3.1.1. Identification of interactions between microparticle constituents
The infrared spectra of the initial components of sodium alginate, chitosan, zinc sulfate, and silver nitrate were recorded (
Figure 1a), and compared with the microparticle spectra (
Figure 1b). Despite the complexity of the spectra as a result of the overlapping of different absorption bands as well as the coupling of different vibrations, valuable information was obtained about the molecular interactions of microparticle constituents. In the spectra analyses, more attention is focused on those absorption bands corresponding to the characteristic molecular vibrations where changes occur due to the alginate gelation. The most noticeable changes are observed in the area of the functional groups of hydroxyl and carboxyl.
The spectrum of the sodium alginate shows a strong broadband assigned to the stretching modes of the hydroxyl groups (–OH) with a peak at 3300 cm
-1 and a shoulder at 3198 cm
-1. Stretching vibrations of weak intensity observed at 2900 cm
-1 correspond to –CH
2 groups and very sharp stretching at 1595 cm
-1 and medium sharp stretching at 1405 cm
-1 correspond to vibrations of asymmetric and symmetric carboxyl groups (COO
-). A weak broad CO stretching can be observed at 1295 cm
-1, while bands at 1026 cm
-1 are characteristic of polysaccharides [
22].
The spectrum of chitosan is characterized by a broadband occurring between 3291 - 3610 cm
-1 due to the stretching vibrations of the -OH groups that overlapped with the stretching vibration of the -NH
2 groups. Vibrations at 2925 cm
-1 (peak of lower intensity) and 2875 cm
-1 (peak of higher intensity) are assigned to asymmetric and symmetric modes of CH
2 vibrations, respectively. Characteristic bands of N-acetyl groups: C=O stretching (amide I), −NH bending (amide II), and C-N stretching (amide III), are arising at wave numbers 1645, 1550 and 1325 cm
−1 [
23]. The medium intensity peak at 1373 cm
-1 belongs to the symmetric CH
3 deformation, while the vibrations in the region 1190-920 cm
-1 belong to the C-N stretching and overlapping vibrations from the carbohydrate ring [
24].
The spectrum of silver nitrate has several peaks at 3328, 2129 and 1635 as well as a broad high intensity at 1300 cm
-1 due to the stretching vibration of the N=O bond in NO
3- [
25]. Due to the presence of water, the spectrum of zinc sulfate heptahydrate shows a broad band around 3100 cm
-1 and a narrower band at 1657 cm
-1 occurring due to O–H stretching vibrations and H–O–H deformation vibrations, respectively. The peaks observed at 1100, 983, and 612 cm
-1 correspond to the stretching vibration of sulfate groups [
26].
The FTIR-ATR spectra of the microparticles are presented in
Figure 1b. The presence of cations in the alginate matrix causes the most significant changes in the area of alginate functional groups: hydroxyl (OH) and carboxyl (COO
-), indicating that the interactions of microparticle constituents are mainly hydrogen bonds and electrostatic interactions [
11]. Compared to the sodium alginate spectrum, the spectrum of zinc alginate shows a more intense and wider stretching band of hydroxyl groups (–OH), which indicates the formation of new hydrogen bonds. More intense, somewhat broader bands of asymmetric (at 1589 cm
-1) and symmetric (at 1409 cm
-1) (COO
-) carboxyl groups are the result of interactions with Zn
2+ ions and crosslinking by binding to carboxyl groups of guluronic and mannuronic acids, in contrast to Ca
2+ ions that bind mainly to guluronic carboxyl groups [
27]. The structure of the three-dimensional network of zinc alginate is looser and contains larger amounts of water than calcium alginate.
The mechanism of ion-induced crosslinking of alginate chains is based mainly on the interaction of multivalent cations and carboxyl groups. According to the quantum chemical computational method, alkaline earth cations form ionic bonds with alginate chains, while transition metal ions form complexes with covalent coordination bonds [
28]. The binding of zinc ions has been attributed, by some authors, to an exclusive covalent coordination bond with carboxyl groups [
29,
30]. However, although Zn
2+ is a transition metal (but with an ionic radius comparable to alkaline earth metals), the analysis of the main features of zinc hydrogels showed more similarities to alkaline earth hydrogels. It was concluded that the bond of zinc with alginate, although quite weak, is predominantly ionic [
30].
The spectrum of ALG/(Zn+Ag) shows slightly lower intensities of the characteristic peaks without significant shifts. A somewhat narrower and less intense absorption band of hydroxyl groups around 3300 cm
-1 and reduced intensities of the peaks attributed to carboxyl groups indicate slightly weakened hydrogen bonds and electrostatic interactions compared to ALG/Zn. The lower intensity of the broadband assigned to the hydroxyl groups implies the breaking of some of the inter- and intramolecular hydrogen bonds in ALG/(Zn+Ag), possibly due to the formation of a complex between Ag
+ and oxygen atoms from O-H groups [
31]. Furthermore, from the slight differences in the spectra of zinc alginate microparticles and those with encapsulated silver, it was not possible to unambiguously detect the formation of a bond between sodium alginate and silver ions. Lin et al. [
32] attributed the interaction of Ag
+ ions with the sodium alginate matrix to van der Waals interactions, while Zhang et al. [
33] showed that Ag
+ can also react electrostatically with anionic alginate, that is, under certain conditions, it is possible to gel alginate by ionic crosslinking with monovalent Ag
+ cations, similar to crosslinking with Ca
2+ cations.
A significant increase in the intensity and broadening of the absorption band around 3300 cm
-1 and an increase in the intensities of vibrations at 1406, 1292, and 1020 cm
-1 in the spectrum of zinc alginate coated with a layer of chitosan (CS/(ALG/Zn)) are the result of the formation of hydrogen bonds due to the complexation of Zn
2+ ions with the amino and hydroxyl groups of chitosan [
34,
35,
36]. The lack of other characteristic chitosan bands in the spectra can be explained by the complexation of sodium alginate and chitosan [
11].
All characteristic band intensities in the spectrum of CS/(ALG/(Zn+Ag)) are slightly reduced compared to those of ALG/(Zn+Ag). The broad band around 3300 cm
-1 is mainly attributed to N-H stretching vibrations (amide A), although in that region the N-H and O-H stretching vibrations overlap [
37]. Transmission reduction in this region shows that Ag
+ is bound to N-H groups. Other changes observed in the wavenumbers (shifts from 1585 to 1571 cm
-1, 1406 to 1392 cm
-1, and from 1020 to 1045 cm
-1) are related to the bending of N-H groups, by stretching of C-N groups and N-H oscillating deformation. All these changes indicate that Ag
+ ions bind to nitrogen atoms and thus reduce the intensity of vibrations of N-H bonds [
38].
The comprehensive analysis of the infrared spectra provided insightful details into the molecular interactions and structural changes of the sodium alginate, chitosan, zinc sulfate, and silver nitrate when formulated as microparticles. The significant alterations in the absorption bands, especially within the regions associated with hydroxyl and carboxyl groups, reinforced the understanding of the interactions, including hydrogen bonding and electrostatic interactions, prevalent among the microparticle constituents. This deepened understanding of the ion-induced crosslinking and associated bonding dynamics paves the way for fine-tuning the microparticle properties for desired applications.
3.1.2. Size, surface morphology, and topography of microparticles
Generally, the size and uniformity of microparticles are determined mainly by the viscosity of the alginate solution, the diameter of the nozzle, the solution flow rate, and the distance between the point from a nozzle to the gelling bath [
39]. Under our experimental conditions, the microparticles prepared were mostly spherical and light brown. The surface of the wet microspheres was smooth, while the surface of the wet microcapsules was slightly rippled. It can be seen that the addition of silver and chitosan increased the size (
Table 1). By lyophilization, the sphericity of the microparticles was lost, and the surface characteristics were modified becoming irregular and wrinkled. Their sizes are reduced and approximately two times smaller than those of wet microcapsules (
Table 1).
The surface morphology of dried microparticles studied at different SEM magnifications is presented in
Figure 2. After drying, all of the microparticles were deformed, and the surface became wrinkled with more or less intertwined fibers and pronounced pores. The appearance of wrinkles can be attributed to the loss of water and moisture associated with the stress relaxation processes of biopolymers [
40]. The coating of the zinc alginate microspheres with chitosan (
Figure 2e) resulted in more pronounced wrinkles with somewhat thicker fibers and waviness. Compared to zinc alginate microspheres with an average pore size of ~69 nm (
Figure 3c), the average pore size of microcapsules is smaller (~65 nm) (
Figure 2f).
The loading of zinc alginate microspheres with silver showed a surface with thicker fibers and a somewhat higher size of pores (~73 nm) (
Figure 2i) compared to zinc alginate. This implies a change in the structure of the gel network due to the silver interactions with alginate and the mechanical influence of cations with a larger ionic radius (the ionic radius of silver ions is 0.126 nm, and that of zinc ions is 0.074 nm). The chitosan layer on the surface of ALG/(Zn+Ag) microspheres is thinner than on the surface of zinc alginate (fibers are thinner and less intertwined) (
Figure 2k) with a smaller average pore size (~63 nm) (
Figure 2l). The pore size on the surface of the microparticles plays an important role in the release rate of the encapsulated material. The release of encapsulated active substances is faster from microparticles with a larger pore size and vice versa [
41].
The EDS spectra analysis of the area nearest to the surface (the electron probe can penetrate to a depth of about 1 μm) exhibited the major percentage of elements corresponding to C and O (
Figure 3) The detection of Zn on the surface of the microparticles indicated a part of the Zn is localized near the surface. The small amount of detected S was probably a residue of sulfate used during formulation preparation (cation donor solution - ZnSO
4). In silver-loaded microparticles, it is also localized near the surface.
The AFM images presented in
Figure 4 and
Figure 5 complemented the SEM analysis of the surface morphology. The scanned sample area presented by topographic images of height data is shown as the "top view" characterizing individual microparticle morphology and the "3D surface view" with corresponding color scale characterizing the microparticle 3D-height distribution (
Figure 4) while the characteristic vertical profile ("section analysis") of a single microparticle reveals a quantitative 2D height analysis (
Figure 5). The ALG/Zn microspheres have granules on the surface that are spatially oriented due to the grain structure and have a regular spherical shape linearly arranged due to the cross-linking of the negatively charged alginate chains by Zn
2+ ions. A similar structure was already described by Simpliciano et al. [
42]. Such crosslinking leads to a high value of roughness (R
a = 76±1 nm) (
Table 2). The addition of chitosan does not change grain morphology but leads to a loss of directionality and restricts crosslinking to two dimensions, which is expressed in a lower roughness (R
a = 7.47±0.02 nm). The addition of Ag+ to ALG/Zn leads to a reduction in the size of the grains, which still have a regular spherical shape, while the degree of lateral crosslinking is reduced and manifests itself in a reduced roughness (R
a = 21.97±0.52 nm) respect to the surface of ALG/Zn (see section analysis profiles in
Figure 5). The addition of chitosan to ALG/(Zn+Ag) microspheres only slightly reduces the crosslinking that is still directional, resulting in a slightly lower roughness (R
a = 18.62±0.45 nm).
3.1.3. Encapsulation efficiency, loading capacity, swelling degree, and cation releasing from microparticles
The determination of encapsulation efficiency (EE) and loading capacity (LC) was performed to obtain information on the relative amount of Zn
2+ and Ag
+ ions encapsulated in the microparticles. The results on the loading efficiency and loading capacity of Zn
2+ and Ag
+ ions are presented in
Table 3. The encapsulation efficiency for Zn
2+ ions is very high and was almost the same for all types of microparticles. Also, 100% EE indicated that almost all Ag
+ ions were encapsulated. The addition of chitosan decreased the loading capacity of microcapsules in comparison to microspheres due to the diffusion in the media during the microcapsule process preparation.
When dispersed in solution, microparticles swell, thus changing many properties, such as mechanical strength, permeability, release behavior, stability, and the rate of disintegration. The swelling process involves two underlying molecular processes: (i) penetration of the solution into the matrix and (ii) relaxation of polymer stress (transition of glassy structure to a rubbery state) [
43]. The greater extent of swelling of microparticles simultaneously loaded with Zn
2+ and Ag
+ ions than those loaded only with Zn
2+ ions may be attributed to the less dense alginate network structure due to the addition of Ag
+ ions. During gelation of sodium alginate, Zn
2+ cations interact with carboxylate groups forming a crosslinked network of alginate chains. Ag
+ ion addition and concomitant gelation likely differ from those with Zn
2+ ions, thus causing changes in the properties of the gel network. The extent of crosslinking determines the density of the hydrogel that affects its swelling. It was shown that swelling can be used to determine the degree of crosslinking [
44]. When a microsphere is dispersed in a medium, a higher degree of crosslinking and a denser network structure result in less swelling and, as a result, lower S
w values. Compared to microspheres, those coated with chitosan (microcapsules) exhibit a higher degree of swelling. This can be attributed to the higher water uptake capabilities of chitosan [
45,
46]. The encapsulation efficiency, loading capacity, and swelling dynamics of microparticles emphasize the importance of Zn
2+ and Ag
+ ions and the incorporation of chitosan in modulating these properties.
The possible use of biopolymer microparticles imposes research on their release capacity in certain physicochemical conditions. The release profiles of Zn
2+ and Ag
+ ions from different types of alginate microparticles are presented in
Figure 6a,b. A set of release profiles exhibited a burst initial release followed by a slower release obeying the power law equation. It can be seen that the amount of cations released depends on the active agents and the presence of chitosan. The release patterns of Zn
2+ and Ag
+ ions heavily rely on the presence of chitosan which had a profound influence on the release rates.
All curves presented in
Figure 6 a,b can be described by the equation:
where f represents the fraction of released cations,
k is a constant characteristic of the active agent/polymer system that considers structural and geometrical aspects of the system, and the exponent
n characterizes the mechanism controlling the release of active agents from microparticles. The values of the release constants
k and the exponents
n are listed in
Table 4. The correlation coefficients ranged from 0.97 to 0.99.
Various mechanisms such as desorption from the surface, diffusion through the microparticle matrix and wall, and microparticle disintegration, dissolution, or erosion of the structure, or their combination, may be included in the release of active agents from microparticles. The most important release mechanisms of hydrophilic microparticles are swelling and dissolution/erosion at the microcapsule surface [
43]. When dispersed in deionized water, the hydrophilic polymer microcapsules swelled, thus influencing the release of cations from them. To identify the type of rate-controlling mechanism involved in cations release, a semi-empirical Korsmeyer–Peppas model was applied [
47]. According to Korsmeyer–Peppas, the release exponent
n can be characterized by three different mechanisms (Fickian diffusion, anomalous (non-Fickian diffusion), or Type II transport). Values of
n < 0.43 indicate that the release is controlled by classical Fickian diffusion,
n > 0.85 is controlled by Type II transport, involving swelling of the polymer and relaxation of the polymeric matrix, while values of
n between 0.43 and 0.85 show the anomalous transport kinetics determined by a combination of the two diffusion mechanisms and Type II transport. Lower
n values than 0.43 for all microparticles (
Table 4) indicated that the rate-controlling release mechanism involved is a classical Fickian diffusion. The results showed that changing the extent of crosslinking did not affect the release control mechanism.
The
k values pointed out remarkable differences in the release rate of Zn
2+ ions between microspheres and microcapsules. This can be ascribed to the coating of the microspheres with a polyelectrolyte layer and differences in the structure of the microparticles. In addition to the mechanical barrier and the smaller pores, chitosan can bind metal ions to amino (-NH
2) and to a lesser extent via hydroxyl (–OH) groups [
48]. A significantly lower proportion of released silver ions can be explained by slower diffusion through the microcapsule matrix and probably greater binding to chitosan than to zinc ions. A comparison of our results with data from the literature showed that the concentration of Zn
2+ and Ag
+ ions released from prepared microparticle formulations in deionized water is below the level of plant toxicity [
49].