3.1 Characterizations of samples
The mechanical strength is particularly important for macroscopic three-dimensional adsorbent materials because adsorbents are easily damaged by extrusion pressure in the real environment. The stress-strain tests result of CS-FM, SLS/CS-FM, CS@ZIF-8 and SLS/CS@ZIF-8 were presented in Fig. 1. It could be clearly seen that the mechanical strength of SLS/CS-FM and SLS/CS@ZIF-8 were significantly stronger than that of CS-FM and CS@ZIF-8. The improvement of mechanical strength showed that CS and SLS were well combined and compatible, SLS played a supporting role in the material. Meanwhile, it could be seen that after the in-situ immobilization of ZIF-8 on CS-FM and SLS/CS-FM, the mechanical strength of the obtained materials for CS@ZIF-8 and SLS/CS@ZIF-8 were slightly enhanced, indicating that the chemical bond between ZIF-8 and carrier foams helps to improve the mechanical strength of the material.
Digital photographs of CS-FM, SLS/CS-FM, CS@ZIF-8 and SLS/CS@ZIF-8 were presented in Fig. 2 (a, b, c, d). The color of CS-FM changed from white to brownish yellow after the introduction of lignin. CS-FM and SLS/CS-FM had a dash of white on their surface after loading ZIF-8, which was caused by the white ZIF-8 crystals. The SEM images of CS-FM, SLS/CS-FM, CS@ZIF-8 and SLS/CS@ZIF-8 at magnification 500 times were shown in Fig. 2 (e, f, g, h). CS-FM and SLS/CS-FM had similar structures, both had macroscopic three-dimensional cellular network pore structure. The reason for these pores were formed by the loss of moisture during the freeze drying (Wang et al. 2021). The three-dimensional aperture of SLS/CS-FM was significantly smaller than that of CS-FM. Hence, SLS/CS-FM could immobilization more ZIF-8 per unit volume than CS-FM due to it has more pore wall area to provide attachment sites for ZIF-8. The increased loading content of ZIF-8 in adsorbent materials would contribute to improve its adsorption capacity. In addition, when ZIF-8 was loaded on CS-FM and SLS/CS-FM, their pore macroscopic three-dimensional cellular network pore structure remains unchanged. The SEM images of CS-FM, SLS/CS-FM, CS@ZIF-8 and SLS/CS@ZIF-8 at magnification 100000 times were shown in Fig. 2 (i, j, k, l). The pore wall of CS-FM and SLS/CS-FM was uneven surface. After the in-situ immobilization ZIF-8 on CS-FM and SLS/CS-FM, their pores wall presented a large number of particles with smooth surface rhomboid dodecahedron morphology. These particles were the typical morphology for ZIF-8 crystals, indicating that ZIF-8 was successfully in-situ immobilization on CS-FM and SLS/CS-FM.
The crystalline structure of CS-FM, SLS/CS-FM, ZIF-8, CS@ZIF-8 and SLS/CS@ZIF-8 were investigated by XRD (Fig. 3). The XRD patterns of ZIF-8 show that its characteristic peaks were located at 7.43°, 10.42°, 12.86° and 18.20°. This was consistent with previous reports (Wang et al. 2020; Zhao et al. 2020), indicating that ZIF-8 had been successfully synthesized. The XRD patterns of CS-FM and CS/SLS-FM both preserved one wide diffraction peak at about 20°. Moreover, it could be seen that the typical ZIF-8 diffraction peaks in the XRD patterns of CS@ZIF-8 and SLS/CS@ZIF-8, which indicating that ZIF-8 was successfully in-situ immobilization on CS-FM and SLS/CS-FM, and the crystal structure of ZIF-8 did not change during the in-situ immobilization process.
The FT-IR spectra for CS-FM, SLS/CS-FM, ZIF-8, CS@ZIF-8 and SLS/CS@ZIF-8 were showed in Fig. 4. In the spectrum of CS-FM, the broad peaks at 3449 cm− 1 were attributed to the stretching vibration of O-H and N-H bonds, the peaks at 2860 cm‒1 and 2934 cm‒1 belong to the symmetric and asymmetric vibrations of C-H bonds, respectively, the absorption peak at 1658 cm− 1 belongs to amide I band stretching (Baran et al. 2020) After CS and SLS were prepared into foams composite (SLS/CS-FM), the peak of amide I band stretching peak in CS-FM moved from 1658 cm− 1 to 1649 cm− 1. It can be inferred that there was hydrogen bonding between CS and SLS. The vibrations peak of the asymmetric absorption vibration peak of -SO3− was appeared in CS/SLS-FM at absorption peak of 1032 cm‒1, the -SO3− exist electrostatic interaction with − NH3+ in CS (Gu et al. 2019). In the spectrum of ZIF-8, the aliphatic stretching vibration and the aromatic stretching vibration of C–H bond on imidazole rings were described by peaks appearing at 2932 cm‒1 and 3136 cm‒1, respectively (Hoseinzadeh et al. 2021), the stretching vibrations of C = N bond was described by the peak appearing at 1580cm‒1, and the stretching vibration of C–N bond in the methyl and imidazole rings was described by peaks at 995cm‒1 and 1147cm‒1, respectively (Cao et al. 2020). In addition, the spectrum of CS@ZIF-8 and SLS/CS@ZIF-8 showed the main peaks of CS-FM and SLS/CS-FM functional groups, respectively. Moreover, the spectrum of CS@ZIF-8 and SLS/CS@ZIF-8 both had the vibration peak of Zn-O bond at 756 cm‒1 and the vibration peak of Zn-N bond at 420 and 690 cm‒1 (Wang et al. 2019), which further indicated that ZIF-8 grown on CS-FM and SLS/CS-FM.
The N2 adsorption/desorption isotherm curves of CS-FM, SLS/CS-FM, CS@ZIF-8 and SLS/CS@ZIF-8 were shown in Fig. 5. According to the IUPAC classification, the N2 adsorption/desorption isotherms curves of CS-FM and SLS/CS-FM display the type Ⅲ, which indicated that the CS-FM and SLS/CS-FM were a typical of non-porous materials with weak affinities to nitrogen (Imran et al. 2019). When ZIF-8 was immobilized on CS-FM and SLS/CS-FM, their adsorption/desorption isotherm display the type Ⅳ and the specific surface area significant increased. The result confirmed the existence of microporous pores in the CS@ZIF-8 and SLS/CS@ZIF-8 (Imran et al. 2019). The parameters of surface area and porous structure of CS@ZIF-8 and SLS/CS@ZIF-8 were listed in Table 1, it could be seen that the BET specific surface area of SLS/CS@ZIF-8 was about 5 times that of CS@ZIF-8. The results suggested that SLS/CS-FM immobilized more ZIF-8 per unit volume than CS-FM, which was in line with SEM observation SLS/CS-FM could provide more attachment sites for ZIF-8 than CS-FM per unit volume.
Table 1
Textural parameters of CS@ZIF-8 and SLS/CS@ZIF-8
Materials | BET surface area(m2/g) | Total pore volume(cm3/g) | Average pore size(nm) |
CS@ZIF-8 | 19.5123 | 0.015434 | 11.0176 |
SLS/CS@ZIF-8 | 108.3678 | 0.081055 | 12.2503 |
3.2 Effect of pH on adsorption capacity
The adsorption of CIP by CS-FM, SLS/CS-FM, CS@ZIF-8 and SLS/CS@ZIF-8 should be attributed to their chemical interaction. In this respect, considering the solution pH has a significant influence on dissociation of functional groups of adsorbents and the ionization forms of CIP, the pHzpc (point of zero charge) of these four materials was tested by the potentiometric tiration and the effect of pH for CIP adsorption performance was carried out. The pHpzc value of these four materials as shown in Fig. 6(a), meaning that these four materials surfaces had negatively charged when pH more than their point of zero charge, however, these four materials surfaces had positively charged when pH less than their point of zero charge. Combined with CIP molecules forms of existence (Fig. 6 (c)) and the hydrophobic interaction (Li et al. 2017; Wang et al. 2017), the electrostatic interaction and hydrophobic interaction between these four materials surfaces and CIP resulted in a larger adsorption capacity when 6༜pH༜9, which was consistent with the results of the adsorption experiment in Fig. 6 (b). In addition, the adsorption capacity was significantly improved when ZIF-8 immobilization on CS-FM and SLS/CS-FM, and the adsorption performance of SLS/CS@ZIF-8 was better than CS@ZIF-8.
3.3 Adsorption kinetics
The effect of contact time for SLS/CS@ZIF-8 adsorption capacity was investigated, and the experimental data was fitted by the quasi-first-order and quasi-second-order kinetic models. The adsorption data and fitting curve were shown in Fig. 7, and the parameters were listed in Table 2. The quasi-first-order kinetic and the quasi-second-order kinetic models are described by Eqs. (2) and (3), respectively.
$${q_t}{\text{=}}{q_e}(1 - {e^{{\text{-}}{k_1}t}}{\text{)}}$$
2
$$\frac{t}{{{q_t}}}{\text{=}}\frac{1}{{{k_2}q_{e}^{2}}}{\text{+}}\frac{t}{{{q_e}}}$$
3
Where, qt (mg/g) and qe (mg/g) are the CIP adsorption amount at different time intervals and the CIP adsorption amount at equilibrium, respectively; k1 (min− 1) and k2 (g/mg/min) are the pseudo-first-order and pseudo-second-order rate constant, respectively.
As shown in Fig. 7, the CIP adsorption rate was fast at the initial 200 min, and then reaches equilibrium gradually with the increase of time. It could be known from Table 2, the quasi-second-order kinetic model had a higher R2 and the maximum adsorption capacity (qcal) had a good correlation with the experimental value (qexp), implying that the rate-limiting steps of adsorption were mainly affected by chemisorption mechanism (Ghani et al. 2020).
Table 2
Kinetic parameters for CIP adsorption onto SLS/CS@ZIF-8
C0(mg/L) | qe(exp) (mg/g) | Pseudo-first order | Pseudo-second order |
qe(cal)(mg/g) | k1(/min) | R2 | qe(cal) (mg/g) | k2(g·mg− 1/min) | R2 |
250 | 413 | 389 | 0.0012 | 0.973 | 426 | 4.080 | 0.993 |
3.4 Adsorption isotherms
In order to evaluate the adsorption performance of CIP on SLS/CS@ZIF-8, the CIP adsorption equilibrium data at different temperatures (303K, 318K, 333K and 348K) were fitted by Langmuir and Freundlich models in Fig. 8 (a, b), and the related parameters are listed in Table 3. The corresponding two adsorption isotherms models were expressed by Eqs. (4) and (5), respectively (Wu et al.2020).
$${q_e}{\text{=}}\frac{{{q_m}{K_L}{C_e}}}{{1+{C_e}{K_L}}}$$
4
$${q_{\text{e}}}{\text{=}}{K_F}{C_{\text{e}}}^{{1/{\text{n}}}}$$
5
Where, Ce is the equilibrium concentration of ciprofloxacin solution (mg/L), qm (mg/g) is the maximum adsorption capacity, KL (L/mg) and KF (L/g) are the adsorption constants of Langmuir isotherm and Freundlich isotherm, respectively, n is the constant of intensity.
As could be seen from Fig. 8 (a, b), the adsorption capacity of SLS/CS@ZIF-8 for CIP increased with the increasing CIP concentration. The qe also increased with the increasing of temperature, the maximum adsorption capacities (qm) of SLS/CS@ZIF-8 for CIP was 413 mg/g, 430 mg/g, 439 mg/g and 449 mg/g at the temperatures of 303K, 318K, 333K and 348K, respectively. The relative parameters were listed in Table 3, it could be seen that Langmuir isothermal model was more suitable for describing CIP adsorption behavior on SLS/CS@ZIF-8 than Freundlich isothermal model because it had the highest R2 value. Table 4 showed the comparison of CIP adsorption capacity between SLS/CS@ZIF-8 and other adsorbents. It could be seen that the adsorption capacity of SLS/CS@ZIF-8 for CIP was higher than that of most reported adsorbents.
Table 3
Isotherm parameters for CIP adsorption onto SLS/CS@ZIF-8
Isotherm | Parameters | 303K | 318K | 333K | 348K |
Langmuir | qm (mg/g) | 470 | 482 | 490 | 509 |
| KL(L/mg) | 0.191 | 0.267 | 0.284 | 0.358 |
| R2 | 0.991 | 0.992 | 0.989 | 0.990 |
Freundlich | n | 2.65 | 2.65 | 2.61 | 2.61 |
| KF(mg/g(L/mg)1/n) | 114 | 129 | 137 | 155 |
| R2 | 0.917 | 0.927 | 0.929 | 0.911 |
Table 4
The adsorption capacity for CIP onto various adsorbents
| Conditions | | |
Adsorbents | Initial concentrations (mg/L) | Dose (g/L) | pH | T/(K) | qm(mg/g) | References |
SLS/CS@ZIF-8 | 50–250 | 0.5 | 7 | 303 | 413 | Present work |
Titanate nanotubes | 3.3–26.7 | 0.1 | 5 | 298 | 153 | Theamwong et al. (2021) |
Ga2S3 and sulfur co- | 100–190 | 0.25 | 3.23 | 298 | 330 | Zheng et al. (2021) |
modified biochar composites MIL-53(Fe-Cu) | — | 1 | 6 | 293 | 190 | Chatterjee et al. (2021) |
Ordered mesoporous carbon | 20–100 | 0.3 | 7 | room | 233 | El-Bendary et al. (2015) |
Bamboo-based carbon | 20–100 | 0.3 | 7 | room | 362 | El-Bendary et al. (2015) |
Chitin-biocalcium | 50-1800 | 0.5 | 4–10 | 298 | 2432 | Antonelli et al. (2020) |
KGM/ZIF-8 aerogels | 100–1500 | 1 | 7 | 303 | 811.03 | Yuan et al. (2018) |
3.5 Adsorption thermodynamics
Thermodynamic parameters including enthalpy (ΔH0), free energy (ΔG0) and entropy (ΔS0) can be used to study the extent and driving force of adsorption process. The thermodynamic parameters of CIP adsorption on SLS/CS@ZIF-8 were obtained from the following Eqs. (7), (8) and (9).
$${K_0}{\text{=}}\frac{{{{\text{q}}_{\text{e}}}}}{{{C_{\text{e}}}}}$$
7
$$\ln {K_0}=\frac{{\Delta {S^0}}}{R} - \frac{{\Delta {H^0}}}{{RT}}$$
8
$$\Delta {G^0}=\Delta {H^0} - T\Delta {S^0}$$
9
Where K0 is the thermodynamic equilibrium constant (L/mg), T is the absolute temperature (K), and R is the universal gas constant (8.314 KJ/mol).
Figure 9 shown the linear relationship between ln(K0) and 1/T, the ΔH0 and ΔS0 could be obtained from the slope and intercept of the line. According to Table 5, the positive value of ΔH0 indicated that the CIP adsorption on SLS/CS@ZIF-8 was endothermic nature, and the ΔS0 value was positive indicates that the randomness of the solid-liquid interface increased when CIP was adsorbed on SLS/CS@ZIF-8, the ΔG0 values were all negative indicates that the adsorption process was spontaneous (Antonelli et al. 2020; Chatterjee et al. 2021).
Table 5
The determined values of thermodynamic parameters
ΔH 0(KJ/mol) | ΔS 0(J/(mol•K)) | ΔG 0/(KJ/mol) |
303K | 318K | 333K | 348K |
1.22 | 60.53 | -6.14 | -7.04 | -7.96 | -8.86 |
3.6 Mechanisms of CIP adsorption on SLS/CS@ZIF-8
The FTIR and XPS were used to further explore the potential adsorption mechanism of CIP on SLS/CS@ZIF-8. Figure 10 showed the FT-IR spectra of SLS/CS@ZIF-8 before and after adsorption of CIP, respectively. In the spectrum of SLS/CS@ZIF-8, the absorption peak at 3449cm‒1 belongs to O‒H and N‒H stretching, the absorption peak at 1600 cm− 1 belongs to the C = C stretching in aromatic rings. After adsorption of CIP, the bond of O‒H and N‒H from 3449cm‒1 shifted to 3457cm‒1, suggesting the existence of a hydrogen bond and electrostatic interaction between CIP and SLS/CS@ZIF-8 (Zhao et al. 2020). The absorption peak at 1600 cm− 1 shifts to 1617 cm− 1 after the adsorption of CIP because of the π − π interaction. Figure 11(a) showed high-resolution spectra of C1s peak intensity of SLS/CS@ZIF-8 before and after CIP adsorption. The C–C/C = C and C–N/C–O were described by absorption peak appearing at 284.8 and 286.1 eV, respectively (Wang et al. 2019). After adsorption CIP, the two C1s peaks shift to 285.0 and 286.3 eV, respectively, indicating that the existence of π-π interaction between SLS/CS@ZIF-8 and CIP (Sca et al.). Figure 11 (b) and (c) showed high-resolution spectra of N1s and O1s peak intensity of SLS/CS@ZIF-8 before and after CIP adsorption. The peaks at 399.1, 400.5, 531.8 and 533.1 eV were corresponded to C‒N, C = N, Zn‒OH and O‒C = O, respectively. After adsorption of CIP, except for the binding energy of Zn‒OH peak, the binding energy of the other three peaks moved to higher values, which shows that there was hydrogen bonding interaction between SLS/CS@ZIF-8 and CIP and the hydrogen bonding interaction formed by the O and N functional groups was dominant. Figure 11(d) showed that the two binding energy peaks of Zn2p. The two peaks moved to lower values after adsorption of CIP, indicating that Zn2+ had electrostatic interaction with CIP. In summary, electrostatic interaction, π-π interaction and hydrogen bonding interaction dominated the adsorption of CIP on SLS/CS@ZIF-8, and the multiple adsorption mechanism of the SLS/CS@ZIF-8 towards CIP was shown in Fig. 12.
3.7 Reusability
The reusability efficacy of adsorbent is important for industrial application. As shown in Fig. 13, the adsorption capacity of SLS/CS@ZIF-8 for CIP decreased with the increase of adsorption cycles. However, SLS/CS@ZIF-8 was still have an excellent adsorption capacity after six adsorption-desorption cycles, which indicated that SLS/CS@ZIF-8 exhibits acceptable reusability as CIP adsorbent and has good industrial application value.