Open Access Article
Nafisa Tabassuma,
Raamisa Anjuma,
Papia Haque*a,
Md. Sahadat Hossain
b,
Mashrafi Bin Mobarak
b,
Md. Saiful Quddus
b,
Fariha Chowdhury
c,
Lutfor Rahmanb,
Dipa Islamc,
Samina Ahmed
*bd and
Monika Mahmud
*b
aDepartment of Applied Chemistry and Chemical Engineering, University of Dhaka, Dhaka-1000, Bangladesh. E-mail: papiahq@du.ac.bd
bInstitute of Glass and Ceramic Research and Testing (IGCRT), Bangladesh Council of Scientific and Industrial Research (BCSIR), Dr. Qudrat-i-Khuda Road, Dhanmondi, Dhaka-1205, Bangladesh. E-mail: shanta_samina@yahoo.com; monika0197@gmail.com
cBTRI, Bangladesh Council of Scientific and Industrial Research (BCSIR), Dr. Qudrat-i-Khuda Road, Dhanmondi, Dhaka-1205, Bangladesh
dBCSIR Laboratories Dhaka, Bangladesh Council of Scientific and Industrial Research (BCSIR), Dr. Qudrat-i-Khuda Road, Dhanmondi, Dhaka-1205, Bangladesh
First published on 15th November 2024
The deployment of magnetically responsive and polymeric materials to remove dyes that are hazardous in aquatic environments has profoundly revolutionized environmental sustainability. This study focuses on removing the hazardous cationic Malachite Green (MG) dye from solutions, employing a novel magnetic composite film as an adsorbent, designated as Ag0.2Co0.8 Fe2O4 (ACFCeP). The composite was synthesized via solvent casting, incorporating Ag0.2Co0.8 Fe2O4 nanoparticles and CeO2 into a cellulose acetate/polyvinylpyrrolidone (CA/PVP) polymer matrix. The Ag0.2Co0.8Fe2O4 nanoparticles were synthesized by a co-precipitation method. Comprehensive characterization of the synthesized composite was conducted using techniques, such as Fourier transform infrared spectroscopy (FT-IR), X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), field emission scanning electron microscopy (FE-SEM), and vibrating sample magnetometer (VSM). The Ag-doped cobalt ferrite component retained a strong hysteresis loop within the final composite, even when blended with the CA/PVP polymer, preserving the robust magnetic properties that facilitate the easy removal of the composite post-treatment without secondary pollution. Additionally, the mesoporous structure of the composite effectively aids in the adsorption mechanism. The isothermal study shows that both linear Langmuir isotherm and Freundlich isotherm are well fitted with R2 values of 0.99 and 0.97, respectively. The linear Langmuir maximum adsorption capacity, qmax, is 45.66 mg g−1 at pH 7. The kinetic studies of the composite resemble the pseudo-second-order kinetic model, reaching adsorption equilibrium within 70 min for a 100 ppm MG dye concentration. The composite film exhibits excellent reusability, maintaining high removal efficiency over three cycles. Overall, the ACFCeP composite film showcases excellent dye removal capabilities, a fast adsorption rate, and satisfactory magnetic properties and offers a sustainable solution for environmental pollution, thus contributing to ecosystem preservation through efficient recycling and reuse in dye adsorption applications.
000 different synthetic dyes and global annual synthetic dye production of 7 × 105 tons, out of which the textile industries discharge 3600 tons of concentrated dye waste in the natural water resources.2 The persistent, non-biodegradable synthetic dyes are responsible for making the water unsuitable for drinking, while the demand for freshwater is expected to increase from the current 4500 billion cubic meters per year to 6900 billion cubic meters by 2030.2,3 Moreover, the presence of dyes significantly alters various aquatic environmental parameters like BOD and COD, causing damage to the aquatic food chain, photosynthesis and exerting detrimental effects on aquatic life.4–6 Additionally, dyes can cause a multitude of health issues, affecting the nervous system, skin, liver, kidneys, reproductive system, and enzymatic functions within the human body.6
Among synthetic dyes, Malachite green (MG) is extensively employed in aquaculture and other industries. Initially, it was effective as a parasiticide, fungicide, and antiprotozoan agent. However, subsequent research revealed that MG is highly toxic, with its toxicity escalating with increased temperature, time, and concentration.7 Consequently, treating wastewater containing MG dye is imperative to safeguard both aquatic and terrestrial life from its acute toxicity.
Several biological, physical and chemical methods exist for the treatment of wastewater, among which adsorption stands out as a physical process. It is highly effective, straightforward, cost-efficient, energy-conserving, and easy to operate.8 Ongoing research aims to develop superior, eco-friendly, and more efficient adsorbents for maximum dye removal. In pursuit of this goal, numerous composite adsorbents are being developed to combine the most beneficial properties into a single material.
Recently, magnetic nanoparticles, particularly spinel ferrite nanoparticles (MFe2O4; M can be Fe, Ni, Co, Mn, Zn, etc.), have gathered remarkable attention because of their high surface area, exceptional magnetic properties and active sites, resulting in enhanced adsorption capacity and broad applicability.9,10 Spinel ferrite (SF) has the chemical formula AB2O4, where A occupies the tetrahedral site (e.g., Pb, Mg, Cr, Mn) and B occupies the octahedral site (e.g., Fe, Al, Cu).11 The cations at both sites are connected to oxygen atoms tetrahedrally and octahedrally, respectively.9
Among the three types of spinel ferrites—normal, inverse, and mixed—CoFe2O4 is an inverse spinel ferrite. It is a significant SF as it is chemically stable and has intrinsic magnetic, electrical, and mechanical properties.12 Cobalt ferrite possesses a mesoporous structure with moderate saturation magnetization, making it suitable as both an adsorbent and a photocatalyst for pollutant removal.13–15 Studies have demonstrated that hydrothermally synthesized CoFe2O4 exhibits one of the highest adsorption capacities to remove Congo red dye from solutions.16,17 Post-adsorption, removing adsorbents from the solution is crucial to prevent further contamination. Conventional separation methods like filtration, sedimentation, or coagulation are laborious and expensive.18 In contrast, magnetic separation is simpler, more economical, and effective, as it uses an external magnetic field to remove the adsorbent from the effluent, ensuring no additional pollution in the treated water.
Recent advancements have seen techniques such as surface modification, metal ion doping and nanocomposite preparation to enhance the adsorption capacity of ferrite nanoparticles.19 Doping cobalt ferrite with various metals and non-metals has been shown to improve coercive force and specific surface area.20,21 Significant interest is placed on Ag nanoparticles due to their high conductive nature, good catalytic performance and wide range of antibacterial actions.22 Many works have proved the enhancement of the adsorption capacity for both cationic and anionic dyes after the addition of Ag nanoparticles to materials, including CoFe2O4.23–25
Moreover, as a rare earth metal oxide, cerium oxide is characterized by its cubic crystal structure and has demonstrated a remarkable ability to enhance dye adsorption capacity. This enhancement is attributed to its high surface area, affordability, water solubility, catalytic properties, and chemical reactivity.26–28 Thus, integrating cerium oxide into composite films can markedly boost their dye adsorption efficiency.
Other than the nanoparticles, natural polymers are gaining attention due to their biodegradability, non-toxicity, flexibility, and eco-friendliness.29 Cellulose acetate (CA) is one of these and has been found to have wide applicability as an adsorptive polymer matrix because of its biocompatibility, low cost, film-forming ability and simple preparation.30–32 It has been functionalized with different organic and inorganic materials and showed better performance in removing different dyes.33,34 A study has also reported the fabrication of ferrite in CA to adsorb methylene blue.35 The film formation ability of CA facilitates better adsorption by improving the surface area.32
Even synthetic polyvinylpyrrolidone (PVP), a non-ionic, biodegradable, non-toxic, hydrophilic polymer, is also known for its excellent film-forming properties.36–38 PVP binds with nanoparticles, preventing aggregation and providing stability and effectiveness.39–41 It also increases the dye adsorption capacity by creating a porous film.42
This research endeavors to engineer an innovative composite film that amalgamates Ag-doped cobalt ferrite, cerium oxide, cellulose acetate (CA), and polyvinylpyrrolidone (PVP). By proposing a heterostructured composite film, we aim to prevent the aggregation of powdered materials, thereby enhancing its efficacy. Comprehensive analyses, including XPS to observe the interactions and crosslinking, along with N2 gas adsorption–desorption for assessing the surface area and pore size, have been meticulously conducted. Furthermore, VSM was utilized to determine the magnetic responsiveness of the composite. Additionally, adsorption isotherms and kinetic models have been scrutinized to elucidate the adsorption method. Emphasizing the magnetic properties of cobalt ferrite, this study highlights its pivotal role in environmental pollution mitigation. The reusability of the composite across multiple cycles is also rigorously assessed, underscoring its potential for sustainable and eco-friendly applications in protecting our ecosystem.
| Co(NO3)2·6H2O + 2Fe(NO3)3·9H2O + NaOH → CoFe2O4 + 8NaOH + 8NaNO3 + 28H2O | (1) |
Ag0.2Co0.8Fe2O4 nanoparticles (AgxCo1−xFe2O4; x = 0.2) were synthesized in the same manner described previously by adding 0.4 M 50 mL Fe(NO3)3·9H2O and 0.16 M 50 mL Co(NO3)2·6H2O solution with 0.04 M 25 mL AgNO3 salt solutions. The preparation procedure is represented in Scheme 1a.
:
1, v/v) under continuous stirring for 30 min in a fume hood. Similarly, 2% polyvinylpyrrolidone (PVP) was dissolved in 10 mL of acetone/DMF (4
:
1, v/v) and also stirred for 30 min in the fume hood. These two solutions were then mixed together and stirred continuously for 1 hour to ensure homogeneity. The stirring was conducted inside a fume hood to ensure the safe exhaustion of the evaporated solvent. Next, 12.5 wt% of Ag0.2Co0.8Fe2O4 (ACF) nanoparticles and 2 wt% of CeO2 powder (based on the total weight of solid polymers) were added to the CA/PVP mixture. A further stirring for 2 h was continued by placing the solution in a fume hood at room temperature. The resulting polymer solution, now containing finely dispersed ACF nanoparticles and cerium oxide, was carefully poured into a 60 mm diameter Petri dish. It was then naturally air dried at room temperature at 22 ± 5 °C and 35 ± 5% relative humidity in a well-ventilated area for 24 h. The remaining organic solvent slowly evaporated during this period, generating pores in the film. After 24 h, the dried Ag0.2Co0.8Fe2O4/CeO2/CA/PVP (ACFCeP) composite film was obtained by carefully peeling it off the Petri dish. The resulting film had a uniform thickness. As a comparison, a blank CA/PVP film (without ACF and CeO2) was also prepared to evaluate the dye removal efficiency of the composite. Scheme 1b illustrates the preparation process of the composite film.At equilibrium, the solutions were allowed to settle, and the MG-loaded composites were separated. The remaining equilibrium concentration of MG in the solutions was calculated by measuring the absorbance at 617 nm (λmax of MG) in a UV-vis spectrophotometer and via the calibration curve of MG.
The removal percentage of the dye was determined using the following formula:
![]() | (2) |
The amount of adsorbed Malachite Green per gram of the adsorbent (qe) was calculated according to the following equation:
![]() | (3) |
000 to 20
000 Oe was applied at room temperature for the analysis.The linear and non-linear forms of Langmuir isotherms are represented by eqn (4) and (5), respectively.43
![]() | (4) |
![]() | (5) |
Freundlich isotherms in the linear and non-linear forms are presented by eqn (6) and (7), respectively.44
![]() | (6) |
![]() | (7) |
Dubinin–Radushkevich isotherm is used to determine whether the adsorption process undergoes physisorption or chemisorption. The linear and non-linear forms of the D–R isotherm are shown in eqn (8) and (9), respectively.45
ln Qe = ln Qm − βDRε2
| (8) |
| Qe = QmeβDRε2 | (9) |
![]() | (10) |
![]() | (11) |
Eqn (12) and (13) represent the linear and non-linear forms of Temkin equations, respectively.46
qe = A ln KT + A ln Ce
| (12) |
qe = A ln(KTCe)
| (13) |
![]() | (14) |
The dye adsorption rate is dependent on both the contact time and diffusion process between the adsorbate and the adsorbent.47 The adsorption process happens in two specific steps. In the first step, molecules migrate from the aqueous dye solution towards the adsorbent, and in the next step, diffusion on the adsorbent surface occurs.48 To understand the adsorption kinetics of the ACFCeP film, Lagergren pseudo-first-order equation, pseudo-second-order equation and Elovich model were assessed. The linear and non-linear pseudo-first-order equations are given in eqn (15) and (16), respectively.49
ln(qe − qt) = ln qe + K1t
| (15) |
| qt = qe(1 − e−K1t) | (16) |
The linear and non-linear forms of the pseudo-second-order model are shown in eqn (17) and (18), respectively.50
![]() | (17) |
![]() | (18) |
Eqn (19) and (20) present the linear and non-linear Elovich kinetic models, respectively.51
![]() | (19) |
![]() | (20) |
![]() | ||
| Fig. 1 XRD pattern (a) and FTIR spectra (b) of cobalt ferrite, Ag-doped cobalt ferrite, CA/PVP blend and ACFCeP composite. | ||
The FTIR spectra of cobalt ferrite, Ag-doped cobalt ferrite, CA/PVP and the ACFCeP composite are demonstrated in Fig. 1b. In the spectrum of cobalt ferrite, the higher frequency absorption peak at 592 cm−1 and 556 cm−1 indicates the vibration of the tetrahedral metal oxide (M−O, M = Fe, Co) site and the lower frequency absorption peak at 425 cm−1 indicates the vibration of octahedral M−O of the spinel structure of cobalt ferrite.61,62 As Ag was doped in the cobalt ferrite, the characteristic peak of Ag–O is observed at 548 cm−1.63
In the CA/PVP blend, the stretching vibration of O–H at 3413 cm−1, bending of the C–H group at 1425 cm−1 and asymmetric stretching vibration of the C–H group at 2963 cm−1 resemble cellulose acetate.64,65 Moreover, the symmetric stretching of C
O from the COO− bond of CA is observed at 1746 cm−1.54 The CA/PVP spectrum also shows C–O stretching from the acetate group and stretching of the C–O–C group from cellulose at 1235 cm−1 and 1043 cm−1, respectively. The bands observed at 1287 cm−1 and 1651 cm−1 are attributed to the C–N stretching of the pyrrole structure and C
O stretching of the lactam ring from PVP, respectively.66
In the spectrum of the composite film, all the characteristic peaks of its components are present, indicating the successful preparation of the composite. Notably, in the ACFCeP composite, the peak observed at 487 cm−1 represents the Ce–O group from cerium oxide incorporated into the composite.67,68
The major peaks observed around 285.92 eV, 532.87 eV, and 399.9 eV are attributed to the C 1s, O 1s and N 1s spectra, respectively.69 The C 1s of the composite were deconvoluted into three peaks placed at 284.86, 286.27, and 288.35, eV (Fig. 3a) allocated to C–C, O–C–O, and O–C
O, respectively.70,71 After adsorption, the binding energy shifted to 284.92, 286.64, and 288.82 eV (Fig. 3b) due to the π–π interaction of the dye with the aromatic ring of the composite polymers. The O 1s spectra of the composite show the functional O–H and O
C groups at 532.23 eV and 529.34 eV (Fig. 3c).71,72 After dye adsorption, the O 1s is shifted to 532.63 and 529.65 eV (Fig. 3d) due to the electrostatic interaction of the dye with the composite. In Fig. 3e, N 1s spectra before MG adsorption are deconvoluted into three peaks at 399.92, 398.55, and 404.58 for N–O, C–N/C
N, C–N bonds, respectively, whereas after MG adsorption (Fig. 3f), peaks appear at 399.86 and 404.95 and the peak at 398.55 disappeared (Table S2†).
In dye adsorption, nitrogen atoms can donate electrons to the metal centres; therefore, their electron cloud distribution changes, which explains the disappearance of the peak at 398.55 eV. Similar peak disappearance after adsorption is also reported by P. Du et al.73 Also, the disappearance of the 398.55 eV peak after MG adsorption is likely due to the surface sensitivity of XPS, which detects only the topmost 10 nm. On the other hand, with a pore diameter of 14.85 nm, our prepared mesoporous composite allows dye molecules to adsorb deeper, which is beyond XPS detection. These may also explain the absence of a peak at 398.55 eV. Moreover, the atomic percentage of N 1s decreased from 4.24% to 1.19% after MG adsorption (Table S1†). The decrease in N 1s intensity after adsorption can be explained by the charge transfer mechanism between the nitrogen atoms in Malachite Green and the metals in the composite (i.e. Ce Ag, Co, Fe). The nitrogen atoms in the dimethylamino groups of Malachite Green possess lone pairs of electrons, which can act as electron donors. Meanwhile, Ce4+, with its high oxidation state and available empty 4f orbitals, can serve as an electron acceptor. This creates a charge transfer interaction, where nitrogen donates electron density to the empty 4f orbital of cerium. From the XPS spectrum of Ce 3d (Fig. 4a), it is observed that there are six distinctive peaks of Ce 3d divided into two groups of V and U types, linking to the two states Ce 3d5/2 and Ce 3d3/2.74 Before adsorption, the peaks denoted as V (882.63 eV), V″ (898.45 eV), U (900.34 eV), and U″ (916.44 eV) were attributed to Ce4+ and u′ (904.32) and v′ (885.43) for Ce3+.75,76 These peaks confirm that in the composite, both cerium Ce3+ and Ce4+ states are present. After adsorption, the Ce4+ binding energy shifted from 882.63 to 881.76 eV, 898.45 to 898.47 eV, 900.34 to 900.98 eV, and 916.44 to 916.24 eV, whereas the Ce3+ binding energy shifted from 885.46 to 884.27 eV and 904.32 to 904.24 eV (Fig. 4b). This shifting indicated the changes in the electronic environment around cerium, likely due to the co-ordination or charge transfer from the nitrogen loan pair of MG, which influences the reduction in the N 1s signal after adsorption. Moreover, the XPS peaks of Ag 3d appeared for the Ag 3d5/2 and Ag 3d3/2 states of Ag at 367.78 eV and 373.77 eV (Fig. 4c), respectively, confirming the doping of Ag into the composite.77 For silver (Ag), the peaks corresponding to the Ag 3d5/2 and Ag 3d3/2 states shift from 367.78 eV and 373.77 eV before adsorption to 367.97 eV and 373.98 eV after adsorption (Fig. 4d). The doublet peak at binding energies of 780.33 eV and 795 eV (Fig. 4e) represent Co 2p3/2 and Co 2p1/2 electronic states, respectively, of the Co 2p XPS spectra.78 For cobalt (Co), the Co 2p3/2 and Co 2p1/2 peaks shift from 780.33 eV and 795.00 eV before adsorption to 780.76 eV and 795.88 eV after adsorption (Fig. 4f), indicating the interaction between the MG molecules and the cobalt ions, which may involve electron donation from the dye to the metal centre. The Fe 2p XPS spectrum of the composite before adsorption reveals two primary peaks at 710.2 eV and 723.39 eV (Fig. 4g), corresponding to Fe 2p3/2 and Fe 2p1/2, respectively, which are characteristic of Fe3+ in ferrite materials.79,80 The satellite peak observed at approximately 718 eV further confirms the presence of Fe3+.81 After adsorption of MG, the iron (Fe) peaks for Fe 2p3/2 and Fe 2p1/2 shift from 710.2 eV and 723.39 eV to 710.29 eV and 723.59 eV (Fig. 4h). These shifts in the Fe 2p3/2 and 2p1/2 peaks suggests that there is no detectable reduction of Fe3+ to Fe2+ after dye adsorption, implying that Fe does not undergo redox changes during the adsorption process. This stability of the Fe oxidation states highlights the role of surface adsorption mechanisms rather than redox interactions between Fe and the dye. Overall, all shifts indicate a possible coordination interaction between the nitrogen atoms of MG and metal ions in the composite, suggesting that an inner sphere surface complexation occurs during the adsorption process.
O) groups in CA formed hydrogen bonds with CeO2 and PVP and coordinated with metal ions in the ferrite. PVP contributed additional stability by coordinating through its nitrogen atoms with Ce and Ag ions and forming hydrogen bonds with CA's hydroxyl groups. CeO2, with its surface oxygen and Ce3+/Ce4+ ions, participates in both hydrogen bonding with the hydroxyl (–OH) group of CA and coordination with carbonyl groups in CA and PVP. Cerium in the composite also allowed possible electron transfer interactions with the N lone pair of PVP. Hence, it is observed from the XPS spectra of cerium that both Ce3+ and Ce4+ states are present before adsorption. Ag-doped cobalt ferrite further stabilized the composite through coordination between metal ions with the oxygen of CA and oxygen as well as nitrogen of PVP. Additionally, the Ag ions provided electrostatic interactions with the nitrogen atoms in PVP, contributing to the overall stability of the composite. These combined interactions create a cohesive, stabilized network within the composite structure.
Adsorption is a surface phenomenon where adsorbates (ions or molecules) are held together by either van der Waals forces (physisorption) or chemical bonds (chemisorption). In this study, the adsorption of Malachite Green dye onto the surface of the ACFCeP composite can be attributed primarily to five main factors. (i) electrostatic interaction, (ii) H-bonding, (iii) surface complexation, (iv) pi–pi interaction, and (v) pore filling. (i) Electrostatic interactions: the electrostatic attraction between the positively charged Malachite Green (MG) molecules and the negatively charged functional groups (such as –OH groups in cellulose acetate and carbonyl groups in both PVP and cellulose acetate) plays a significant role in adsorption. These functional groups act as active binding sites for MG molecules.82 (ii) Hydrogen bonding: hydrogen bonding is another important interaction between the nitrogen-containing groups (dimethylamino groups) of MG and the hydrogen of the –OH group of cellulose acetate. This interaction enhances the adsorption process. (iii) Surface complexation and charge transfer: H. Zhu et al. reported that in surface complexation, the electron pair donor and electron acceptor interact to form various complexes.83 The XPS analysis reveals significant shifts in the binding energies of several metal ions before and after the adsorption of Malachite Green (MG), which supports the involvement of surface complexation and charge transfer interactions in the adsorption mechanism. This shift indicates a possible coordination interaction between the nitrogen atoms of MG and metal ions in the composite, suggesting that inner sphere surface complexation occurs during the adsorption process and the hypothesis of metal–dye complex formation (iv) π–π interactions: π–π stacking occurs between the aromatic rings of MG and the planar surfaces of cellulose acetate and PVP.84 These non-covalent interactions stabilize the dye molecules on the adsorbent surface.
Similar interactions were reported by A. A. Alqadami et al. where they observed electrostatic interactions, π–π stacking, and hydrogen bonding in the adsorption of Malachite Green onto Fe3O4@AMCA-MIL53(Al) composites.85 (v) Pore filling: the micropores in the ACFCeP composite structure may also contribute to the adsorption of MG by pore filling, where dye molecules are physically trapped within the porous network. From the BJH pore volume analysis, it is found that the composite possesses a pore volume of 0.0216 cm3 g−1, which also contributes to the dye adsorption mechanism. Scheme 2 presents the adsorption mechanism of the dye with the film.
Notably, no catalytic effect of MG on the ACFCeP film was observed in our experiments, as no reaction products indicative of catalytic degradation or chemical transformation of MG were detected in our analysis.
![]() | ||
| Fig. 5 FE-SEM image of cobalt ferrite (a); Ag-doped cobalt ferrite (b); cerium oxide (c); CA/PVP polymer blend (d); ACFCeP composite (e). | ||
Comparing the FE-SEM image of CA/PVP in Fig. 5d and ACFCeP in Fig. 5e, many pores and cavities can be observed. The mixing of nanoparticles (ACF and CeO2) with the polymeric matrix (CA/PVP), along with the solvent evaporation process, likely contributed to the formation of pores and cavities within the composite structure.87,88 During solvent evaporation, voids can be formed as the solvent leaves the system, especially in the presence of nanoparticles, which can disturb the packing of the polymer chains and increase the porosity.
The EDX analysis of CF and ACF are shown in Fig. S1a and b.† Comparing the atomic percentages of CF and ACF given in Tables S3 and S4,† respectively, the decreased atom percentage of Co indicates that Co was mostly replaced by Ag in ACF.
Table 1 shows the obtained BET surface area, pore size diameter and pore volume of the ACFCeP film. IUPAC (International Union of Pure and Applied Chemistry) classification was followed to determine the isotherms and pores of the film. According to IUPAC, pores with a diameter smaller than 2 nm are defined as micropores, mesopores with a diameter of 2–50 nm and macropores with a diameter greater than 50 nm.91 The BET analysis shows that the composite film exhibits a Type IV isotherm with an H4 type hysteresis loop.92 The specific surface area of the ACFCeP composite shows a moderate surface area of 5.824 m2 g−1, which is beneficial for the adsorption of organic dye molecules. The composite's pore volume is 0.0216 cm3 g−1, while the average pore diameter of 14.85 nm indicates the composite's mesoporous structure, which contributes to the diffusion of dye molecules into the composite film. Importantly, the molecular size of Malachite Green is 0.82 nm.93 Hence, it can fit into the pores of the ACFCeP composite during adsorption and can make the ACFCeP composite a suitable candidate for adsorption applications. Although the surface area is not particularly high, research by Chaukura et al. and N. El Badawi et al. shows that porous materials with similar surface areas can perform well in dye adsorption due to the accessibility of pores.94,95
| Specific surface area (m2 g−1) | 5.824 |
| Pore volume BJH (cm3 g−1) | 0.0216 |
| Average pore diameter (nm) | 14.85 (mesopores) |
![]() | ||
| Fig. 7 Magnetic hysteresis (M−H) curve of cobalt ferrite (CF) (a); Ag-doped cobalt ferrite (ACF) (b) and ACFCeP composite (c). | ||
Fig. 7 indicates the saturation magnetization (Ms) and remnant magnetization (Mr) of cobalt ferrite to be 82.9858 emu g−1 and 37.6368 emu g−1. A big hysteresis loop obtained from the M−H curve of cobalt ferrite (CF) suggests that it has ferrimagnetism.96 After silver doping, the hysteresis loop of Ag-doped cobalt ferrite (ACF) shows lower saturation magnetization and remanent magnetization, which are 29.8742 emu g−1 and 7.4171 emu g−1, respectively. The final ACFCeP composite exhibits a Ms of 3.7123 emu g−1 and Mr of 0.8467 emu g−1. Though ACFCeP shows lower magnetization values compared to pure cobalt ferrite, it also gives a visible hysteresis loop in the M−H curve, indicating the presence of magnetic properties in it.
To understand the relation between solution pH and MG dye adsorption process on ACFCeP, 50 mg of the composite was taken in a 50 ppm dye solution with pH ranging from 2 to 8, maintaining a contact time of 90 min. The result (Fig. 8a) shows that cationic MG dye adsorption is trivial in an acidic solution (pH 2). This happens as the H+ ion is present in high concentration, which replaces the MG dye molecule during adsorption. With increasing pH, the concentration of H+ ion decreases, and the removal percentage of the cationic MG dye increases. At pH 7, the removal% reaches the maximum at 93.3%. Fig. 8b shows that the ACFCeP composite film has a pHpzc of 6.7, which is below pH 7, indicating that the adsorbent surface is negatively charged and able to bind with the cationic MG dye.
Another important parameter is adsorbent dosage, which fixes the adsorbent's capacity for a certain initial dye concentration. For the batch experiment, ACFCeP adsorbents of weight 10–100 mg were taken separately in 30 mL of 50 ppm MG dye solutions, and the shaking speed was maintained at 200 rpm for 90 min.
The graph in Fig. 8c depicts that the adsorbent capacity of the ACFCeP film decreases with increasing adsorbent dosage. These may result from the aggregation or overlapping of adsorption sites and increased diffusion pathways.67 It is also visible that the removal percentage improved with the increasing quantity of adsorbents. The reason might be the accessibility to more active sites and the rise in surface area with the increasing adsorbent molecule.99 From the experiment, it is observed that the optimum adsorbent dose is 50 mg as it shows a maximum removal percentage of 94% with qe of 110 mg g−1, and further addition of the adsorbent does not influence the obtained values.
With increasing initial dye concentration, the percentage removal of the dye decreased but the adsorption capacity increased. This tendency indicates that a certain quantity of the adsorbent has almost a fixed amount of adsorption sites. So, the adsorbent cannot absorb dye molecules after the adsorption sites are occupied.100 Therefore, at lower initial dye concentrations, the composite adsorbent can adsorb the highest number of dye molecules. On the contrary, at higher initial dye concentrations, the active sites of the composite become saturated and the dye removal percentage decreases.
The relation between the adsorbate MG dye molecules and the ACFCeP surface is examined by the Langmuir, Freundlich, Dubinin–Radushkevich and Temkin isotherms, which are shown in Fig. 9b–e, respectively, in their linear forms. The non-linear forms of the corresponding isotherms are also demonstrated in Fig. 10a–d.
K and qmax values are measured from the slope and intercept of the linear plots of the Langmuir and D-R isotherms, respectively, using eqn (21) and (22). qmax is the theoretical maximum adsorption capacity, which is the highest adsorbate quantity that can be adsorbed per unit mass of the adsorbent (mg g−1).101 The equation shows a qmax value of 45.66 mg g−1 and 36.39 mg g−1 for Langmuir and D-R linear models, respectively.
| y = 0.0219x + 0.0252 | (21) |
| y = −0.00000005x + 3.5944 | (22) |
| y = 0.2606x + 1.318 | (23) |
| y = 6.633x + 24.514 | (24) |
The linear form of the Freundlich isotherm for the composite film is expressed by eqn (23), which gives the values of Kf and 1/n. As n is a function of the strength of adsorption, adsorption becomes more favorable with the increasing value of n.102 The value of n for good adsorption is between 2–10; for difficult adsorption, it is 1–2 and less than 1 for very poor adsorption.103 The value of n found in this study is 3.8 at room temperature, which indicates that adsorption is satisfactory in this case. The R2 value is found to be 0.972, which represents the moderate following of the Freundlich isotherm. The linear Temkin isotherm equation is shown in eqn (24). From eqn (11) and Table 2, the sign of b is positive, which indicates the process is endothermic.104 The data of all the non-linear isotherms are provided in Table S5.† The best-fitted isotherm model is indicated by the maximum value of the regression factor (R2). Among the linear and non-linear isotherms, the D–R isotherm was proven the most unfitted in both forms, with the lowest R2 values. Among all linear and non-linear models, both forms of the Langmuir isotherm and linear form of the Freundlich isotherm exhibited R2 values of 0.99 and 0.97, which is close to 1. Therefore, it can be said that the ACFCeP composite followed the linear Langmuir and Freundlich isotherms than the other isotherms. Furthermore, the adsorption capacity is also influenced by the pore volume, which can be observed from the calculation based on a pore volume of 0.0216 cm3 g−1 and the density of MG (1.2 g cm−3), suggesting an expected adsorption capacity of approximately 26 mg g−1. This calculation underscores the significance of pore volume in the adsorption process, as it directly impacts the capacity values.
| Isotherm model | Parameter | Value for ACFCeP composite |
|---|---|---|
| Langmuir | qmax (mg g−1) | 45.66 |
| K (L mg−1) | 0.869 | |
| R2 | 0.9956 | |
| Freundlich | Kf (mg g−1) | 20.79 |
| n | 3.8 | |
| R2 | 0.972 | |
| D–R | βDR | 4.60 × 10−8 |
| qmax (mg g−1) | 36.3924014 | |
| R2 | 0.80922 | |
| Temkin | A (unitless) | 6.63 |
| KT (L mg−1) | 40.3 | |
| b (kJ mol−1) | 373.69 | |
| R2 | 0.9678 |
The relation between the contact time and adsorption capacity is shown in Fig. 11a for the three different concentrations. From the graph, it is visible that adsorption capacity rises rapidly in the first 10 min for all studied concentrations. Then, adsorption capacity becomes constant after 50 min for 20, 60 ppm and 70 min for 100 ppm. The plot suggests that with the increase in time, open sites for adsorption on the ACFCeP surface are decreased and at the plateau, the adsorption efficiency does not change anymore with any increase in adsorption time.106
To study the ACFCeP adsorption kinetics, MG dye solutions of different concentrations (20, 60, 100 ppm) are taken. The linear pseudo first order, pseudo second order and Elovich plots are shown in Fig. 11b–d, and the non-linear plots are demonstrated in Fig. 12a–c.
The adsorbent's adsorption capacity at equilibrium and rate constant are determined from the slope and intercept of each linear plot, respectively, and displayed in Table 3. The data for the non-linear plots are presented in Table S6.† The linear first order, second order and Elovich equations for three specific concentrations are displayed in Table S7.†
| Kinetic model and parameter | 20 ppm | 60 ppm | 100 ppm |
|---|---|---|---|
| Experimental qe (mg g−1) | 11.9081 | 32.5260 | 44.0642 |
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| Pseudo first order (PFO) | |||
| qe (mg g−1) | 1.0796 | 6.2651 | 50.3702 |
| K1 (min−1) | 0.0252 | 0.0402 | 0.0658 |
| R2 | 0.8989 | 0.9794 | 0.9356 |
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| Pseudo second order (PSO) | |||
| qe (mg g−1) | 11.9047 | 33.1125 | 48.3091 |
| K2 (g mg−1 min−1) | 0.0728 | 0.0137 | 0.0019 |
| R2 | 0.9999 | 0.9991 | 0.9914 |
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| Elovich kinetics model | |||
| α (mg g−1 min−1) | 0.142450142 | 0.526316 | 2.083333 |
| β (g mg−1) | 44.6014365 | 551 722.9 |
2.87000000 |
| R2 | 0.815 | 0.979 | 0.979 |
Comparing the R2 values, it is noticeable that pseudo second order kinetics and Elovich model both showed satisfactory R2 values in the non-linear forms but only the pseudo second order kinetic reached an R2 value close to 1 in the linear form for three different concentrations. Hence, it is suggested that the linear pseudo second order kinetics is more suitable than any other kinetic models for the adsorption of MG dye on the ACCFCeP film.
Fig. 13 shows that the dye removal percentage drops from 93.3% in the 1st cycle to 85% in the 3rd cycle. The removal percentage reduced gradually due to the partial desorption of dye molecules when regenerated after each cycle. Besides, blocking the pores by the dye molecules also contributes to a successive decrease in performance.107,108 So, experimentally, it is evident that the ACFCeP composite film has the potential for long-term reusability in industrial applications for removing organic dye molecules. Table 4 compares the adsorption capacities of the MG dye on various polymers and nanoparticle composites with the newly developed magnetic composite.
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| Fig. 13 Demonstration of the reusability of the ACFCeP composite for removing MG up to three cycles. | ||
| Adsorbent | Qmax (mg g−1) | References |
|---|---|---|
| Chitin hydrogel | 33.57 | 109 |
| Graphene oxide (GO)-cellulose bead (GOCB) | 17.86 | 110 |
| Activated carbon-chitosan-SDS film | 4.80 | 8 |
| Zinc oxide-chitosan composite | 11.00 | 111 |
| ZnFe2O4-polyaniline-graphene oxide nanocomposite | 9.17 | 112 |
| Zeolite loaded PVA-CMC-sodium alginate membrane | 29.58 | 113 |
| Mn–Fe layered double hydroxides-polyethersulfone (PES) membrane | 13.49 | 114 |
| Magnetic activated carbon | 36.36 | 115 |
| Ag0.2Co0.8 Fe2O4/CeO2/cellulose acetate/polyvinylpyrrolidone (ACFCeP) composite film | 45.66 | This work |
| Magnetic nano copper ferrite, CuFe2O4 | 22 | 116 |
| Bentonite | 7.72 | 117 |
| Sugarcane dust | 4.88 | 118 |
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ra06315e |
| This journal is © The Royal Society of Chemistry 2024 |