Characterization of magnetic carbon xerogel nanocomposites
In this study water was used as solvent to examine the molar ratios of resorcinol/water (R/W) between 0.4 and 0.5 on the adsorption of arsenic. The molar ratios used for synthesis of XMC5-600 and XMC10-600 were R/C = 100 and M/R = 0.07 at different R/W ratios as shown in Table 3. It can be observed that the percentage of Fe contents of materials increased with decreasing R/W ratio. The initial solution with decreasing reactant concentration has the significant effect of the mass of dissolved solids in a fixed volume of solvent that used deionized water in this synthesis and the resulting properties of final material (Prostredný et al. 2018).
Table 3
Synthesized magnetic carbon xerogel nanocomposites with varying R/W ratios.
Sample
|
R/C ratio
|
R/W ratio
|
M/R ratio
|
Fe content (%)
|
XMC5-600
|
100
|
0.05
|
0.07
|
3.19
|
XMC10-600
|
100
|
0.04
|
0.07
|
3.56
|
The determination of N2 physisorption was analyzed from the data of two materials before and after carbonization, which were XMC5 and XMC5-600, respectively. Figure 1(a) shows the nitrogen adsorption isotherms and Fig. 1(b) presents the pore size distribution of XMC5 and XMC5-600. The isotherms of both materials exhibit type IV with an H2 type hysteresis loop shape that indicate the mesoporous types corresponding to the results obtained from the mesoporous distribution (Moreno et al. 2013; Quach et al. 2017). The specific surface area from BET analysis of before and after carbonization of XMC5-600 increased from 329.1 to 579.2 m2/g (Table 4). The average pore size of XMC5 (6.171 nm) was larger than that of XMC5-600 (3.715 nm), however both were in the range of mesoporosity and identified an average pore size between 2 and 50 nm. The textural properties and particle sizes of carbon xerogels have significant changes in the carbonization process (Moreno et al. 2013). The BET surface area and total pore volume of XMC5-600 increased, but the average pore diameter decreased as shown in Fig. 1. Due to the thermal treatment, not only temperature increases and releases volatile compounds from XMC5, but also it is possible to remove non-crosslinked polymer chains and labial surface groups of oxygen and hydrogen in the carbonization process at optimum temperature under the inert gas like N2 (Calvo et al. 2011). Finally, it can be obtained thermally stable carbonaceous materials with development of microporosity in the xerogels and resulting in the nanostructured carbon xerogel with effect on adsorption capacity.
Table 4
Specific surface area, average pore diameter and total pore volume of magnetic xerogel XMC5 and magnetic carbon xerogel XMC5-600.
Samples
|
BET surface
|
Average pore diameter (nm)
|
Total pore volume
|
area (m2/g)
|
(cm3/g)
|
XMC5
|
329.1
|
6.171
|
0.508
|
XMC5-600
|
579.2
|
3.715
|
0.538
|
Figure 2 shows SEM images that were achieved by using secondary electron (SE) and backscattering electron (BSE) detection with a magnification ranging from 10,000x to 400,000x, spatial resolution of 50 to 300 nm. The actual acceleration voltage of 5 kV was applied to all images. The microstructure of magnetic carbon xerogels at R/C = 100 and M/R = 0.07 were compared with the different of R/W ratios between XMC10-600 (R/W = 0.04) and XMC5-600 (R/W = 0.05) as shown in Fig. 2(a, b, c) and 3(e, d, f), respectively. All SEM images represent carbon xerogels in the form of nanosized particles composed of spherical particles less than 100 nm as shown in Fig. 2(a) and 2(d). It can be observed that RF carbon xerogels both of XMC10-600 and XMC5-600 had uniformly interconnected large numbers of microclusters like a three-dimensional polymer and result in porous materials for adsorption application (Yoon et al. 2019). The decreasing of R/W ratios can be controlled the microclusters and porous properties on the resulting RF carbon xerogel because decreasing reactant concentration and affecting to have less compaction or less voids of RF gel structure and increase surface areas (Al-Muhtaseb and Ritter 2003). The structure of void was a resulting of solvent removal and evaporation during the process of carbonization, although the solvent exchange by using acetone was applied on the preparation to protect the collapse of the porous structure of the gel (Thubsuang et al. 2014; Canal-Rodríguez et al. 2017). Figures 2(b) and 2(e) illustrate that XMC5-600 had more compaction of nanoporous xerogels than XMC10-600. Microtexture determination by ESBD shows that MNPs were deposited and distributed homogeneously onto the surface of carbon xerogels. The brightened regions in Figs. 2(c) and 2(f) represent the area where Fe networks were formed, also the gray and dark regions illustrate nanopores. Moreover, the results of the determination of Fe contents by AAS confirmed that the percentage of Fe contents of XMC5-600 and XMC10-600 at different R/W ratio increased with decrease in R/W ratio which were 3.19% and 3.56%, respectively. The corresponding EDX image in Fig. 3 shows that magnetic carbon xerogel XMC10-600 after adsorption of As(V), contained C, O, Al, Si, Fe and As, and most of the bulk of XMCs composed of carbon approximately 84.5% wt. (Embaby et al. 2021).
The XRD patterns of XMC5 before and after thermal treatment with carbonized temperature at 600°C, XMC5-600M and XMC10-600M with surface modification are presented in Fig. 4. The XRD examination indicated the presence of magnetite nanoparticles composed in carbon xerogels that displayed crystallization peaks of the samples at 30.2°, 35.5°, 43.1°, 57.0°, and 62.6° corresponding to (220), (311), (400), (511), and (440) planes of the characteristic peaks of magnetite (JCPDS No. 88–0866) (Sundrarajan and Ramalakshmi 2012). It can be observed that the peaks at 2θ between 20–30° that confirm the structure of materials are amorphous (Huang et al. 2018). The XRD diffraction profile at 20° and 43° corresponds to the (002) and (100) planes of graphene sheets and graphite, respectively, that are reflected in a carbon structure (Kiciński et al. 2011; Arsić et al. 2016).
Figure 5(a) shows FTIR spectra of magnetic carbon xerogels with R/W molar ratios of 0.4 and 0.5 before and after carbonization at 600°C as named XMC10, XMC10-600, XMC5, and XMC5-600. The FTIR bands at 3400 cm− 1 are attributed to –OH groups bonding to benzene rings caused by the stretching and bending vibration (Attia et al. 2017). The bands at 1620 cm− 1 are attributed to H-O-H bonds ending vibration of hydroxyl groups of water (Min et al. 2017). It can be observed that both adsorption peaks at 3400 and 1620 cm− 1 of XMC5-600 and XMC10-600 decreased when compared with the FTIR spectra of XMC5 and XMC10, respectively. Therefore, the influence of the carbonization process with increasing the temperature of thermal treatment to 600°C that evaporated water inside the pores and released the gases (Morales-Torres et al. 2010; Huang et al. 2018). The bands at 1584 cm− 1 are associated with the C = C stretching in the aromatic ring (Gore et al. 2018). The band in the region of 1271 cm− 1 is due to the C-O stretching vibrations in C–O–C structure caused by the formation of methylene and methyl ether bridges between the aromatic rings (Morales-Torres et al. 2012). The 571 cm− 1 band is attributed to Fe-O stretching vibration that can be present in magnetite composite in RF carbon xerogels affecting the arsenic adsorption (Min et al. 2017).
Figure 5(b) illustrates the FTIR of XMC10-600 before and after As(V) adsorption. After As(V) adsorption on XMC10-600, it can be observed the decreased bands at 2950 cm− 1 (C–H stretching) and 1584 cm− 1 (C = C aromatic stretching) that corresponded to ring C–C bond stretch of aromatic compound of resorcinol-formaldehyde interacted with arsenic on the adsorption process (Gore et al. 2018). It can also be found in the presence of the new band peak with small intensity at 1490 cm− 1 due to Fe = O bonds (Ruiz-Mora et al. 2022).
Models fitted and optimal parameters.
The evaluation of the removal of arsenic using XMC5-600 was carried out executing a RSM and consisted of a response variable which was removal efficiency of arsenic, three independent variables dose of adsorbent, initial concentration of arsenic and solution pH with three levels (low, medium, high). The experimental method and data analysis was implemented using the statistical software R v4.0.3.
Equations 3 and 4 describe the most significant parameters after applying the RSM method with respect to the removal efficiency of As(V) and As(III), respectively. Figure 6 shows the contour plot of the removal efficiency of As(V) with two different factors. In Fig. 7 the x and y axes show the two variable input parameters (pH, dose, or initial concentration) that maximize As(V) removal. It can be seen that the most efficient As(V) removal was achieved for the significant quantitative factors which were x1 = pH and x2 = adsorbent dose (Fig. 6). Moreover, as can be seen in Fig. 7a 3D surface estimation plot represents As(V) removal efficiency as a function of parameter variations pH vs. dose (Fig. 7(a)) and pH vs. concentration. initial (Fig. 7(b)). The maximum efficiency of As(V) removal was obtained when a low pH and a high dose of adsorbent were applied.
Figure 8 illustrates the results of the As(III) removal efficiency contour profile. The highest As(III) removal efficiency was obtained for the significant quantitative factors that were x2 = adsorbent dose and x3 = initial concentration. Equations 3 and 4 describe the most significant parameters after applying the RSM method with respect to the percentage of As(V) and As(III) adsorption, respectively. Code categorical variables were described according to Table 1.
As(V) removal [%] = 28.6177–23.4317x1 + 10.8115x2 − 11.9858x1x2 + 26.0798\({x}_{1}^{2}\) − 9.5217\({x}_{3}^{2}\) (3)
As(III) removal [%] = 51.96523–7.42122x1 + 13.36756x2x3 − 18.22614\({x}_{1}^{2}\) + 15.53519\({x}_{3}^{2}\) (4)
In the statistical study, the optimal values were found using the compute estimated marginal means for factor combinations in a linear model by means of the package emmeans (Lenth 2023) into the R software. The optimum values of pH, dose of adsorbent and initial concentration for the removal of As(V) 95.03±5.98% were 3.0, 4.5 g/L, and 0.15 mg/L, and the removal of As(III) 65.04±10.32% were 4.0, 4.5 g/L, and 0.18 mg/L, respectively, that calculated regarding the range of quantitative factors of the design of experiments as displayed in Table 1. However, the use of adsorbent dose at 4.5 g/L is quite high and not economical, therefore the continuing experiments were considered to apply only 2 g/L by computing the optimum values with the Eqs. 3 and 4.
Preliminary test for the removal of arsenic
The preliminary test of arsenic removal using magnetic carbon xerogels was studied in a batch experiment. Figure 9. shows the removal efficiency and adsorption capacity of As(V) and As(III) using XMC10-600 were higher than XMC5-600. Both of them demonstrate that their adsorption capacities for As(V) were higher than As(III). Regarding the obtained result, this research was to evaluate XMC10-600 and XMC5-600 in detail the removal of As(V) and As(III), respectively.
Adsorption of As(V) on magnetic carbon xerogel nanocomposites XMC10-600 from aqueous solution
Adsorption kinetics models
In adsorption, as a time-dependent process, it is necessary to know its speed for the design and evaluation of adsorbents. Various kinetic models were used to determine the kinetic adsorption constant. The most used for adsorption kinetics analysis are pseudo first order (PFO) and pseudo second order (PSO) kinetic adsorption models (Lima et al. 2015). Therefore, two kinetic models PFO and PSO were applied to fit the kinetic data by non-linear regression to describe As(V) and As(III) adsorption with XMC10-600 and XMC5-600M adsorbents, respectively, as follows:
Pseudo first-order equation: \({q}_{t}={q}_{e}\left(1-{e}^{{-k}_{1}t}\right)\) (5)
Pseudo second-order model: \({q}_{t}=\frac{{k}_{2}{q}_{e}^{2}t}{1+{k}_{2}{q}_{e}t}\) (6)
Where qt is the amount of arsenic adsorbed at time t (mg/g) and qe is the equilibrium adsorption capacity (mg/g). k1 is the pseudo first order rate constant PFO (min− 1) and k2 is the pseudo second order rate constant PSO (min− 1). t is the contact time (min). α and β are constants of the rate of chemisorption (mg/g min) and the degree of coverage of the surface (g/mg), respectively.
The experimental data was calculated by nonlinear regression analysis to obtain the adsorption kinetic models PFO and PSO as shown in Fig. 10. The corresponding parameter estimates, and correlation coefficients are presented in Table 5. It can be seen that the PSO equation was best described in the As(V) adsorption data due to higher R2 value (0.8427) and lower RMSE value which are considered to represent goodness of conformity.
Table 5
Estimation of the kinetic model parameters and correlation coefficients for the adsorption of As(V) by magnetic carbon xerogel nanocomposites XMC10-600.
Pseudo first-order equation | k1 | qt (µg/g) | R2 | RMSE |
0.027 | 43.367 | 0.770 | 4.127 |
Pseudo second-order equation | k2 | qt (µg/g) | R2 | RMSE |
0.001 | 45.986 | 0.843 | 3.413 |
Adsorption isotherm
An adsorption isotherm describes the phenomenon that governs the retention (or release) of a substance from solution to a solid surface at a temperature and pH constants. Adsorption equilibrium is established when one adsorbate phase is in contact with the adsorbent for a period. Normally, the isotherm is represented graphically by expressing the concentration of adsorbent against its residual concentration. It provides insight into the adsorption mechanism, the degree of harmony of adsorbents and surface properties. In this experiment was analyzed isotherm data by applying Langmuir and Freundlich isotherm models with non-linear regression to describe the relative concentrations of As(V) and As(III) adsorbed to the XMC10-600 and XMC5-600 adsorbents, respectively, as follows:
Langmuir isotherm: qe\(=\frac{\text{b} \text{q}\text{m} \text{C}\text{e}}{(1+\text{b} \text{C}\text{e})}\) (7)
Freundlich isotherm: qe =\(K{Ce}^{\frac{1}{n}}\) (8)
Where qe is the amount of arsenic adsorbed by the XMCs (mg/g), Ce is the equilibrium concentration of adsorbate in solution (mg/L), qm is the maximum adsorption capacity (mg/g), and b is adsorption energy (L/mg) of the Langmuir. K indicates the measure of adsorption capacity and n are Freundlich constants of intensity.
The experiment of the adsorption isotherm for As(V) removal using XMC10-600, was applied with different As initial concentrations between 53–325 µg/L with fixed dose of adsorbent 2 g/L at 25°C. Figure 11 shows the Langmuir and Freundlich isotherms for As(V) adsorption. It can be seen that the As(V) adsorption capacity increased with increasing As(V) concentration. Table 6 summarizes the isotherm parameters and correlation coefficients. It can be seen that a similar value of R2 was found for the Langmuir and Freundlich isotherm. Furthermore, the Freundlich model indicated a better fit to describe the experimental equilibrium data of As(V) adsorption using XMC10-600 due to the higher value of R2. It is evident that As(V) adsorption is similar to having adsorption on a heterogeneous surface instead of monolayer adsorption.
Table 6
Parameters of the Langmuir and Freundlich isotherm models for the adsorption of As(V) on magnetic carbon xerogel nanocomposites XMC10-600.
Langmuir
|
|
Freundlich
|
qm (µg/g)
|
b (L/mg)
|
R2
|
|
K
|
n
|
R2
|
153.4
|
2.797
|
0.827
|
|
158.2
|
1.496
|
0.857
|
Thermodynamics of adsorption
The application of thermodynamics to adsorption is important to realize the behavior of adsorbent react to variable temperatures. Temperature is one of the key parameters in the adsorption process. In the experiment of adsorption thermodynamics, the effect of arsenic adsorption with three different temperatures at 298, 308 and 318 °K was studied using the magnetic carbon xerogel XMC10-600. According to the van't Hoff equation, the thermodynamic parameters are the Gibb free changes (ΔG), the entropy of adsorption (ΔS) and the enthalpy of adsorption (ΔH) of the experimental data were calculated as follows:
ΔG= \(-RTIn\left({K}_{D}\right)\) (9)
ΔG = ΔH-TΔS (10)
ln(KD)= \(-\frac{H}{RT}\)+\(\frac{S}{R}\) (11)
where R is the universal gas constant, T is the absolute temperature, and KD is the equilibrium constant.
According to the results obtained from the experiment of thermodynamics of adsorption, their parameters for the adsorption of As(V) with three different temperatures on magnetic carbon xerogel XMC10-600 are presented in Table 7. It can be seen that negative values of ΔG with all studied temperatures demonstrates that the adsorption of As(V) by using XMC10-600 is a spontaneous process. In the case of ΔH, obtaining the positive value of change in enthalpy of the adsorption indicates the endothermic nature of the adsorption process. Finally, ΔS was positive and indicates that the process is irreversible. Therefore, thermodynamic study of As(V) adsorption on the magnetic carbon xerogel nanocomposites XMC10-600 confirmed that the adsorption process is endothermic and spontaneous in nature due to the negative value of free energy change and positive value of enthalpy change.
Table 7
Thermodynamic parameters for As(V) adsorption on XMC10-600
Temperature (K)
|
ΔG (KJ/mol)
|
ΔH (KJ/mol)
|
ΔS (J/mol)
|
298
|
-1.6191
|
170.8270
|
0.5808
|
308
|
-10.0988
|
|
|
318
|
-9.5648
|
|
|
Adsorption of As(III) on magnetic carbon xerogel nanocomposites XMC5-600M from aqueous solution
In the case of the adsorption of As(III) with XMC5-600M, the conditions for the time effect experiment were: a solution of As(III) with a concentration of 0.1mg/L at pH = 4.6 and kept stirring at 150 rpm. The adsorption kinetics experiment of XMC5-600M fits a pseudo-second order model according to the data shown in Fig. 12 and the values of parameters presented in Table 8. Therefore, XMC5-600M and XMC10-600 can be used for the removal of As(III) and As(V) due to the fact that the materials have a high BET surface area (579.2m2/g), as well as contain of iron with a value of 3.19 and 3.56, respectively. The pHpzc defines the state in which the surface electric charge density is zero, that is, it is neutralized under certain pH conditions, therefore, the point of zero charge after carbonization increases from pHpzc of 4.77 (XMC10) to pHpzc of 9.6 (XMC10-600) (data not shown). The surface of the materials is charged positively at a higher pH and pH dependence of arsenic species in various dominant inorganic forms: H3AsO3, H3AsO4, \({HAsO}_{4}^{2-}\), H2AsO3 (Min et al. 2017).
Table 8
Estimation of the kinetic model parameters and correlation coefficients for As(III) adsorption by magnetic carbon xerogel nanocomposites XMC5-600M.
Pseudo first-order equation
|
k1
|
qt (µg/g)
|
R2
|
RMSE
|
0.054
|
14.242
|
0.708
|
1.055
|
Pseudo second-order equation
|
k2
|
qt (µg/g)
|
R2
|
RMSE
|
0.007
|
14.834
|
0.808
|
0.855
|
The experiment of the adsorption isotherm for As(III) removal using XMC5-600M, was applied with different As initial concentrations between 23–210 µg/L with fixed dose of adsorbent 2 g/L at 25°C. The adsorption constants obtained from the experiment of As(III) adsorption isotherm are listed in Table 9. The values of R2 reveal both models of the Langmuir and Freundlich isotherm were similar. After the surface modification of XMC5-600M, the maximum adsorption capacity of As(III) is 859.5 µg/g. Therefore, an oxidizing agent H2O2 used in the surface oxidation by generating oxygen-containing functional groups of carbon xerogels, consequently enhances the adsorption of arsenic.
Table 9
Parameters of the Langmuir and Freundlich isotherm models for As(III) adsorption on magnetic carbon xerogel nanocomposites XMC5-600M.
Langmuir
|
|
Freundlich
|
qm (µg/g)
|
b (L/mg)
|
R2
|
|
K
|
n
|
R2
|
859.5
|
0.253
|
0.976
|
|
196.1
|
1.021
|
0.975
|
Application of the removal of As(V) and As(III) by using magnetic carbon xerogels in groundwater
Evaluation of the effect of solution pH on As(V) and As(III) adsorption from groundwater in the field experimental site I.
This study area was carried out in Jiutepec, Morelos, Mexico. The effects of pH on As(V) and As(III) removal were studied using XMC10-600 (Fig. 13(a)) and XMC5-600M (Fig. 13(b)), respectively, from groundwater with solution pH = 3 and pH = 5, dose of 2 g/L, initial concentration of arsenic solution of 100 µg/L, contact time of 5 h, and temperature 25°C. The results showed that the As(V) removal efficiency in XMC10-600 for pH 3 and 5 was 74.37% and 47.46%, respectively. The As(III) removal efficiency in XMC5-600 for pH 3 and 5 was 76.62% and 88.41%, respectively. It can be indicated that the effect of pH for As(V) adsorption on XMC10-600 was a significant change in arsenic removal efficiency and adsorption capacity which is different from As(III) adsorption on XMC5-600M which no significant changes are observed in the pH 3 and pH 5.
The reduction of the R/W ratio during the synthesis of xerogel, it can be explained that resorcinol is an important part of formation of the nodules or clusters, and formaldehyde generates the interconnected structure gaining strength of gels, therefore the volume of water added in this synthesis affects to the distance between nodules (Canal-Rodríguez et al. 2020). The higher volume of water added into preparing the RF solution, results in the high segregation of the nodules that are confirmed with less the compactness of XMC10-600 (R/W = 0.4) than XMC5-600 (R/W = 0.5) appearance in the analysis of SEM.
Evaluation of the effect of contact time on arsenic adsorption from groundwater in the field experimental site II.
According to the result of XMC10-600 using for As(V) and As(III) adsorption in groundwater provided from well in the state of Durango as illustrated in Fig. 14, shows the removal efficiency and qe for pH 3 and pH 5 approximately 48–74% and 18.70–29.30 µg/g, respectively, that was lower than results obtained from XMC5-600M. Therefore XMC10-600M was modified to surface with H2O2 as described above to evaluate the arsenic adsorption in groundwater provided from wells in the state of Durango that heavy metals As and F− were over than the permissible limit established by NOM-127-SSA1-2021. The condition obtained from experimental design with RSM was applied in this application of groundwater and performed in the condition: an initial arsenic concentration of 0.06 mg/L, an adsorbent dose of 2 g/L, solution pH of 3 a stirring speed of 150 rpm at a temperature of 25–28°C with different contact time of 4 h and 24 h. The performance of XMC10-600M in the removal efficiency of arsenic were 96.79% and 97.5% at contact time 4 h and 24 h, respectively (Fig. 14). The adsorption capacity with different contact time of 4 h and 24 h were similar of 104.5-105.3 µg/g, therefore, the optimum contact time was 240 minutes, and the appropriate pH was found to be 3.0 can lower the arsenic from groundwater to comply with the requirements of NOM-127-SSA1- 2021. Regard to the physical-chemical characterization of the real water, this natural groundwater contains nonmetallic and heavy metals (F−, Fe and Mn) and abundant anion ions such as Cl−, \({NO}_{3}^{-}, {SO}_{4}^{2-}{ and PO}_{4}^{3-}\) but the presence of these ions did not significantly affect the performance of arsenic removal. It can be explained that the presence of interfering ions of groundwater replace in the adsorption process of arsenic, but in the case of lower solution pH, showing a higher selectivity for adsorbing arsenic and a higher number of sites (Bono et al. 2021).
The surface modification of XMC5-600M and XMC10-600M exhibits surface chemistry heterogeneity strongly due to containing of various functional groups and influence to increase the adsorption capacity, also the main mechanisms controlling the surface chemistry such as repulsive and dispersive interactions, and hydrogen bonds (Pego et al. 2019). The results of porous structural morphology with high surface area and low pore volume, were caused by the increment of the ratio of surface area to overall volume of magnetic carbon xerogels that were affected to have higher the adsorption capacity of As(III) and As(V) (Bono et al. 2021). The mesoporous matrix of resorcinol-formaldehyde carbon xerogel provide the hierarchical pathways for the adsorbate molecules like arsenic in the adsorption process and the surface modification of these adsorbents improved and enhanced the adsorption capacity (Faizal and Zaini 2019). Moreover, the carbonization under an inert atmosphere removes oxygen and hydrogen, can control the microclusters and porous properties on the resulting magnetic carbon xerogel with high specific surface areas, thermally stable nanostructure carbon and affect the adsorption capacity of arsenic (Canal-Rodríguez et al. 2017).