mg g−1 min−1) compared to the desorption parameter (β = 0.043 g mg−1), highlighting a strong adsorbent–adsorbate affinity and an energetically favorable adsorption process.60 This disparity implies that Pb2+ ions interact robustly with diverse functional groups (–COOH, –NH2, and amide) introduced through BSA immobilization, as evidenced by FTIR analyses, creating a variety of energetically distinct adsorption sites.
In this work, equilibrium adsorption data for Pb2+ on the BSA-CN composite were fitted into different kinds of isotherm models (Langmuir, Freundlich, Temkin, and Redlich–Peterson) to examine the underlying adsorption process. All model fittings were performed using non-linear model fit to the original Qe vs. Ce data as non-linear fitting minimizes residuals in the dependent variable (Qe) directly and provides more reliable parameter estimates and uncertainty bounds than linearization.61 The analysis of adsorption isotherms was conducted under controlled isothermal conditions of 298 K and a contact time of 180 min, sufficient to reach equilibrium. The adsorption isotherms and corresponding parameters of the Langmuir, Freundlich, Temkin and Redlich–Peterson models fitted to the experimental data are presented in Fig. 7(b) and Table 2 respectively. The fitting of the models was compared using both the coefficient of determination and reduced chi-square (χ2_red) values to ensure rigorous statistical assessment.
| Isotherm model | Model parameters | Values | |
|---|---|---|---|
| 1 | Langmuir isotherm model | qm (mg g−1) | 292.94 |
| KL (L mg−1) | 0.821 | ||
| R2 | 0.953 | ||
| χ2 red | 647.3 | ||
| 2 | Freundlich isotherm model | KF (mg g−1) (L mg−1)(1/n) | 129.23 |
| n | 3.221 | ||
| R2 | 0.997 | ||
| χ2 red | 40.64 | ||
| 3 | Temkin isotherm model | KT (L mg−1) | 35.59 |
| B | 4.342 × 10−2 | ||
| R2 | 0.977 | ||
| χ2 red | 314.67 | ||
| 4 | Redlich–Peterson isotherm model | KR (L g−1) | 2934.6 |
| aR (L mg−1)β | 20.958 | ||
| β | 0.722 | ||
| R2 | 0.998 | ||
| χ2 red | 24.34 |
Although all models showed reasonably good correlation (R2 > 0.95), significant differences were observed in their error functions. The Redlich–Peterson model exhibited the highest R2 (0.998) and the lowest χ2 red value (24.34), confirming it as the most statistically appropriate descriptor of the adsorption system, followed closely by the Freundlich model as the superior descriptor of the data (R2 = 0.997; χ2 red = 40.54). Whereas Temkin (R2 = 0.977; χ2 red = 314.67) and Langmuir models (R2 = 0.953; χ2 red = 647.3) showed comparatively larger deviations from experimental data, thus statistically rejecting the foundational assumption of purely homogeneous, monolayer coverage described by the Langmuir model.62 The R–P model, therefore, is designated as the optimal model for describing the equilibrium adsorption of Pb2+ onto the BSA composite. This statistical result is corroborated by the visual representation in Fig. 7(b), where the R–P isotherm and Freundlich isotherm curves overlay the experimental data points most accurately across the entire concentration range tested. The R–P model is advantageous because it incorporates characteristics of both the Langmuir model (when beta to 1) and the Freundlich model (when beta to 0). This hybrid nature allows it to accurately describe adsorption across a wide concentration range on both homogeneous and heterogeneous surfaces.63 The critical parameter is the exponent β, which was determined to be 0.722. Since the value lies well within the favourable adsorption range (0< β < 1), this confirms that the adsorption process is decidedly non-ideal and occurs on a heterogeneous surface. The deviation of β from unity indicates that the BSA composite surface possesses multiple types of functional groups (e.g., amino or carboxyl groups) with varying affinities for Pb2+ confirming a strong degree of heterogeneity in the binding sites. Furthermore, the strong affinity constant KR (2934.6 L mg−1) suggests that at lower concentrations, the binding is extremely favorable, indicative of specific, high-energy interactions. Further mechanistic validation was provided by the highly successful fit of the Freundlich isotherm, with parameters KF = 129.23 and n = 3.221. This corresponds to a surface heterogeneity index 1/n of approximately 0.310. Since 1/n is well below 1, this result establishes the adsorption as highly favorable and confirms that the BSA-CN composite surface is heterogeneous, implying that the sorption energy exponentially decreases as the most energetic sites are progressively occupied.64 Despite the inferior statistical fit, the Langmuir model provided the theoretical maximum monolayer capacity (Qm) of 292.94 mg g−1, confirming the synthesized material's high potential capacity for Pb2+ sequestration. Furthermore, the Temkin isotherm, with parameters KT = 35.59 L mg−1 and B = 4.342 × 10−2, suggests that the heat of adsorption decreases linearly with increasing surface coverage, indicating significant adsorbate–adsorbate interactions or competitive site occupation typical of a strong physicochemical uptake mechanism. Collectively, the isotherm data robustly conclude that Pb2+ uptake onto the BSA composite is a favorable, complex, and mixed-mode physicochemical process dominated by surface heterogeneity, where multiple functional groups contribute to binding across the concentration range. The adsorption capabilities of several other absorbents are compared in Table S3.
In addition, to examine the thermodynamic evaluation, the activation energy of the adsorption process was calculated by using the Arrhenius equation (eqn (12)) The Arrhenius plot of log
k2 vs. 1/T obtained by plotting the rate constant (k2) from the pseudo-second-order kinetic equation against temperature (298 K, 308 K and 318 K) is illustrated in Fig. S5. The plot exhibited excellent linearity (R = 0.997), confirming the temperature-dependent nature of the rate-controlling step. From the slope and intercept of the Arrhenius plot, the activation energy (Ea) and pre-exponential factor (A) were determined to be 5.592 kJ mol−1 and 53.74, respectively. A relatively moderate Ea value obtained from the slope suggests that Pb2+ adsorption on BSA-CN occurs via a chemisorption-dominated mechanism involving coordination interactions between Pb2+ ions and amino, carboxyl, and carbonyl groups of the immobilized protein. The combined thermodynamic and kinetic findings collectively establish that the adsorption of Pb2+ onto BSA-CN is spontaneous, endothermic, and facilitated by energetically favorable coordination interactions.
In order to further examine the thermodynamic properties of the adsorption process, enthalpy (ΔH, kJ mol−1), entropy (ΔS, kJ mol−1), and Gibbs free energy (ΔG, kJ mol−1) were studied in this experiment and they were calculated with the help of Gibbs and van't Hoff equations described in Section 2.7. The equilibrium thermodynamic constant (Kad) calculated at each temperature was used to determine ΔG° according to eqn (11), and the consistently negative ΔG° values (Table 3) confirm that the adsorption of Pb2+ onto BSA-CN is spontaneous at all tested temperatures. The van't Hoff plot (ln
Kad vs. 1/T) was constructed to determine the ΔH and ΔS from the slope and intercept of the linear fit based on eqn (10). As observed, the adsorption increases from 298 K to 318 K, indicating an endothermic behaviour. However, at 328 K, the thermodynamic equilibrium constant (Kad) decreases sharply suggests temperature dependent adsorption behaviour, where increased thermal energy may weaken adsorbate–adsorbent interactions, leading to partial desorption.65 Since the van't Hoff model assumes constant enthalpy over the temperature range and requires linear behaviour of ln
Kad vs. 1/T, the thermodynamic parameters were calculated using the linear temperature region (endothermic region, 298–318 K) to ensure accuracy and reliability. The positive ΔH° value (45.03 kJ mol−1) demonstrates that Pb2+ uptake is endothermic, which is consistent with increasing adsorption capacity at elevated temperatures. The high positive ΔS° value (248.34 J mol−1 K−1) indicates increased randomness at the solid–liquid interface, likely due to the displacement of coordinated water molecules and structural relaxation of the protein matrix as Pb2+ ions bind to BSA functional groups.
| Temp. (K) | ΔG° (kJ mol−1) | ΔH° (kJ mol−1) | ΔS° (J mol−1 K−1) |
|---|---|---|---|
| 298 | −29.03 | 45.03 | 248.34 |
| 308 | −31.44 | ||
| 318 | −34.00 | ||
| 328 | −30.02 | — | — |
O) groups from BSA, along with pyridinic and graphitic nitrogen of g-C3N4. These oxygen and nitrogen-donor functionalities act as high-affinity coordination sites, enabling inner-sphere complexation of Pb2+ through multidentate chelation, which is consistent with the strong pseudo-second-order kinetic fit and the moderate activation energy (Ea = 5.592 kJ mol−1) obtained from the Arrhenius analysis. The positive enthalpy change (ΔH° = +45.03 kJ mol−1) further confirms the endothermic and chemically driven nature of Pb2+ binding, requiring energy to form stable coordination bonds with the protein-derived functional groups. Additionally, SEM, TEM and BET analyses show that BSA immobilization increases surface roughness, mesoporosity, and surface area, facilitating faster diffusion and providing a larger population of accessible binding sites. The Freundlich isotherm fit (1/n < 1) indicates heterogeneous sorption sites, implying that both high-energy BSA coordination pockets and lower-energy CN defects participate in Pb2+ uptake, while the high selectivity seen in multi-ion experiments confirms the strong preference of these sites for Pb2+ over other divalent cations. Therefore, the experimental results converge to support a mechanism in which Pb2+ adsorption proceeds through (i) electrostatic attraction, (ii) surface complexation with BSA functional groups and CN nitrogen centers, and (iii) diffusion into mesopores followed by heterogeneous site occupation. This integrated mechanism aligns with similar protein-modified adsorbent systems reported in the literature, and explains the superior adsorption performance, selectivity, and thermodynamic favorability observed for BSA-CN (Fig. 9).
O, and sulfhydryl residues) present on the BSA-modified nanosheets. Pb2+ possesses high electronegativity, a large ionic radius, and a strong tendency to form inner-sphere complexes, which collectively enhance its binding affinity relative to other metal ions.66 Furthermore, the immobilization of BSA introduces heterogeneous, high-density binding domains that resemble natural metal-binding sites in proteins, thereby enhancing selective complexation. The lower uptake of Cd2+, Cu2+, and Mn2+ suggests weaker interactions due to their differing ionic radii, hydration energies, and coordination preferences. These findings confirm that the BSA-CN composite is intrinsically selective toward Pb2+, making it suitable for targeted remediation of lead-contaminated water.
Reusability and regeneration are critical parameters for any adsorbent that determine the practical and economic applicability. Therefore, reusability tests were performed for five consecutive adsorption–desorption cycles. For each cycle 20 mg of BSA-CN were added to 50 mL of Pb2+ solution with 180 rpm agitation at 25 °C for 180 min. Fig. 10(b) shows the percentage removal and desorption efficiency of Pb2+ from BSA-CN. In the first cycle the composite shows the highest percentage removal of 96.2% and a desorption efficiency of 94.9% under acidic conditions, causing the protonation of the adsorbent surface and allowing the desorption of positively charge Pb2+ ions from the adsorbent.67 A gradual decline in performance was observed over successive cycles, with removal efficiencies decreasing to 91.2%, 85.4%, 75.4%, and 69.9% in cycles 2–5, respectively, while desorption efficiency values remained relatively high (85–95%) throughout the cycle. The slight decline in adsorption capacity is likely due to partial blockage, irreversible occupation of high-affinity sites or mild protein conformational changes during repeated washing and desorption processes. To verify the structural stability of the composite after mild acid (0.1 M HCl) treatment, FTIR and zeta potential analyses were conducted after cycle 1 and cycle 3, as illustrated in Fig. S7. The FTIR spectra retained the characteristic amide I band (∼1632 cm−1) and the weaker feature of N–H bending and C–N stretching at around 1544 cm−1 of BSA without significant peak shifts and disappearance, confirming the preservation of the protein backbone structure. Additionally, zeta potential measurements showed only minor variations in surface charge values to −20.3–21 mV compared to BSA-CN (−23.3 mV) in neutral medium, indicating that the immobilized BSA layer remained chemically stable and was not significantly leached during regeneration. The slight shifts may be due to the protonation/deprotonation effect during regeneration.
The recyclability of CO2 adsorption on the BSA–CN sample was evaluated at 3 °C, as shown in Fig. S8(a and b), yielding an adsorption capacity of 23.40 cm3 g−1 in the second cycle. A minor decrease in CO2 capture was observed during the second cycle; however, the adsorption capacity remained considerable. The retention value of 6.01 cm3 g−1 suggests that the material possesses good recyclability for repeated CO2 adsorption.
Supplementary information (SI): ZETA potential graph of g-C3N4, Ox-CN, Ep-CN and BSA-CN; AFM image and corresponding height profile of Ox-CN; TEM images of as synthesised g-C3N4 and SAED pattern; Pb2+ ion adsorption comparison of CN and BSA-CN; Arrhenius plot of log k2 vs. 1/T ; SEM of BSA-CN after Pb2+ adsorption along with corresponding EDX spectra; FTIR spectra of BSA-CN after Pb2+ and CO2 adsorption respectively; FTIR spectra of fresh BSA-CN and after the 1st and 3rd adsorption–desorption cycles and corresponding zeta potential distributions after cycle 1 and cycle 3; recyclability of CO2 adsorption isotherm of BSA-CN at 276 K, equilibrium Pb2+ adsorption comparison of CN and BSA-CN; Pb2+ adsorption performance in real water samples; comparative analysis of Pb2+ adsorption capacity of BSA-CN with other materials; comparison of CO2 adsorption capacity. See DOI: https://doi.org/10.1039/d5na01167a:.
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