3.1. Characterization of C3N4/CDs/4A
The morphology of the composited was characterized via SEM in Fig. 1. The SEM images revealed the typical cubic morphology of 4A molecular sieve (Fig. 1A-B) with a smooth and flat surface. The average size of the 4A molecular sieve particles was approximately 2 µm. The SEM characterization of the C3N4/CDs/4A showed that the C3N4 exhibited thin edges and folded layers, tightly wrapped around the surface of the 4A molecular sieve (Li W et al. 2022). Carbon dots were also observed on the surface (Fig. 1C-D). The presence of carbon dots on the surface of 4A molecular sieve significantly increased its specific surface area, enhancing its adsorption capacity. Moreover, even after multiple cycles of thermal regeneration, the adsorption performance remained excellent, indicating the strong anchoring of carbon dots on the crystal surface of 4A molecular sieve.
Further structural characterization was conducted using FTIR spectroscopy in Fig. 2. The FTIR spectra of 4A molecular sieve and C3N4/CDs/4A exhibited characteristic absorption peaks (Li W et al. 2022). The absorption peak at 466 cm− 1 corresponded to the stretching vibration of Si-O bonds (YU J et al. 2021), while the peak at around 551 cm− 1 indicated the bending vibration of Al-O bonds. The absorption peak at 665 cm− 1 represented the bending vibration of Si-O bonds, indicating the formation of AlO4 and SiO4 tetrahedra. The absorption peak at 1002 cm− 1 corresponded to the asymmetric stretching vibration of Si-O-Si bonds, indicating the presence of asymmetric Si-O-Si linkages and the formation of the framework structure of the molecular sieve. The absorption peak at 1658 cm− 1 indicated the bending vibration of H-O-H bonds, and a broad peak at 3432 cm− 1 suggested the presence of bound water in the product (Goyal et al. 2020). The FTIR spectra of C3N4/CDs/4A exhibited a characteristic absorption peak at 812 cm− 1, corresponding to the tri-s-triazine structure of graphitic carbon nitride, and a new peak at 2341 cm− 1, attributed to the vibrational mode of the O = C = O bond in carbon dots.
The XRD patterns of 4A molecular sieve and the C3N4/CDs/4A were also analyzed, which were shown in Fig. 3. The XRD pattern of 4A molecular sieve exhibited strong diffraction peaks at 2θ angles of 7.22°, 10.19°, 12.48°, 16.13°, 21.70°, 24.02°, 27.14°, 29.97°, and 34.21°, matching the standard card of 4A molecular sieve without any additional peaks, indicating good crystallinity of the unmodified 4A molecular sieve. The XRD pattern of C3N4/CDs/4A showed a leftward shift of the peaks, indicating an increase in the lattice parameters and interplanar spacing due to the doping of foreign atoms. Compared to 4A molecular sieve, the new peak observed at 2θ = 27.2° in C3N4/CDs/4A corresponded to the (002) crystal plane of carbon nitride (Ma T et al. 2019; Song et al. 2014). The decrease in peak intensity of 4A molecular sieve was attributed to the loading of carbon nitride and carbon dots on the surface, disrupting the crystalline state of the molecular sieve (Fang L J et al. 2019).
The adsorption-desorption isotherms and particle size distribution of 4A molecular sieve and C3N4/CDs/4A were obtained in Fig. 4. CO2 was used to characterize the microporous structure of 4A molecular sieve, while nitrogen gas was used for the C3N4/CDs/4A (Chen Z et al. 2018). The adsorption isotherm of 4A molecular sieve exhibited a type I isotherm, indicating predominant microporous adsorption. The adsorption isotherm of the C3N4/CDs/4A belonged to type IV with hysteresis loops, indicating the presence of mesoporous adsorption characteristics. Specific surface area, pore volume, and pore size of the materials were analyzed and presented in Table 1. The C3N4/CDs/4A showed increased specific surface area and total pore volume, indicating a structure more favorable for adsorption.
Table 1
Specific surface area, pore volume, and pore size of 4A molecular sieve and C3N4/CDs/4A.
Sample | Specific surface area (m2/g) | Pore volume (ml/g) | Pore size (nm) |
4A | 77.45 | 0.04 | 5.42 |
C3N4/CDs/4A | 164.54 | 0.05 | 2.79 |
3.2. Adsorption performance of C3N4/CDs/4A for MB
3.2.1. dosage effect
The relationship between varying adsorbent dosages and adsorption efficacy, with a constant MB concentration of 100 mg/L and a solution volume of 100 mL, was demonstrated by Fig. 5. Up to an adsorbent mass of 0.40 g, the adsorption efficiency escalated with increasing mass. However, at 0.40 g, the adsorption efficiency peaked at 99.6%, and further increasing the mass to 0.50 g did not yield significant improvements. Therefore, the mass of 4A molecular sieve and C3N4/CDs/4A was 0.4 g in the subsequent adsorption kinetics experiments.
3.2.2. kinetics study
The effect of contact time on adsorption efficiency, with a constant MB concentration of 100 mg/L (pH = 5.9) and a solution volume of 100 mL, was illustrated by the Fig. 6. The mass of 4A molecular sieve and C3N4/CDs/4A was 0.40 g. During the initial 10 minutes period, the adsorption rate for MB was remarkably high due to the abundant availability of adsorption sites on the surface of the adsorbent and its effective dispersion within the solution. Subsequently, as the adsorption process progressed without reaching equilibrium, the gradual occupation of adsorption sites led to a deceleration in the adsorption rate. Notably, the equilibrium adsorption capacity of the C3N4/CDs/4A was 4.34 times than 4A molecular sieve. This remarkable enhancement showed the substantial improvement in adsorption performance following material modification. The adsorption conditions and specific adsorption data at other masses were given by the supporting information.
Kinetic fitting of the adsorption process was carried out. The pseudo-first-order Eq. (3) and the pseudo-second-order Eq. (4) were used to fit the data (Ho Y S. 2004).
$${ln}\left({q}_{e}-{q}_{t}\right)=ln{q}_{e}-{k}_{1}t$$
3
$$t/{q}_{t}=1/\left({\text{k}}_{2}^{2}{*q}_{e}^{2}\right)+\text{t}/{q}_{e}$$
4
where qe (mg/g) is the equilibrium adsorption capacity, qt (mg/g) is the adsorption capacity at time t, k1 and k2 are the rate constants for the first-order and second-order kinetics, which can be calculated from the slope and intercept of the linear plot. The fitting of experimental data to the models was shown in the Fig. 7 and Table 2.
Table 2
Kinetic parameters of 4A and C3N4/CDs/4A.
Sample | qe, exp (mg/g) | Pseudo-first-order model | Pseudo-second-order model |
k1(min− 1) | qe,cal (mg/g) | R2 | k2[g/(mg*min)] | qe,cal (mg/g) | R2 |
4A | 5.75 | 0.206 | 3.59 | 0.946 | 0.172 | 5.88 | 0.999 |
C3N4/CDs/4A | 24.95 | 0.232 | 12.50 | 0.924 | 0.065 | 25.25 | 1 |
From the correlation coefficients, it could be observed that the R2 values of the Pseudo-second-order equation were higher than that of the Pseudo-first-order equation. The results suggested that the adsorption process better fit the Pseudo-second-order kinetic equation, indicating a chemisorption process where MB molecules shared exchangeable electrons with the functional groups on the surface and within the pores of the C3N4/CDs/4A. When comparing the adsorption rate constants with 4A molecular sieves, the C3N4/CDs/4A. exhibited significantly lower adsorption rate constants. This was attributed to the increased carbon dot carbon content on the surface of 4A molecular sieves, hindering the transfer of MB to 4A, resulting in slower adsorption kinetics (Khan T A et al. 2012 ). However, C3N4/CDs/4A exhibited a much higher adsorption capacity compared to 4A molecular sieves.
3.2.3. pH effect
Figure 8a highlighted the distinctive adsorption of C3N4/CDs/4A attributes under varying pH conditions. The optimal adsorption effectiveness of C3N4/CDs/4A was observed when the solution pH remained unchanged, achieving a 74.79% adsorption efficiency for a 50 mg/L MB solution. However, significantly lower adsorption was seen in more acidic conditions, with a mere 33.94% adsorption efficiency. This decline was due to the instability of 4A molecular sieve in acidic environments, coupled with electrostatic repulsion between the cationic MB dye and protonated molecular sieve under acidic conditions. C3N4/CDs/4A exhibited robust adsorption performance at pH = 5 7, 9, and 11, with slight reductions.
3.2.4. isotherm study
The relationship between equilibrium concentration and adsorption capacity at 0.40 g of C3N4/CDs/4A and 4A molecular sieve at different MB concentrations (50 ~ 250 mg/L and a solution volume of 100 mL under 25℃ was shown in Fig. 9. With the increase of the initial concentration, the adsorption capacity gradually increased, and then tended to a constant value. The adsorption capacity of C3N4/CDs/4A was much higher than that of 4A molecular sieve. Then, the adsorption isotherm was fitted to the adsorption process. Langmuir (Kraus et al.2009), Freundlich (Wang J L et al. 2020), and Tempkin (Ma J et al.2012) models are commonly used to describe the characteristic parameters of adsorption at interfaces. The Langmuir adsorption equation assumes a uniform surface, single-layer adsorption, and no interaction between adsorbed molecules. The Freundlich and Tempkin equations are empirical equations applicable to heterogeneous surface adsorption. The former relates adsorption enthalpy to coverage in a logarithmic relationship, while the latter shows a linear relationship. The Freundlich equation is suitable for low coverage, while the Tempkin equation is suitable for moderate coverage. By comparing the linearity coefficient or the proximity of experimental points to the model, the adsorption isotherm that best fits the actual data can be determined.
Langmuir adsorption isotherms can be expressed as:
$${C}_{e}/{q}_{e}=1/{q}_{m}b+{C}_{e}/{q}_{m}$$
5
In the Langmuir equation, qe (mg/g) is the equilibrium adsorption capacity, Ce (mg/L) is the equilibrium concentration of MB, qm (mg/g) is the maximum adsorption capacity, and b (L/mg) is the Langmuir constant related to adsorption energy. According to Eq. (5), qm and b can be calculated from the slopes of 1/qm and the intercepts of 1/qmb.
The Freundlich isotherm, based on adsorption on energetically heterogeneous surfaces with no restrictions on monolayer formation, can be expressed as:
$$ln{q}_{e}=ln{K}_{f}+(1/\text{n})ln{C}_{e}$$
6
where Kf is the Freundlich constant, and 1/n is the heterogeneity factor related to the adsorption capacity and intensity. According to Eq. (6), Kf and n can be calculated from the slope of 1/n and the intercept of lnKf.
Tempkin isotherms equation:
$${q}_{e}=RT/{A}_{T}\text{*}(ln{K}_{T}+ln{C}_{e})$$
7
where R is the ideal gas constant (8.314 J/(mol·K)); AT is the adsorption constant of the Tempkin model (J/mol); T is the absolute temperature (K); KT is the equilibrium binding constant (L/g).
The adsorption isotherms for MB on the C3N4/CDs/4A and 4A molecular sieve, as described by Langmuir, Freundlich, and Tempkin equations, were shown in the Fig. 10 and the calculated parameters and R2 values were presented in Table 3. The R2 values served as indicators of the degree of fit between the experimental data and the model. As shown in Table 3, the Langmuir model exhibited the highest regression coefficient (R2 = 0.999), indicating its superior suitability in describing the adsorption behavior of the C3N4/CDs/4A. Consequently, it could be inferred that adsorption took place at uniformly binding sites on the surface of the adsorbent until a monolayer was formed. The adsorption process was classified as chemisorption, which was commonly regarded as a spontaneous phenomenon. Based on the Langmuir model, the maximum adsorption capacity of the C3N4/CDs/4A for MB was determined to be 44.34 mg/L. The incorporation of C3N4/CDs onto the surface of 4A molecular sieves increased the specific surface area of the C3N4/CDs/4A, enhancing its adsorption performance. Additionally, the electrostatic interaction between oxygen-containing functional groups on the carbon dots and positively charged MB molecules also contributed to the adsorption process.
Table 3
Langmuir, Freundlich and Tempkin isotherm parameters of 4A molecular sieve and C3N4/CDs/4A.
| 4A | C3N4/CDs/4A |
Langmuir | b (L/mg) | 0.056 | 1.776 |
qmax (mg/g) | 19.810 | 44.343 |
R2 | 0.972 | 0.999 |
Freundlich | Kf (L/mg) | 3.669 | 27.539 |
n | 2.828 | 8.635 |
R2 | 0.781 | 0.990 |
Tempkin | AT (J/mol) | 551.200 | 691.891 |
KT (L/g) | 0.522 | 3133.795 |
R2 | 0.829 | 0.973 |
3.2.4. Thermodynamics study
Figure 8b presented the temperature-dependent adsorption behavior of the composites towards MB solutions of a 50 mg/L concentration. As the temperature rose, the diffusion rate of MB molecules within the external boundary layer and internal pores of C3N4/CDs/4A accelerated, promoting the achievement of adsorption equilibrium. Equilibrium was achieved within 60 minutes at varying temperatures. Notably, 87% of the adsorption efficiency persisted even at 47°C, showcasing the applicability of C3N4/CDs/4A across a wide temperature range. A decline in equilibrium adsorption capacity with rising temperature implied an exothermic adsorption process. Given that the treatment of dye wastewater typically occurs at room temperature, conducting adsorption experiments under these conditions was appropriate. The adsorption mechanism of C3N4/CDs/4A for MB can be determined using thermodynamic values. The standard free energy (ΔG), enthalpy (ΔH), and entropy (ΔS) are calculated using the following formulas (Khatibi et al. 2021):
$$lnK=\varDelta S/R-\varDelta H/RT$$
9
where K is the adsorption equilibrium constant, which can be calculated from the following equation:
The thermodynamic parameters for MB adsorption on the C3N4/CDs/4A at different temperatures were shown in Fig. 11 and Table 4. Among these parameters, ΔG was negative at all temperatures, indicating a spontaneous process. ΔG increased with increasing temperature, suggesting that lower temperatures were favorable for this process. ΔH was negative and relatively large, indicating that the adsorption of MB was exothermic and tended to be a chemisorption process. This could be attributed to the electrostatic interaction between the C3N4/CDs/4A and MB. The change in entropy, ΔS, was negative, indicating a decrease in system disorder after adsorption. Combining the adsorption isotherm and adsorption rate, it was determined that the adsorption of MB on the C3N4/CDs/4A was a spontaneous, exothermic, and entropy-decreasing chemical adsorption process.
Table 4
Thermodynamic parameters for adsorption of MB.
ΔH(J/mol) | ΔS(J/mol/K) | ΔG(J/mol) |
-14419.802 | -40.795 | 298 K | 303 K | 313 K | 320 K |
-2179.998 | -2127.270 | -1763.273 | -1268.607 |
3.2.3. Recycling properties of C3N4/CDs/4A
The conventional method for material regeneration involves the addition of chemical regenerants, which can cause certain damage to the adsorbent material (Sivalingam et al. 2019). In this study, however, regeneration was achieved through pyrolysis, which resulted in excellent regeneration performance without causing any damage to the material. The recyclability of C3N4/CDs/4A held paramount significance as a key metric for their practical utility. In this investigation, thermal regeneration was employed as the methodology for material regeneration. Figure 12 encapsulated the outcomes of subjecting the composite to five consecutive cycles of adsorbing MB solutions. The observed adsorption efficiency for these successive cycles were 99.6%, 98.7%, 98.4%, 98.1%, and 98.6%, respectively. The adsorption efficiency was almost not reduced. Some of the sorbents in the other literature were given by the supporting information. These findings affirmed the exceptional cyclic stability and thermal endurance of C3N4/CDs/4A. With its consistent and high adsorption efficiency across multiple cycles, the material demonstrated its robust potential for industrial application. This showed the composite's suitability for sustained use and its promising viability within real-world scenarios.