3.2. Fourier-Transform Infrared (FTIR) Analyses
Figure 3 shows the FTIR spectra of untreated pine sawdust (UPSD) and cellulose fibres (CF) before they were used for adsorption. The application of NaOH to pine sawdust resulted in the dissolution of lignin and soluble extracts, improving the chemical reactivity of the surface functional groups [
31]. Acid hydrolysis modified pine sawdust’s physical and structural properties [
22]. In
Figure 3, a shift from 3336.87 cm
−1 (UPSD) to 3322.50 cm
−1 for cellulose fibres (CF) indicated a change in the hydroxyl group (-OH). Additionally, the peak at 2886.80 cm
−1 suggested the presence of aliphatic C–H group stretching vibrations of the -CH
3 and -CH
2 groups, implying the existence of aliphatic hydrocarbon chains. No shift was detected, indicating that the functional groups directly attached to the aliphatic chains remained intact. However, their intensity decreased, suggesting a reduction in the concentration of aliphatic C–H groups following acid treatment. The band at 1726.52 cm
−1 (UPSD) C=O signifies that the stretching vibration of the C=O of carboxyl groups shifted to 1721.73 cm
−1 in the cellulose fibres (CF). The peaks observed at 1587.67 and 1506.27 cm
−1 (UPSD) denote N-H and N-O; in the cellulose fibres (CF), the two bands appeared to be merged at 1597.24 cm
−1. UPSD shows peaks at 1425.14 cm
−1 and 1257.30 cm
−1 associated with the stretching of the carboxylic/aromatic hydroxyl group (-OH) of the phenol group, and the band at 1025.94 cm
−1 shows the stretching vibration of the C-O of the primary alcohol group. However, the carboxyl/aromatic hydroxyl (-OH) stretching band for the cellulose fibres (CF) shifts to 1434.45 cm
−1, and the C-O of the primary alcohol shifts to 1021.89 cm
−1.
Figure 4 compares the major functional groups for UPSD and cellulose fibres (CF) after adsorption. A shift and a decrease in intensity were observed, indicating that a metal binding process occurred at the surface of the adsorbents. Following the metal biosorption process, distinct alterations were noted in the wavenumbers (3338.18 cm
−1, 2977.77 cm
−1, 2901.16 cm
−1, 1166.32 cm
−1, and 1054.06 cm
−1) [
32]. The observed shifts, accompanied by a slight decrease in peak intensity, indicated the participation of hydroxyl and carboxyl groups in the adsorption of chromium ions (VI). Additionally, the bands within the range of 1625 to 900 cm
−1, primarily originating from C–OH groups, exhibited a slight decrease in intensity after the reaction. This reduction signified the removal of these groups from cellulose due to oxidation by Cr (VI). Consequently, cellulose’s C–OH groups served as the solution’s reductant for Cr (VI) [
33].
3.4. SEM–EDS Analysis
Figure 6 displays SEM images, while
Figure 7 presents EDX analyses of (a) untreated pine sawdust, (b) cellulose fibres before adsorption and (c) cellulose fibres after adsorption for examining the chemical composition of the adsorbent. The SEM examination of untreated pine sawdust (
Figure 6a) reveals a rough surface with distinct crystalline patterns resulting from the regular arrangement and boundaries of cells like tracheids in pinewood. The roughness was caused by the irregular shape and size of the wood particles formed during cutting. The presence of lignin, cellulose, and hemicellulose in pine wood further contributes to the observed crystalline patterns on the surface. Lignin, an amorphous polymer, forms crystalline regions within the cell walls of wood fibres, becoming visible when the wood is converted to sawdust. In
Figure 6b, acid hydrolysis effects on cellulose fibres are evident, resulting in significant changes such as reduced length, increased irregularity, and a higher aspect ratio than untreated fibres. The rinsing process following hydrolysis uncovers gaps between crystallites that were previously filled with dissolved sugars, further leading to morphological changes in the cellulose fibres. In
Figure 6c, cellulose fibres display surface modifications resulting from their interaction with chromium ions. These alterations may involve chromium species binding or forming a chromium oxide layer on the fibre surface. These surface-level changes have the potential to reduce the carbon content, as evidenced by the observations in
Table 1, SEM images, and EDS graphs.
Table 4 and
Figure 7 present the elemental composition percentages of carbon (C), oxygen (O), and chromium (Cr) in untreated pine sawdust (UPSD) and cellulosic fibres. The results for untreated pine sawdust (UPSD) (
Figure 7a) indicate that carbon (C) constitutes approximately 54.31% of the weight and 61.29% of the atoms. Carbon is a significant component of organic materials, such as wood. Oxygen (O) is approximately 45.69% of the weight and 38.71% of the atoms. Oxygen can be found in organic and inorganic compounds and is a common element in biomass.
Table 4 and
Figure 7 display the elemental composition percentages of carbon (C), oxygen (O), and chromium (Cr) in both untreated pine sawdust (UPSD) and cellulosic fibres. The results for untreated pine sawdust (UPSD) (
Figure 7a) show that carbon (C), being a significant component of organic materials like wood, makes up around 54.31% of the weight and 61.29% of the atoms. Oxygen (O), a common element in organic and inorganic compounds, including biomass, constitutes approximately 45.69% of the weight and 38.71% of the atoms. Prior to adsorption, cellulose fibres (
Figure 7b) have a similar elemental composition to UPSD (untreated pine sawdust), with carbon (C) accounting for approximately 54.33% of the weight and 63.10% of the atoms. Oxygen (O) constitutes 39.57% of the weight and 34.50% of the atomic percentage. Notably, the carbon content remains relatively constant before adsorption, but its presence is no longer observed after absorption. The reduction in carbon (C) content in cellulose fibres after chromium (Cr) adsorption in
Figure 7c could be attributed to several factors, one of which may be the modifications induced by Cr ions’ adsorption on the fibre surface [
37]. These modifications could involve the formation of new chemical bonds, crosslinking, or the deposition of Cr ions’ compounds on the fibre surface. Consequently, new non-carbon components may remove or replace carbon-containing functional groups. This overall effect could have decreased carbon content, supporting the findings observed in the FTIR and XRD results (
Section 3.2 and
Section 3.3).
In adsorption, oxygen (O) content increased, constituting approximately 51.67% of the weight and 72.44% of the atoms. Meanwhile, chromium (Cr) content was around 12.02% of the weight and 5.19% of the atoms, indicating successful chromium ions (VI) adsorption onto the cellulose fibre. The elemental analysis results demonstrated changes in the fibre’s composition during adsorption. The increase in chromium content suggested binding to the adsorbent, while the increase in oxygen content indicated overall compositional changes in the cellulose fibre [
38,
39].
3.7. Thermogravimetric (TGA) Analysis
Figure 10 displays the TGA and DSC thermograms of the (a) UPSD and (b) cellulose fibres (CF) in the temperature range of 25–900 °C.
Figure 9a shows an apparent weight loss that occurred at three different temperature ranges for both graphs. In the temperature range of 25–100 °C, the first phase of weight loss results in a decrease of nearly 6.82% for UPSD (
Figure 10a) and 5.13% for cellulose fibres (CF), as demonstrated in
Figure 10b through the TGA and DSC thermograms. This could be attributed to removing water molecules from the surface of the adsorbent, which is known to possess hygroscopic properties [
7,
44]. The second stage of weight loss is observed to commence around 100 °C and is completed at 350 °C, resulting in a reduction of approximately 56.6% for UPSD (
Figure 10a) and 68.95%, as shown in
Figure 10b through the TGA and DSC thermograms, for both UPSD and cellulose fibres (CF) in the temperature range of 25 to 900 °C, utilising a heating rate of 10 C/min. The mass loss for UPSD may be attributed to the breakdown of hemicelluloses and some portions of lignin at 300–450 °C. Additionally, the massive loss for the cellulose fibres (CF) (
Figure 10b) thermogram may be due to the thermal decomposition of the carbonyl in the adsorbent surface [
23].
In the third phase, from 350 to 700 °C, a weight loss of 14.22% for UPSD (
Figure 10a) corresponds to the decomposition of cellulose at about 450–700 °C. The weight reduction in cellulose fibres (CF) depicted in
Figure 10b, which amounts to 17.49%, occurs at a temperature above 400 °C and is ascribed to the carbonisation mechanism of cellulose chains. Moreover, the morphology of untreated pine sawdust (
Figure 10a) does not exhibit significant changes in contrast to cellulose fibres (CF) (
Figure 10b) because of the existence of lignin, which comprises numerous aromatic rings with diverse branches [
45].
The DSC thermograms in
Figure 10 demonstrate that UPSD and cellulose fibres (CF) remain in a consistent chemical and physical state throughout the temperature range of 30–350 °C. Additionally, the thermogram illustrated in
Figure 10a displays a reduction in weight between 250 °C and 450 °C, which could be attributed to the breakdown of hemicellulose. Similarly, in
Figure 10b, the DTA peak observed at approximately 350–450 °C shows a slight weight loss of about 20%, which may also be associated with the decomposition of cellulose in the sample. In the DTA graph (
Figure 10b), cellulose fibres are stable up to 450 °C [
46].
3.9. Isotherm Study for Adsorption of Chromium
Adsorption isotherms were demonstrated by plotting the amount of solute adsorbed per unit of adsorbent against the equilibrium concentration in the bulk solution while maintaining a constant temperature. In
Figure 16a,b, logarithmic plots are generated to fit the linear and nonlinear Freundlich and Langmuir isotherms, respectively, for a concentration of 100 ppm at 299 K. The plots of log C
e versus log q
e for the Freundlich isotherm and C
e versus C
e/q
e for the Langmuir isotherm were used to analyse the adsorption behaviour and establish the fitting parameters for the respective isotherm models. The Langmuir adsorption isotherm, which assumes that the adsorption occurs in a monolayer and that similar active sites are uniformly distributed on the adsorbent surface with no interaction, was found to govern the adsorption process. The results presented in
Table 4 indicate that the linear correlation coefficient, R
2, had a value of 0.9958. The Langmuir constant (K
L) indirectly relates to the maximum monolayer adsorption capacity (mg/g). The relationship between the solute and the adsorbent’s affinity, supported by K
L, the Langmuir isotherm coefficient [
50], showed contrasting values in this study. A higher K
L value indicated a stronger affinity between the solute and the adsorbent. However, this study observed contrasting K
L values when comparing the linear and nonlinear Langmuir plots. The K
L value of 2.9 × 10
−3 in the linear Langmuir plot indicated a relatively weak affinity between the solute and the adsorbent. Conversely, in the nonlinear Langmuir plot, the K
L value was 171.589, suggesting a significantly higher affinity between the solute and the adsorbent. The low K
L value from the linear plot may be indicative of factors like incomplete monolayer formation or heterogeneity in the adsorbent surface, which weaken the solute’s affinity to the adsorbent.
In contrast, the high K
L value obtained from the nonlinear plot suggests a strong affinity between the solute and the adsorbent. This was possibly due to the nonlinear plot accommodating deviations from the ideal assumptions, resulting in a more accurate representation of the adsorption process and indicating a higher affinity between the solute and the adsorbent [
56]. Additionally, the Langmuir isotherm can be mathematically expressed using a dimensionless constant, the separation factor (R
L), represented by Equation (6).
where the R
L value indicates the characteristics of the biosorption process. Suppose the R
L values range from 0 to 1; in this case, they indicate a favourable biosorption process: R
L greater than 1 represents the unfavourable biosorption, R
L equal to 1 represents the linear biosorption, and R
L equal to 0 specifies the irreversible biosorption process but is favourable when 0 < R
L < 1 [
57,
58]. The linear and nonlinear Langmuir R
L was 0.476 and 6.5 × 10
−2, respectively (
Table 5), suggesting favourable biosorption. The nonlinear Langmuir isotherm model better describes the adsorption data points than the linear Langmuir isotherm model, as indicated by the R
L values. A lower R
L value suggests a stronger affinity between the adsorbate (chromium (VI)) and the adsorbent (cellulose fibres) at various equilibrium concentrations. Moreover, the R
L value implies that the total light power absorbed by the sample does not follow a linear relationship with the incident light intensity. This suggests that the incident irradiance influences the absorption coefficient, and multiple absorption mechanisms are at play, leading to nonlinear absorption behaviour. These various absorption mechanisms contribute to the nonlinear results observed in the study, supporting the findings obtained from the nonlinear analysis [
59].
The
Table 5 results offer essential insights into the adsorption behaviour and fitting parameters of the linear and nonlinear Freundlich isotherm models. The parameter “n” in the Freundlich equation signifies the adsorbent surface heterogeneity. In the linear Freundlich model, “n” has a relatively high value (12.136), indicating significant heterogeneity on the adsorbent surface. This implies that a wide range of binding energies influenced the adsorption process. In contrast, in the nonlinear Freundlich model (
Figure 16b), “n” has a significantly lower value (3.95 × 10
−2), suggesting a reduced degree of heterogeneity. These findings suggest that the nonlinear Freundlich model better fit the experimental data compared to the linear model.
Additionally, since the value of “n” is more significant than 1 in the nonlinear Freundlich model, the adsorption isotherm becomes increasingly nonlinear, deviating from ideal behaviour and leading to physisorption. Physical adsorption is facilitated by van der Waals forces between atoms or molecules on the adsorbent surface and the adsorbate [
60,
61]. The parameter k
F in the Freundlich equation represents the adsorption capacity of the adsorbent. In both the linear and nonlinear models, the k
F value is approximately 10, indicating a moderate adsorption capacity. The high k
F values implies a significant uptake of chromium ions onto the absorbent surface [
62].
The coefficient of determination (R2) evaluates the model’s good fit to the experimental data. For the linear Freundlich model, the R2 value is 0.8854, indicating a reasonable fit between the model and the experimental data. However, in the case of the nonlinear Freundlich model, the R2 value is substantially higher (0.9988), which signified an excellent fit between the model and the experimental data. Therefore, the higher R2 value indicates a closer agreement between the model and the observed data.
Error Analysis for Isotherm
Three distinct linear error functions are utilised to assess the goodness of fit of the isotherms, and these functions are considered an effective method for analysing experimental data generated from the adsorption process.
Sum of the Squares of the Errors (SSE). The sum of the squares of the errors (SSE) is similar to the Sum of the Absolute Errors Function (SAE), which is the most-used error function (Equation (7)) [
63]:
Residual root-mean-square error (RMSE). RMSE is also a widely used error evaluation function, and the mathematical form is
This error evaluation function is used if the deviation between the experimental and predicted values is significant. Additionally, RMSE is commonly used to prevent models that generate occasional significant errors and adhere to the normal distribution, which is the foundation for fitting ordinary least squares regression models [
64].
Chi-square test,
χ2 can be used to confirm the best-fit isotherm for the adsorption system (Equation (9)); if the results from the model are similar to the experimental results, χ
2 is a small number; if they are different, χ
2 is a large number [
65].
where q
m is the equilibrium capacity obtained by calculating from the model (mg/g), and q
e is the equilibrium capacity (mg/g) experimental data. The parameter k
F in the Freundlich equation represents the adsorption capacity of the adsorbent. In both the linear and nonlinear models, the k
F value was approximately 10, indicating a moderate adsorption capacity. The high k
F values implied a significant uptake of chromium ions onto the absorbent surface [
62].
Table 6 demonstrates that the nonlinear Langmuir model was better than the linear Langmuir model in various aspects. It had a significantly lower sum of squares error (SSE) of 0.1158 compared to 1.84 × 10
−2, indicating a better fit with reduced discrepancies between the observed and predicted values. The root-mean-square error (RMSE) was also lower in the nonlinear model (0.1079) compared to the linear model (1.46 × 10
−2), suggesting more minor average deviations. The χ
2 value for the nonlinear Langmuir model was much lower (3.14 × 10
−7) than that of the linear model (8.40 × 10
−2), indicating a superior fit. Additionally, the nonlinear model had a higher R
2 value of 0.9992 than the linear model’s R
2 value of 0.9985, explaining a more significant proportion of the total variation in the data. Moreover, the Sum of Normalised Errors (SNE) was substantially smaller for the nonlinear model (6.976 × 10
−4) than the linear model (2.78 × 10
−2), further confirming it was a better fit.
The nonlinear Freundlich model (
Figure 16b) had a higher SSE of 5.44 × 10
−3 than the linear Freundlich model’s SSE of 2.82 × 10
−4. This indicated that the linear Freundlich model provides a better fit due to its smaller sum of squares error, implying reduced differences between the observed and predicted values. Additionally, the linear Freundlich model had a lower RMSE of 7.13 × 10
−3 than the nonlinear Freundlich model’s RMSE of 3.46 × 10
−2, suggesting minor average deviations between the observed and predicted values. Moreover, the χ
2 value for the linear Freundlich model (4.91 × 10
−5) was significantly lower than the nonlinear Freundlich model’s χ
2 value (6.20 × 10
−3), indicating a better fit for the linear model. On the other hand, the nonlinear Freundlich model had a higher R
2 value (0.9988) than the linear Freundlich model’s R
2 value of 0.8854, explaining a more significant proportion of the total variation in the observed data and suggesting a better fit. Furthermore, the Sum of Normalised Errors (SNE) value for the linear Freundlich model (7.52 × 10
−3) was smaller than the nonlinear Freundlich model’s SNE value (5.44 × 10
−3), indicating a better fit for the linear Freundlich model [
66].
The nonlinear Langmuir model (
Figure 16a) was better than the linear Langmuir model with lower SSE, RMSE, χ
2, and SNE values and a higher R
2 value. In contrast, the linear Freundlich model proved superior to the nonlinear Freundlich model with lower SSE, RMSE, χ
2, and SNE values and a comparable R
2 value. These findings highlighted the superior performance of the nonlinear Langmuir model in describing the relationship between the concentration of chromium (VI) in solution and the amount adsorbed onto the adsorbent; the higher R
2 value explained a more significant proportion of the total variation in the observed data. Conversely, the linear Freundlich model performed better for chromium (VI) adsorption onto pine sawdust and cellulose fibres than the nonlinear Freundlich model [
66].
3.10. Kinetic Study for Adsorption of Chromium
The pseudo-first-order and pseudo-second-order kinetic models (
Figure 17a,b) were studied to understand the rate and type of adsorption. A linear relationship can be observed by plotting log(q
e − q
t) against time (t), which enables the determination of biosorption rate constant (k
1), q
e (cal), and the correlation coefficient (R
2) [
21]. The k
1 and q
e (cal) values in mg/g of Cr (VI), calculated from the plot shown in
Figure 17, are 8.2 × 10
−3 and 1.5739 mg/g, respectively.
Table 7 indicates that the correlation coefficient (R
2 = 0.9108) suggests the pseudo-first-order model did not provide a good fit. Birhanu et al. [
67] reported comparable findings when studying chromium removal from synthetic wastewater using the low-cost Odaracha adsorbent from Ethiopia. Additionally, the experimental adsorption result (q
e (exp)) was exceptionally higher than that of q
e (cal), which further revealed that the pseudo-first-order model was not suitable to explain the adsorption kinetics of chromium ions on cellulose fibres (CF)’s adsorbent.
Figure 17 shows the kinetics plots of (a) linear and (b) nonlinear PFO and PSO for the adsorption of hexavalent chromium ions on cellulose fibres (CF).
Figure 17a reveals a linear trend in the plot of t/q
t against time, indicating that the pseudo-second-order kinetic model produced the best fit, with a correlation coefficient value (R
2 = 0.9999) close to unity, as shown in
Table 8. The experimental adsorption equilibrium value (q
e exp.) of 9.7772 mg g
−1 agree with the calculated adsorption equilibrium value (q
e cal.) of 9.7847 mg g
−1. Based on the results, it can be concluded that the pseudo-second-order model is a suitable fit for describing the adsorption kinetics of chromium using the cellulose fibres (CF)’s adsorbent. The obtained results suggest that the adsorption of chromium ions by the cellulose fibres (CF)’s adsorbent is controlled by chemisorption, which involves the exchange of metal ions with the functional groups present on the surface of the adsorbent [
68].
The results in
Figure 17b and
Table 7 suggest that nonlinear kinetics models (Cr (VI)) are not suitable for describing adsorption kinetics. The experimental adsorption equilibrium value (q
e exp.) of 0.706 mg g
−1 aligns with the calculated adsorption value, which is lower than the equilibrium value (q
e cal.) of 9.7847 mg g
−1.
Equation (10) defines the initial rate of sorption (h).
where h (mg g
−1 min
−1) can be regarded as the initial adsorption rate when the initial concentration of metal ions does not influence t → 0, which is the initial adsorption rate (h). Rather, it is determined by the likelihood of collisions between the relevant species and the speed at which chromium ions can bind to the reactive sites present on the surface of the adsorbent [
69].
Error Analysis for Kinetics
The results of the error function, as displayed in
Table 8, suggest that the experimental data are best described by a pseudo-second-order kinetic model, which corroborates the Langmuir isotherm (as discussed in
Section 3.5). The findings indicate that the attachment of chromium onto cellulose fibres (CF) is a chemisorption process. Furthermore, the pseudo-second-order model exhibits lower SSE, RMSE, and χ
2 values, indicating that it could be a better fit [
70].
3.13. Reusability Test
To determine the number of times the adsorbent can be recycled, a reusability test was conducted on the cellulose fibres (CF).
Figure 18 presents the results of the first three cycles of the adsorbent’s reusability study. The results in
Figure 18 reveal that cycles two and three demonstrated lower adsorption of Cr (VI) ions than cycle one on the cellulose fibres (CF)’s adsorbent. Furthermore, the results show that HCl was the best eluent for Cr (VI) ions to determine adsorbent reusability. The highest removal efficiency for Cr (VI) ions was 79% with HCl, while it was 76%, 30%, and 29% for the other solvents (NaOH, CH
3COOH, and H
2O, respectively). The results also indicated that during the regeneration process, cellulose fibres (CF) could not completely desorb the Cr (VI) ions that had been adsorbed onto the surface and pores during cycle one.
Consequently, the removal percentage decreased for cycles two and three. However, the decline in removal percentage in cycles two and three was much more pronounced for the CH3COOH and H2O solvents than for HCl and NaOH. The results demonstrated that the adsorbents could be recycled at least three times, indicating the adsorbents’ economic advantage.