2.5. Particle Size Analysis
Particle size values of the studied carbons measured in 0.001 mol/dm
3 NaCl and 0.001 mol/dm
3 NaNO
3 at different pH are summarized in
Table 4,
Table 5 and
Table 6.
Table 4,
Table 5 and
Table 6 present the particle size measurements of the tested adsorbents in two electrolytes. Particle size measurements of different activated carbons in the same electrolyte show a significant dependence on pH, primarily due to changes in the surface charge density of the particles and their tendency to aggregate or disperse in solution. At low pH, the surface of the activated carbon particles can become protonated, reducing the surface charge, and the zeta potential approaches zero, a consequence of the weaker electrostatic repulsion between particles. This results in particle aggregation, which manifests itself in larger particle sizes than at higher (alkaline) pH. Functional groups (e.g., –OH) are deprotonated, increasing the negative surface charge. The negative zeta potential increases, a consequence of the stronger electrostatic repulsion between particles. This bicarbon/electrolyte system is more colloidally stable; the particles remain more dispersed, resulting in smaller particle sizes. Particle size measurements for the same activated carbon differ depending on the type of electrolyte, such as NaCl and NaNO
3, even though both are monovalent electrolytes (Na
+). These differences are mainly due to the influence of anions (Cl
− vs. NO
3−) on the colloidal stability and double layer structure around the activated carbon particles. The first important phenomenon in such systems is surface charge shielding: both electrolytes reduce the thickness of the electrical double layer, which reduces electrostatic repulsion between particles. The second important difference is based on the anions: Cl
− vs. NO
3−. Cl
− and NO
3− have different adsorption abilities on the activated carbon surface and different polarities and hydration radii. NO
3− has a larger hydration radius than Cl
−, resulting in the formation of a thicker hydration layer and greater colloidal stability of the system. Cl
− can adsorb more easily to the surface, which changes the surface charge and leads to stronger aggregation. For our activated carbons presented in
Table 4,
Table 5 and
Table 6, we see that for BH+KOH, larger grains are present in the NaCl electrolyte than for NaNO
3. This is a result of the aggregation process and weaker hydration of Cl
− ions. For the BH+KOH+urea and BH+KOH+Fe samples, the opposite is true, resulting from the interaction of functional groups on the surface with these electrolytes. Measuring activated carbon particle size depends on the type of modification, as each modification affects: surface structure (porosity, presence of functional groups), surface charge (and therefore zeta potential), colloidal stability (i.e., susceptibility to aggregation), and interaction with the electrolyte (e.g., ion adsorption, shielding). Activated carbons modified with KOH (BH+KOH) have a highly developed surface area and numerous basic groups (-OH), and high porosity. This results in smaller particle sizes (reduced aggregation). The system is more stable in both electrolytes, but NaNO
3 may provide slightly greater stability due to better NO
3− hydration. BH+KOH+urea samples modified with urea have nitrogen-containing groups (–NH
2), which increase the hydrophilicity of these samples and have a moderate effect on porosity. As a result, the average particle size may depend on interactions with ions and, therefore, may be pH-dependent, and amine groups may undergo protonation. Therefore, their particle size is smaller in NaCl (lower stability) than in NaNO
3. BH+KOH+Fe samples have a surface coated with an inorganic ferrocyanide complex (Fe
4[Fe(CN)
6]
3), which increases the charge and mass of the particles and reduces their porosity. Prussian Blue can interact with Cl
− and NO
3− ions, affecting the stability of the more complex system.
2.6. Electrical Double Layer (EDL) Analysis
In the adsorption of ions on solid surfaces, phenomena occurring at the solid-solution interface play a key role. The effectiveness and mechanism of adsorption depend on the way in which solid-phase particles interact with ions and molecules in solution. An ordered structure of matter, known as an electric double layer (EDL), forms at this interface, constituting a fundamental element in describing the electrokinetic and surface properties of disperse systems. Among the most important experimental quantities characterizing EDL are surface charge density and zeta potential. In recent years, these parameters have been increasingly considered in the scientific literature as significant factors describing the behavior of modern adsorbents, alongside their surface and structural characteristics [
33,
34].
Figure 4 and
Figure 5 show the changes in surface charge density as a function of pH for the tested materials: BH+KOH, BH+KOH+urea, and BH+KOH+Fe, in a 0.001 mol/dm
3 NaNO
3 and NaCl solutions. In all cases, a significant decrease in surface charge density was observed with increasing pH, particularly below pHpzc for the tested samples, which is consistent with the expected behavior for materials containing dissociable hydroxyl groups on their surfaces. For the adsorbents modified with KOH and urea (BH+KOH and BH+KOH+urea), the surface charge density is very similar throughout the tested pH range. As pH increases, a decrease in surface charge values is observed, reaching negative values in the alkaline pH range. This indicates that deprotonation of functional groups occurs and negative charges appear. In the case of the BH+KOH+Fe adsorbent, the surface charge density is practically negative from pH = 5.8. This result is consistent with the presence of iron oxides or hydroxyoxides, which impart a permanently acidic character and a strongly negative charge to the surface. The minimum σ value for this material reaches approximately −10 mC/cm
2 for NaNO
3 and −20 mC/cm
2 for NaCl, indicating a potentially high electrostatic cation adsorption capacity.
Figure 5 and
Figure 6 present changes in surface charge density (σ) as a function of pH for the tested materials: BH+KOH, BH+KOH+urea, and BH+KOH+Fe in a 0.001 mol/dm
3 NaCl solution. This parameter is an important indicator of the electrostatic nature of the adsorbent surface and directly influences its ability to adsorb ions. In all cases, a significant decrease in surface charge density was observed with increasing pH, which is consistent with the expected behavior for materials containing dissociable hydroxyl groups on the surface. For adsorbents modified with KOH and urea (BH+KOH and BH+KOH+urea), the surface charge density remains positive in the pH range < 6–7, indicating the presence of protonated groups (–OH
2+, –NH
3+). As pH increases, a decrease in surface charge is observed, reaching negative values in the alkaline pH range. This indicates deprotonation of functional groups and the appearance of negative charges (e.g., –O
−, –COO
−). The x-axis intercept corresponds to the point of zero charge density (pHpzc), which for these materials is approximately, for BH+KOH, pH ~8.5–9, and for BH+KOH+urea, pH ~8–8.5, respectively. In the case of the BH+KOH+Fe adsorbent, the surface charge density is negative throughout the analyzed pH range, suggesting a very low pHpzc, below pH 5. This result is consistent with the presence of iron oxides or hydroxyoxides, which impart a permanently acidic character and a strongly negative charge to the surface. The minimum σ value for this material reaches approximately ~(−35 mC/cm
2), which indicates a potentially high electrostatic adsorption capacity for cations (e.g., heavy metals) under neutral and alkaline conditions. In
Figure 6a–c, the plots for all three samples (BH+KOH, BH+KOH+urea, BH+KOH+Fe) show a similar trend. For each sample, the values of surface charge density in the NaCl solution are more negative than those in NaNO
3 at the same pH. This difference arises from the distinct adsorption behavior of Cl
− and NO
3− ions. The Cl
− ion exhibits a higher affinity for the surface, leading to a more negative charge. This indicates that the chloride anion has a stronger influence on the surface potential compared to the nitrate anion, suggesting the occurrence of specific Cl
− adsorption. The BH+KOH+Fe sample shows the highest negative charge at elevated pH values, implying that this material may have the greatest adsorption potential toward metallic cations (e.g., Ag
+, Pb
2+). The observed trend indicates a gradual increase in surface acidity with modification (KOH → Urea → Fe).
The ζ-potential dependences on pH in the studied electrolytes are presented in
Figure 7.
Although NaCl and NaNO
3 at a concentration of 0.001 mol dm
−3 exhibit identical ionic strength and comparable bulk properties, differences in anion size, hydration energy and interfacial behavior may lead to subtle but measurable variations in electrokinetic parameters such as zeta potential, pHpzc and pH
iep. To determine the electrostatic nature of the surfaces of the studied adsorbents, zeta potential measurements were performed as a function of pH in a 0.001 mol/dm
3 NaNO
3 solution. The obtained curves are presented in
Figure 7. All analyzed materials—BH+KOH, BH+KOH+urea, and BH+KOH+Fe—exhibit a negative zeta potential over a wide pH range, indicating the dominance of functional groups that impart a negative surface charge, such as –O- or –COO
−. For the BH+KOH and BH+KOH+urea adsorbents, zeta potential values close to zero were observed at pH ~2.0 and ~2.5, respectively, indicating isoelectric points (pH
iep) in this range. With increasing pH, the zeta potential becomes increasingly negative, reaching values of approximately −30 mV at pH 9–10, suggesting increasing colloidal stability and a strongly negative surface charge. The BH+Fe adsorbent exhibits different characteristics: the zeta potential from pH ~3 onwards assumes significantly more negative values (approximately −20 mV), not reaching positive values throughout the entire pH range studied. This indicates the acidic nature of the material’s surface and the isoelectric point below pH 2. The presence of iron oxides may contribute to a higher negative charge density on the surface and a greater capacity for adsorption of positive ions, especially in the neutral and alkaline pH range. It is worth noting that at pH > 6, all materials exhibit zeta potentials less than −20 mV, indicating good colloidal stability of the suspension systems. The highest negative zeta potential value was achieved for the BH+KOH+Fe sample, suggesting its potentially highest efficiency in cation adsorption processes over a wide pH range.
Figure 8 shows the dependence of the zeta potential on pH for three adsorbents: BH-KOH, BH+KOH+Urea, and BH+KOH+Fe, in a 0.001 mol/dm
3 NaCl electrolyte. The aim of the measurements was to determine the nature of the zeta potential of the tested materials and to identify their isoelectric points (pH
iep), which are key for predicting their adsorption properties and colloidal stability. All materials exhibit negative zeta potential over a wide pH range, indicating the dominance of acidic functional groups capable of dissociating and generating a negative charge. The KOH-activated adsorbent exhibits a zeta potential close to zero at pH ~2.5, suggesting an isoelectric point in this range. As pH increases, the zeta potential value decreases, reaching a minimum of approximately −25 mV at pH ~9. In the pH range of 6–10, the material exhibits a relatively stable, negative zeta potential, indicating favorable colloidal stability and the presence of persistent –OH
− groups on the surface. The BH+KOH+urea sample exhibits a similar curve to BH+KOH, but with slightly less negative values in the alkaline pH range. The isoelectric point of the material is observed at pH ~2. The minimum zeta potential reaches a value of approximately −22 mV at pH ~9. The adsorbent surface remains negatively charged throughout the tested pH range, which may be due to the presence of amide groups or urea residues (e.g., –NH
2), which modify the electrostatic properties. The iron-modified material (BH+KOH+Fe) exhibits significantly more negative zeta potential than the other samples throughout the pH range. At pH 3, it reaches a value of approximately −20 mV, and the minimum zeta potential is observed at pH ~9 and is approximately −35 mV. The isoelectric point lies outside the studied pH range (<2), indicating the strongly acidic nature of the surface. The presence of iron oxides or hydroxyoxides (e.g., FeOOH) may promote strong dissociation of –OH groups and the generation of a negative charge. This characteristic makes BH+KOH+Fe potentially the most effective adsorbent of cations over a wide pH range.
The increase in zeta potential observed for some samples at very high pH values may be attributed to compression and reorganization of the electric double layer as well as specific interactions of OH− ions with surface functional groups. In the case of the BH+KOH+urea sample, the presence of nitrogen-containing surface functionalities introduces additional acid–base equilibria, leading to a non-linear pH dependence of the zeta potential. The observed maximum may result from complete deprotonation and subsequent reorientation of nitrogen groups, combined with changes in the position of the shear plane and possible aggregation effects under strongly alkaline conditions.
Table 7 presents the pHpzc and pH
iep points depending on the type of electrolyte and adsorbent. pHpzc (point of zero charge) is the pH at which the total surface charge of the adsorbent is zero. Above pHpzc, the surface is negatively charged. Below pHpzc, the surface is positively charged. pH
iep (isoelectric point) is the pH at which the zeta potential = 0, meaning the particle has no electrophoretic mobility. This is the point at which the particle does not migrate in an electric field, which is important for colloid stability. The RH–KOH sample has a very high pHpzc; the material has a positive surface charge over a wide pH range < 9.7. A large difference between pHpzc and pH
iep (>7 units) means that despite the positive charge, the surface is not necessarily electrokinetically neutral. Colloidal stability for this system is most likely only at pH close to pHiep (~2.4), and agglomeration may occur in other ranges. The BH+KOH+urea adsorbent also has a high pHpzc; the surface is strongly positive at lower pH. The preferential adsorption behavior of different anions on carbonaceous surfaces has been reported in the literature. For instance, activated carbon has been shown to exhibit markedly different affinities toward nitrate and chloride ions, with nitrate often being adsorbed more strongly under comparable conditions due to differences in ion hydration and solvation structure [
35].
The pHpzc shifts slightly higher in NaNO
3 than in NaCl, influenced by the type of anion. The material will be negatively charged only at pH > 9. The BH+KOH+Fe material has significantly lower pHpzc values than for BH+KOH and BH+KOH+Urea; the BH+KOH+Fe surface is negatively charged over most of the pH range. This indicates the presence of acidic groups on the surface (e.g., –OH groups bound to iron oxides). The pHpzc increases in the presence of NO
3−, likely due to adsorption of the anion, which changes the surface potential. pH
iep < 2. Additionally, the surface is almost always charged, which means high colloidal stability, and this is beneficial for dispersive materials. For example,
Figure 5 and
Figure 6 present changes in surface charge density (σ) as a function of pH for the tested materials, BH+KOH, BH+KOH+urea, and BH+KOH+Fe, in a 0.001 mol/dm
3 NaCl solution. This parameter is an important indicator of the electrostatic nature of the adsorbent surface and directly influences its ability to adsorb ions. In all cases, a significant decrease in surface charge density was observed with increasing pH, which is consistent with the expected behavior for materials containing dissociable hydroxyl groups on the surface. For adsorbents modified with KOH and urea (BH+KOH and BH+KOH+urea), the surface charge density remains positive in the pH range < 6–7, indicating the presence of protonated groups (–OH
2+, –NH
3+). As pH increases, a decrease in surface charge is observed, reaching negative values in the alkaline pH range. This indicates deprotonation of functional groups and the appearance of negative charges (e.g., –O
−, –COO
−). The x-axis intercept corresponds to the point of zero charge density (pHpzc), which for these materials is approximately, for BH+KOH, pH ~8.5–9, and for BH+KOH+urea, pH ~8–8.5, respectively. In the case of the BH+KOH+Fe adsorbent, the surface charge density is negative throughout the analyzed pH range, suggesting a very low pHpzc, below pH 5. This result is consistent with the presence of iron oxides or hydroxyoxides, which impart a permanently acidic character and a strongly negative charge to the surface. The minimum σ value for this material reaches approximately −35 mC/cm
2, which indicates a potentially high electrostatic adsorption capacity for cations (e.g., heavy metals) under neutral and alkaline conditions.