4. Minor Inclusions.
Fine-grained inclusions and fragments are present on the surface of large plate-like particles. They are more clearly visible at high magnifications, which may indicate a secondary phase or the result of mechanical grinding.
The sample under investigation exhibits a lamellar layered morphology with a high degree of particle agglomeration. The structure is predominantly dense; however, inter-aggregate pores become visible at lower magnifications. The presence of fine inclusions on the particle surfaces indicates structural heterogeneity and the possible presence of secondary phases.
The polysaccharide biopolymer matrix is characterized by a highly developed porous structure dominated by macropores, which is typical of natural carbohydrate polymers. This morphological organization facilitates the efficient diffusion of metal ions to active functional centers and accounts for high sorption activity, as well as the ability to form gel-like structures.
Figure 2.
Raman spectrum of a pectin-based biopolymer matrix.
Figure 2.
Raman spectrum of a pectin-based biopolymer matrix.
Table 7.
Interpretation of the Raman spectrum of a pectin-based biopolymer matrix.
Table 7.
Interpretation of the Raman spectrum of a pectin-based biopolymer matrix.
| № |
Wavelength, cm⁻¹ |
Purpose |
| 1 |
~400–600 |
C–C and C–O vibrational modes in a polysaccharide chain |
| 2 |
~800–900 |
Vibrations of the glycosidic bond (C–O–C) characteristic of polysaccharides |
| 3 |
~900–950 |
Vibrations of β-glycosidic bonds |
| 4 |
~1000–1150 |
Valence C–O and C–C vibrations in galacturonic acid rings |
| 5 |
~1200–1300 |
C–H and O–H vibrational modes |
| 6 |
~1350–1450 |
C–H and O–H vibrational modes; vibrational modes of CH₂ and CH₃ groups |
| 7 |
~1600–1750 |
Vibrations of carboxyl groups (–COO⁻, –COOH) |
| 8 |
~2800–3000 |
C–H stretching vibrations (the most intense peak in the spectrum) |
Typical of glycosidic bonds → confirms the polysaccharide structure.
Bound to carboxyl groups a key area for analyzing interactions with metals.
Conclusion regarding the spectrum:
The Raman spectrum confirms that the sample under investigation is a polysaccharide (pectin) containing:
These functional groups serve as active sites for the sorption of Cu²⁺ and Zn²⁺ ions.
Figure 3.
FTIR spectra of a polysaccharide biopolymer matrix isolated from dahlia tubers before and after sorption of Cu²⁺ ions.
Figure 3.
FTIR spectra of a polysaccharide biopolymer matrix isolated from dahlia tubers before and after sorption of Cu²⁺ ions.
Table 8.
FTIR characteristics of pectin from Dahlia tubers and changes upon Cu²⁺ binding.
Table 8.
FTIR characteristics of pectin from Dahlia tubers and changes upon Cu²⁺ binding.
| № |
Absorption wavelength range, cm⁻¹ |
Recommended dosages of pectin (dahlia tubers) |
Changes upon binding of Cu²⁺ |
| 1 |
3600–3200 |
Valence vibrations of –OH (hydroxyl groups), hydrogen bonds |
Broadening and shift of the band → contribution of –OH groups to complex formation with Cu²⁺ |
| 2 |
2920–2850 |
C–H valence vibrations (–CH₂, –CH₃) |
No significant changes |
| 3 |
1740–1700 |
Valence vibrations of C=O (ether and carboxyl groups –COOH, –COOCH₃) |
Decrease in intensity → deesterification and involvement in binding |
| 4 |
1650–1600 |
Asymmetric vibrations of carboxylate ions –COO⁻ |
Band shift and broadening → coordination of Cu²⁺ with –COO⁻ |
| 5 |
1450–1400 |
Symmetric vibrations –COO⁻ |
Band shift → change in the coordination environment |
| 6 |
1320–1200 |
C–O vibrations (carboxyl and hydroxyl groups) |
Minor changes → involvement of oxygen-containing groups |
| 7 |
1150–1000 |
C–O–C (glycosidic bonds) and C–O vibrations |
Minor changes → preservation of the pectin structure |
| 8 |
900–700 |
C–H stretching vibrations, pyranose ring vibrations |
No significant changes |
| 9 |
<700 |
Cu–O vibrations |
The appearance of faint bands → confirmation of complex formation |
When pectin from Dahlia tubers interacts with Cu²⁺ ions, shifts are observed in the 1600–1400 cm⁻¹ region, corresponding to carboxylate groups, indicating their involvement in coordination. Additionally, changes in the ~3400 cm⁻¹ region indicate the involvement of hydroxyl groups. This confirms the formation of complex compounds between pectin and Cu²⁺.
Figure 4.
FTIR spectra of a polysaccharide biopolymer matrix isolated from Jerusalem artichoke tubers (Helianthus tuberosus) before and after sorption of Cu²⁺ ions.
Figure 4.
FTIR spectra of a polysaccharide biopolymer matrix isolated from Jerusalem artichoke tubers (Helianthus tuberosus) before and after sorption of Cu²⁺ ions.
Table 9.
FTIR spectrum of pectin (Helianthus tuberosus) and changes upon Cu²⁺ binding.
Table 9.
FTIR spectrum of pectin (Helianthus tuberosus) and changes upon Cu²⁺ binding.
| № |
Absorption wavelength range, cm⁻¹ |
Uses of pectin (Helianthus tuberosus) |
Changes upon binding of Cu²⁺ |
| 1 |
3400–3200 |
O–H valence vibrations (hydroxyl groups, hydrogen bonds) |
Broadening of the band, shift toward the low-frequency region—the role of OH in complex formation |
| 2 |
2940–2880 |
C–H valence vibrations (–CH, –CH₂ groups) |
Minor changes or no change |
| 3 |
1750–1730 |
Valence vibrations of C=O groups in ester groups (–COOCH₃) |
Decreased intensity, possible shift—partial demethoxylation/involvement in coordination |
| 4 |
1650–1600 |
Asymmetric vibrations of COO⁻ (carboxylate groups) |
Shift and intensity increase — complex formation with Cu²⁺ |
| 5 |
1450–1400 |
Symmetric vibrations of COO⁻ |
Peak shift—evidence of coordination via carboxyl groups |
| 6 |
1330–1250 |
C–O and O–H (strain) vibrations |
Change in intensity — involvement of hydroxyl groups |
| 7 |
1150–1000 |
C–O–C valence vibrations (glycosidic bonds) |
Minor changes in the structure of the polysaccharide chain |
| 8 |
900–800 |
Vibrations of β-glycosidic bonds |
Virtually unchanged |
The binding of Cu²⁺ ions to pectin from Helianthus tuberosus is accompanied by characteristic shifts in the 1600–1400 cm⁻¹ and 3400 cm⁻¹ regions, indicating the key role of carboxyl (–COO⁻) and hydroxyl (–OH) groups in the complexation process. The shift and change in the intensity of the bands confirm the formation of coordination bonds between Cu²⁺ and the functional groups of pectin.
Figure 5.
FTIR spectra of a polysaccharide biopolymer matrix isolated from dahlia tubers before and after Zn²⁺ ion sorption.
Figure 5.
FTIR spectra of a polysaccharide biopolymer matrix isolated from dahlia tubers before and after Zn²⁺ ion sorption.
Table 10.
FTIR spectrum of pectin (Dahlia tubers) and changes upon Zn²⁺ binding.
Table 10.
FTIR spectrum of pectin (Dahlia tubers) and changes upon Zn²⁺ binding.
| № |
Absorption wavelength range, cm⁻¹ |
Recommended dosages of pectin (dahlia tubers) |
Changes upon binding of Zn²⁺ |
| 1 |
3600–3200 |
Valence vibrations of –OH (hydroxyl groups), intramolecular and intermolecular hydrogen bonds |
Band narrowing and shift → involvement of –OH groups in complex formation |
| 2 |
2920–2850 |
Valence vibrations C–H (–CH₂, –CH₃) |
Virtually unchanged |
| 3 |
1740–1700 |
Valence vibrations of C=O (ether and undissociated carboxyl groups –COOH, –COOCH₃) |
Decrease in intensity → partial deesterification and involvement in binding |
| 4 |
1650–1600 |
Asymmetric vibrations of carboxylate ions –COO⁻ |
Band shift and broadening → coordination of Zn²⁺ with –COO⁻ |
| 5 |
1450–1400 |
Symmetric vibrations –COO⁻ |
Change in the position of the band → confirmation of complex formation |
| 6 |
1320–1200 |
C–O vibrations (carboxyl and hydroxyl groups) |
Minor shift → involvement of oxygen-containing groups |
| 7 |
1150–1000 |
Vibrations C–O–C (glycosidic bonds), C–O vibrations (alcohol groups) |
Minor changes → preservation of the polysaccharide structure |
| 8 |
900–700 |
Vibrational vibrations C–H, structural vibrations of the pyranose ring |
No significant changes |
| 9 |
<700 |
Metal–oxygen (Zn–O) vibrations |
Appearance/intensification of faint bands → confirmation of complex formation |
FTIR spectra showed that, following interaction with Zn²⁺ ions, a shift in the bands in the 1600–1400 cm⁻¹ region was observed, corresponding to the asymmetric and symmetric vibrations of the carboxylate groups. This indicates the involvement of pectin –COO⁻ groups in the complexation process with Zn²⁺ ions. A change in the intensity of the ~3400 cm⁻¹ band was also noted, indicating the participation of hydroxyl groups.
The binding of Zn²⁺ to pectin from Dahlia tubers occurs primarily via carboxyl groups (–COO⁻), as evidenced by the shift and change in intensity of the bands in the 1600–1400 cm⁻¹ region. Hydroxyl groups may also be involved in the process.
Figure 6.
FTIR spectra of the polysaccharide biopolymer matrix isolated from dahlia (Helianthus tuberosus) tubers before and after Zn²⁺ ion sorption.
Figure 6.
FTIR spectra of the polysaccharide biopolymer matrix isolated from dahlia (Helianthus tuberosus) tubers before and after Zn²⁺ ion sorption.
Table 11.
FTIR characteristics of pectin from Helianthus tuberosus tubers and changes upon Zn²⁺ binding.
Table 11.
FTIR characteristics of pectin from Helianthus tuberosus tubers and changes upon Zn²⁺ binding.
| № |
Absorption wavelength range, cm⁻¹ |
Recommended dosage of pectin (Helianthus tuberosus) |
Changes upon binding of Zn²⁺ |
| 1 |
3600–3200 |
Valence vibrations of –OH (hydroxyl groups), hydrogen bonds |
Band narrowing and shifting → involvement of –OH in the coordination of Zn²⁺ |
| 2 |
2920–2850 |
Valence vibrations C–H (–CH₂, –CH₃) |
No significant changes |
| 3 |
1740–1700 |
Valence vibrations of C=O (ether and undissociated carboxyl groups –COOH, –COOCH₃) |
Decrease in intensity → deesterification and involvement in Zn²⁺ binding |
| 4 |
1650–1600 |
Asymmetric vibrations of carboxylate ions –COO⁻ |
Band shift and broadening → coordination of Zn²⁺ with –COO⁻ |
| 5 |
1450–1400 |
Symmetric vibrations –COO⁻ |
Band shift → change in the coordination state of carboxyl groups |
| 6 |
1320–1200 |
Vibrations C–O (carboxyl and hydroxyl groups) |
Minor changes → involvement of oxygen-containing groups |
| 7 |
1150–1000 |
Vibrations C–O–C (glycosidic bonds), C–O vibrations (alcohol groups) |
Minor changes → preservation of the polysaccharide structure |
| 8 |
900–700 |
stretching vibrations C–H, pyranose ring vibrations |
No significant changes |
| 9 |
<700 |
Vibrations Zn–O |
Appearance/intensification of faint bands → confirmation of complex formation |
For pectin derived from Helianthus tuberosus, Zn²⁺ binding occurs primarily via carboxyl groups (–COO⁻), as evidenced by shifts in the absorption bands in the 1600–1400 cm⁻¹ range, as well as changes in the hydroxyl group region (~3400 cm⁻¹).
Table 12.
Primary mechanism of metal binding by pectins.
Table 12.
Primary mechanism of metal binding by pectins.
| Functional group |
IR signatures |
Chemical reaction |
Differences between Dahlia tubers and Helianthus tuberosus |
| Carboxyl (–COO⁻) |
Absorption bands: 1650–1600 cm⁻¹ (Dahlia), 1630–1600 cm⁻¹ (Helianthus); Absorption bands: 1450–1410 cm⁻¹ |
Mе²⁺ + 2(C₆H₇O₆⁻) → Mе(C₆H₇O₆)₂ |
The main coordination centers for both; the predominant influence in Dahlia tubers |
| Esters (–COOCH₃) |
Decrease in the intensity of the 1750–1730 cm⁻¹ band |
C₆H₇O₆–COOCH₃ + H₂O → C₆H₇O₆–COOH + CH₃OH; 2(C₆H₇O₆–COOH) + Mе²⁺ → Mе(C₆H₇O₆)₂ + 2H⁺ |
For Helianthus, partial deesterification is possible, creating additional carboxyl groups; in Dahlia, this effect is less pronounced |
| Hydroxyl (–OH) |
Broadening and weakening of the 3600–3200 cm⁻¹ band (Helianthus); 1330–1250 cm⁻¹ band (Dahlia) |
2(C₆H₇O₆–OH) + Mе²⁺ → (C₆H₇O₆–O)₂Mе + 2H⁺ |
The –OH group is more prominent in Helianthus; in Dahlia, it is primarily present as –COO⁻ |
| Polysaccharide backbone |
The 1150–1000 and 950–850 cm⁻¹ bands |
(C₆H₈O₆)ₙ + Mе²⁺ → [(C₆H₈O₆)ₙ]·Mе²⁺ |
The carbohydrate backbone remains intact; the structural integrity of both biopolymers is preserved upon binding of any metal ions |
FTIR analysis shows that the interaction of polysaccharide biopolymers from Dahlia tubers and Helianthus tuberosus with heavy metal ions (Cu²⁺, Zn²⁺) occurs primarily through carboxyl groups (–COO⁻), with partial involvement of ester (–COOCH₃) and hydroxyl (–OH) groups. The polysaccharide backbone retains its structural integrity, confirming that the sorption process is of a coordination-complex nature. In Dahlia tubers, carboxyl groups play a predominant role, whereas in Helianthus tuberosus, the involvement of hydroxyl groups is more pronounced. These data indicate the high sorption capacity of both matrices and confirm their potential as natural sorbents for heavy metals.
Figure 7.
Kinetic curves of Cu2+ and Zn2+ ion sorption on polysaccharide biopolymer matrices DT (Dahlia tubers) and HT (Helianthus tuberosus).
Figure 7.
Kinetic curves of Cu2+ and Zn2+ ion sorption on polysaccharide biopolymer matrices DT (Dahlia tubers) and HT (Helianthus tuberosus).
Figure 8.
Comparative removal efficiency of Cu2+ and Zn2+ ions from aqueous media using DT and HT biopolymer matrices.
Figure 8.
Comparative removal efficiency of Cu2+ and Zn2+ ions from aqueous media using DT and HT biopolymer matrices.
Sorption of Cu²⁺ Ions
As shown (
Table 2), the initial concentration of Cu²⁺ was 9.24 mg/L (0.1455 mmol/L) for DT and 8.97 mg/L (0.1412 mmol/L) for HT. Already after 5 minutes, the concentration dropped sharply to 3.50 mg/L and 3.39 mg/L, respectively, corresponding to removal efficiencies of 62.12% and 62.20%.
When the contact time was increased to 10 minutes, the removal efficiency rose to 76.80% (DT) and 76.81% (HT). In the 10–30-minute range, a gradual increase in efficiency was observed up to 82.70–82.72%, which is associated with the saturation of active sorption sites.
By 60 minutes, equilibrium was established: the residual concentration was 1.55 mg/L (DT) and 1.52 mg/L (HT), and the degree of purification reached 83.22% and 83.05%, respectively. The sorption capacity in this case was 5.13 mg/g for DT and 4.97 mg/g for HT.
Sorption of Zn²⁺ Ions
A similar pattern was observed for Zn²⁺ (
Table 3). The initial concentration was 7.99 mg/L (0.1223 mmol/L) for DT and 7.32 mg/L (0.1120 mmol/L) for HT.
After 5 minutes, the removal efficiency reached 74.70% (DT) and 62.20% (HT), indicating a higher initial efficiency of DT with respect to Zn²⁺. Subsequently, the process slowed down, and by 10–20 minutes, the removal efficiency stabilized at 76.8–77.7%.
After 30 minutes, a further increase in efficiency to 82.70% was observed, and by 60 minutes, equilibrium values of 83.00% (DT) and 82.80% (HT) were reached. The sorption capacity was 4.42 mg/g for DT and 4.04 mg/g for HT.
Thus, the degree of purification is a key parameter confirming the high efficiency of both sorbents. For Cu²⁺ and Zn²⁺, the main removal of ions occurs in the first 10–20 minutes, when the degree of purification reaches 75–77%, after which the process slows down and reaches a plateau.
Overall, both materials demonstrate comparable efficiency with a final removal rate of about 83%, which indicates the high sorption capacity of the DT and HT polysaccharide biopolymer matrices.
Figure 9.
Comparative analysis of the agreement between experimental and calculated values for the sorption of Cu²⁺ and Zn²⁺ ions for the DT and HT matrices.
Figure 9.
Comparative analysis of the agreement between experimental and calculated values for the sorption of Cu²⁺ and Zn²⁺ ions for the DT and HT matrices.
To evaluate the sorption mechanism and the reliability of the experimental data, the experimental adsorption values (A_(exp)) were compared with theoretical calculations based on the Langmuir and Freundlich models for Cu²⁺ and Zn²⁺ ions (
Table 4 and
Table 5).
Sorption of Cu²⁺ ions
According to
Table 4, the experimental Cu²⁺ adsorption values for the DT sorbent ranged from 0.0603 to 0.0807 mmol/g, while the calculated values according to the Langmuir model were 0.0720–0.0860 mmol/g, and according to the Freundlich model—0.0610–0.0810 mmol/g.
The Aex/Al ratio for DT ranged from 0.84 to 0.94 with a mean of 0.92, whereas Aex/Af ranged from 0.99 to 1.00, indicating a closer fit of the experimental data to the Freundlich model.
A similar trend was observed for HT: A_(ex)/A_l = 0.85–0.94 (mean 0.91), A_(ex)/A_f ≈ 0.99. This indicates that the Freundlich model better describes the Cu²⁺ sorption process compared to the Langmuir model.
Zn²⁺ Ion Sorption
For Zn²⁺ (
Table 5), the experimental adsorption values ranged from 0.0609 to 0.0676 mmol/g for DT and from 0.0465 to 0.0618 mmol/g for HT. The calculated values according to Langmuir were in the range of 0.0710–0.0770 mmol/g, and according to Freundlich, 0.0615–0.0670 mmol/g.
The Aex/Al ratio for DT was 0.86–0.89 (mean 0.87), and for HT, 0.82–0.87 (mean 0.85). At the same time, the Aex/Af values were close to unity (≈0.99–1.01), confirming the high agreement of the experimental data with the Freundlich model.
The results indicate that the sorption of Cu²⁺ and Zn²⁺ ions on the DT and HT polysaccharide biopolymer matrices is better described by the Freundlich model, which indicates the heterogeneous nature of the sorbent surface and the non-uniform distribution of active sites.
The lower fit of the Langmuir model (Aex/Al < 1) indicates the limited applicability of the assumption of monolayer sorption. At the same time, the closeness of the Aex and Af values (Aex/Af ≈ 1) confirms the correctness of the process description within the framework of multilayer adsorption on a heterogeneous surface.
Overall, both sorbents exhibit comparable behavioral patterns, with DT characterized by a slightly higher adsorption capacity compared to HT, especially in the case of Cu²⁺.
The results obtained show good agreement between the experimental and calculated values of Cu²⁺ and Zn²⁺ cation adsorption for the Langmuir and Freundlich models. The values of the Aex/Af ratio are close to unity (0.99–1.01) in all cases, indicating a high degree of agreement between the experimental data and the Freundlich model. This points to the heterogeneous nature of the sorbent surface and the presence of active adsorption sites with different energies.
For the Langmuir model, the Aex/Al ratio values range from 0.82 to 0.94. The lower values compared to the Freundlich model indicate that the Langmuir model slightly overestimates the sorption capacity of the biosorbent under study. Nevertheless, the obtained coefficients remain sufficiently close to unity, which confirms the applicability of this model for describing the adsorption process.
For Cu²⁺ cations, a better fit to the Langmuir model is observed compared to Zn²⁺, especially for the DT sample, where the average value of Aex/Al is approximately 0.92. For Zn²⁺, the average Aex/Al values are slightly lower (0.85–0.87), which may be due to differences in the hydrated radius and the mechanism of interaction between zinc ions and the functional groups of the biosorbent.
The virtually identical A_(ex)/A_f values for the DT and HT samples indicate that heat treatment has no significant effect on the distribution of active surface sites. This confirms the preservation of the main functional groups responsible for binding heavy metal ions.
Overall, the results demonstrate that the Freundlich model more accurately describes the adsorption process of Cu²⁺ and Zn²⁺ cations by the studied biopolymer sorbent compared to the Langmuir model. This indicates a multistep sorption mechanism and energy heterogeneity of the material’s surface.