2.1. Effective Diameter and Zeta Potential of Starch-Based Systems vs. Time
During thermal technological processes, the stability of starch is improved by its cross-linking, especially in an acidic environment and during high shear. Unfortunately, such a modification also has negative effects, e.g., it reduces the transparency and clarity of gruels and resistance to cold storage [
5,
6,
7,
8,
9,
10,
11,
12,
25,
26,
27,
28,
29]. Taking into account the gelatinization temperature for rice starch, three different temperatures were selected for testing: the temperature before the gelation point, the physiological temperature (useful for food and cosmetic products), and the temperature after the end of gelatinization.
In
Figure 1, the relationships of the effective diameter and the zeta potential as a function of time for starch dispersion in a 10
−3 M NaCl solution at three temperatures, 25 °C, 37 °C, and 70 °C, are presented. As was mentioned earlier, during gelatinization, firstly, the amorphous parts of the starch granule are hydrated, which induces swelling of the granules, leading to a distortion of the crystalline area. Secondly, the crystalline regions become more accessible to water. Thus, the size of starch granules increased with temperature increase from 25 °C to 70 °C (
Figure 1a).
The morphological changes associated with gelatinization are swelling and the rupture of the granular crystalline structure. At room temperature, a rapid increase in the effective diameter is visible within 30 min, while at 37 °C, the equilibrium state is reached faster, and the effective diameter values are more stable. After an hour at both temperatures, 25 °C and 37 °C, the diameters are noticeably more stable, and after 2 h, they are even similar. At 70 °C after 30 min, a monotonic increase in the diameter value was observed, which lasts up to 2 h of measurements and proves that the tested system at this temperature is the least stable. Analyzing the dependence of the zeta potential (
Figure 1b), there are also clear differences between the samples, both in terms of the value of the potential and the nature of changes during the measurements. The obtained dependencies of the zeta potential as a function of temperature may be a further indication that starch gelatinization involves a change of the ordered state from the crystalline state to the disordered state. The zeta potential describes the forces occurring in the system and is indirectly a parameter of stability.
Starch granules are held together by hydrogen bonds and interchain hydrophobic bonds. As the temperature increases, the main process may be the breaking of hydrogen bonds between poly-(1 → 4)-glucan chains in crystallites and subsequent hydrophobic bonds. During these processes occurring in starch granules, after breaking hydrogen bonds, the polar groups probably hide inside and the hydrophobic parts remain outside; so as the temperature increases, a decrease in zeta potential is noticeable (
Figure 1b). At temperatures of 37 °C and 70 °C, small negative zeta potential values were obtained, while at room temperature, these values are positive and the highest, which may indirectly confirm this conclusion and also indicate better stability.
It is well known that the gelatinization process of starch is multi-stage, and its course strictly depends on the temperature. Typically, above the temperature of 50 °C, the hydrogen bonds between the amylose chains forming the crystalline fragments of the starch grain are broken. Water penetrates between them, creating new hydrogen bonds with released starch chains [
18,
19,
20]. The gelatinization temperature is the temperature above which the starch does not show a granular structure in an aqueous medium and gives a paste characterized by high viscosity. Large grains lose their structure at the beginning. On the other hand, small grains are more resistant, which results in a large range of gelatinization temperature. This is why particle size measurements are so important in starch studies.
As mentioned, the gelatinization temperature depends on the starch source and for rice starch, it is 65 degrees. Differences between rice varieties can be found in the ratio of amylose/amylopectin, internal ordering, and side chain length distribution. Rice starches have a better resistance to processing stress, are much more stable in time (very slow retrogradation), and have smooth gels with low structure. Starches with 25–30% amylose and 70–75% amylopectin are called “normal” starches; starches with very high levels of amylopectin (98–99%) are named “waxy” starches; and a third group contains starches with high amylose content (50–70%) and has no specific name [
19]. The ratio of amylose to amylopectin in starch profoundly impacts its physicochemical properties or starch-based industrial products’ features, which, in turn, affect their functionality and potential applications. Higher amylose content implies increased film strength, while the presence of highly branched amylopectin leads to the formation of films with poor mechanical strength [
19].
Remylgel belongs to waxy starches with a very high content of amylopectin. It is most probable that the branched chain of amylopectin is directed into the air in a gel film. Changing the parameters of starch during the gelification process (e.g., type of modification solution, temperature, time of modification), the wettability properties of the starch surface, and also the possibility of starch application, can be substantially changed. During gelatinization, the presence of a large amount of water is forming, and then the layered structure of the starch grains disappears and turns into bubbles. As a result of water entering the vesicles, amylose is completely dissolved, amylopectin swells more strongly, and peptization occurs [
18,
19,
20,
21,
22,
23,
24,
25]. These changes can also be seen in the example of measurements of size diameter and values of electrokinetic potential. For starch dispersion in a NaCl solution at 37 °C, slight fluctuations of this parameter were observed during 2 h of measurements. At 70 °C after 1 h, the zeta potential remained at the same level, about −7.0 mV. However, such a low potential does not guarantee the stability of the system; hence, large fluctuations of the effective diameter at this temperature are visible (
Figure 1). At room temperature, higher potential values were noted, which resulted in more stable values of the effective diameter of starch dispersion in the NaCl solution. On this basis, a conclusion can be drawn about the correlation of these two parameters.
Due to the potential medical and pharmaceutical applications, further studies were carried out for an analogous dispersion of starch with the addition of a phospholipid (PC). As already mentioned, the phospholipid increases the biocompatibility of such a system due to the fact that it is one of the main components of cell membranes. The obtained dependencies of the effective diameter and zeta potential as a function of time for the starch/phospholipid dispersions at three temperatures are presented in
Figure 2. At room temperature and 70° during the first hour, large fluctuations are visible; however, after 1 h, in both cases, a monotonic decrease in the value of the effective diameter for up to 2 h of measurements is observable.
However, at a physiological temperature, the starch/PC dispersion in a 10
−3 M NaCl solution is the most stable. The diameter values remained almost all the time at the same level of about 990 nm.
Figure 2b shows the relationship of the zeta potential as a function of time. At room temperature and 37 °C, only negative values of the electrokinetic potential were recorded, unlike the measurements for the dispersion at 70 °C, which are only positive. This is directly related to the changes in starch structure below and above temperature gelatinization, as previously described in detail. The hydrophilic–hydrophobic character of starches depends on temperature, as well as their substitution type and starch pretreatment. At room temperature, the zeta potential values ranged from −29 mV to −9.4 mV, initially showing a decrease and then a monotonic increase. The reverse trend of changes was noted for the dispersion at 37 °C. The values of zeta potentials for room and physiological temperatures after 2 h are similar. On the other hand, the values of the electrokinetic potential of the starch/PC dispersion at 70 °C range from 6.2 mV to 9.7 mV, and fluctuations in time are visible. Such a low potential of approx. 10 mV does not guarantee the stability of the system; hence, large fluctuations of the effective diameter at this temperature are visible in
Figure 2a.
In the next stage of the research, measurements were carried out for the starch/lysozyme dispersion in a NaCl solution. The obtained effective diameter versus time relationships are shown in
Figure 3a. The stability of dispersions depends on several factors, e.g., the type and concentration of the emulsifier used and its surface activity or adsorption rate at the interface. A lysozyme is a protein, and due to its surface properties, it can be used to create and stabilize different kinds of dispersions. Regarding emulsions, it is known that a protein film is formed around the oil droplets, which has a positive charge and prevents coalescence or flocculation. It has a high emulsifying capacity, especially after unfolding [
15,
16,
17,
18,
19,
20]. A rapid increase in the effective diameter is visible within 5–30 min and then a gradual decrease during 2 h at 25 °C. For the dispersion prepared at the physiological temperature (about 37 °C), nearly a double increase in diameter was observed during the first hour. The further course of the curve for 37 °C looks like a mirror image of the dependence obtained for the dispersion at 25 °C (an increase in the effective diameter was noted in the 60th minute, and then there was a decrease at 2 h in the opposite trend for physiological temperature).
At a temperature of 70 °C, a rapid decrease in the effective diameter is visible in the first 15 min, followed by a gradual increase. The obtained values of the zeta electrokinetic potential of the starch/lysozyme dispersion in the NaCl solution are shown in
Figure 3b. It is easy to see that the course of the curves at 25 °C and 37 °C is very similar, but the electrokinetic potential values differ primarily in sign. The electrokinetic potential values at room temperature range from −23.4 mV to −18.0 mV. The positive charge from the protein film is noticeable at the physiological temperature. At this temperature, positive zeta potential values were obtained. This behavior may be related indirectly to the mechanism proposed lately [
22]. The authors stated that the rearrangement of starch chains during heating, especially in the excess of water, leads to the strengthening of bonds between amylose and amylopectin, increasing starch granule stability, which can inhibit enzymatic hydrolysis. Moreover, this process can lead to the leaching of amylose chains from amorphous regions of starch granules, which probably reinforces their crystalline structure. The amorphous regions of semicrystalline starch granules represented regions most susceptible to the initial water absorption. The hydration of starch granules leads to increased mobility, especially in the amorphous regions. During progress in heating/hydration, the initially weaker or imperfect crystallites successively disappear, whereas the other ones become more perfect upon fusion and recrystallization.
At a temperature of 70 °C, within 15 min from the creation of the dispersion, a decrease in potential from −7.9 mV to −10.7 mV was noted, and then the potential remained at a constant level and reached a value of approx. −5.5 mV. Such a low potential does not guarantee the stability of the system; hence, large fluctuations of the effective diameter for this dispersion are visible in
Figure 3a. In the case of the
n-tetradecane/starch emulsion, fluctuations in the diameter value are visible at all temperatures, and the largest was at 37 °C; therefore, for better visibility, some results have been reduced twice (
Figure 4a). On this basis, it can be concluded that the analogous starch dispersions are more stable than the tested
n-tetradecane/starch emulsions.
It is known that an O/W emulsion or its powdered form (dry emulsion) can be a carrier of oil-soluble compounds with health-promoting properties or biological activity (e.g., polyunsaturated fatty acids, sterols, vitamins, or antioxidants). A properly selected recipe and technology for the production of emulsion (dispersion) means that the structure of the particles must ensure the long-term stability of biologically active substances. For a high efficiency of such systems, it is necessary to disperse the oil phase to particles with a diameter of less than 1 mm using an appropriate homogenization technique, as the particle size also affects the stability of the emulsions produced [
15,
16,
17,
18,
19,
20].
The most important difference between proteins and other emulsifiers used is the size. Proteins having a high molecular weight diffuse into the interface much more slowly than a non-protein emulsifier. When the protein reaches the phase boundary, the chains unfold, and fragments are divided between the phases, which takes time. In the case of protein, to achieve the required value of interfacial tension to stabilize the emulsion, such a process may take up to several hours. Protein–polysaccharide combinations show very good stabilizing and emulsifying properties. This makes it possible to replace other low-molecular synthetic emulsifiers, which is advantageous for nutritional and pro-health reasons [
30,
31,
32,
33,
34,
35,
36]. Therefore, the size will be particularly relevant for samples with lysozymes. In addition to the size and changes in the diameter of the tested systems, for a more complete characterization, the electrokinetic potential dependencies should also be considered. The most stable potential is visible at room temperature in the range from −20.8 mV to −18 mV. Despite quite stable values of the zeta potential, which usually guarantee the stability of the system (
Figure 4b), the diameters are not stable (
Figure 4a). This may be due to incomplete dispersion of the fat phase at this temperature. The homogeneity of the dispersion of the lipid phase should increase with increasing temperature. At a temperature of 37 °C, after the initial decrease in the zeta potential in 30 min to the value of −21.4 mV, an increase in the potential to the value of about 17.4 mV is visible. The greatest fluctuations of the potential over time were recorded at a temperature of 70 °C in a range from 10.6 mV to −4.5 mV, and the course of the curve resembles a sine wave (
Figure 4b).
It is well known that changes to temperature involved in food processing and products can also influence emulsion stability. For example, this type of research has been carried out for phospholipids, and the authors [
24] have investigated the effect of the combination of starch and PC on the freeze–thaw stability of an O/W emulsion. The adsorption behavior, rheological properties, and mechanism of the improved stability of the starch–PC complex at the oil–water interface were discussed. The binding energy of the starch–PC complex was significantly lower than that of PC molecules, suggesting that the complex was relatively stable, and their changes were consistent with changes in electrostatic energy, indicating that such energy played a major role in the formation of the starch–PC complex. There were intermolecular hydrogen bonds and hydrophobic interactions in the starch–PC complex, while only hydrophobic interactions existed in the PC molecules [
24].
2.2. Starch System without n-Tetradecane Film
One of the aspects of this research, apart from stability, was to investigate how the substrate and the modification of the starch layer will affect its wettability depending on the starch preparation temperature. The changes in bulk properties are usually seen in the surface properties of the starch. The parameters of wettability of the starch surface obtained also suggest topographical differences, as was concluded in our previous papers [
26,
27]. First, tests were carried out without
n-tetradecane, and then, based on tests with
n-tetradecane, the effect of starch hydrophobization was analyzed.
Figure 5 shows the average values of the contact angle of starch plates without
n-tetradecane film at three different temperatures. Liquids differing in polarity were used for wettability measurements, from highly polar water, through polar formamide, to non-polar diiodomethane. Natural starches have no affinity for hydrophobic substances, fats, or oils due to their hydrophilic nature. Specialized preparations consisting of two parts—hydrophilic and hydrophobic—are produced, having an affinity for both oil and water, so they can form stable oil-in-water emulsions. Starch with an additional layer can fulfill an analogous role, e.g., reduce the cholesterol content, and emulsifying substances make it possible to maintain a uniform structure in such products [
15,
16,
17,
18,
19,
20].
The methodology used for contact angle measurements also indirectly provides information about the changes in the structure of the starch layer before and after modification and the kind (or even strength) of forces between material molecules. The attractive forces between molecules that cannot be explained by ionic or covalent interactions can be caused by polar moments within molecules. During gelatinization, surface flatting can also be observed. Definitely, the highest average values of the contact angle at room temperature (
Figure 5a) are noticeable for water. With the reduction in the polarity of the tested liquid, the hysteresis of the angle decreases because the differences between the values of the contact angles are small. For water, the hysteresis value is about 20°, which confirms the great sensitivity of starch to water. Starch absorbs water at any temperature, so even after a few seconds, its surface is completely different after placing a drop of water, while for the diiodomethane angle, hysteresis is only 2°. In the case of formamide and diiodomethane, the values of the contact angles are comparable.
It is well known that the contact angle depends on composition and temperature, as well as on the roughness of the film surface [
18,
19,
20]. Determined by the rate of water drop absorption, starch films can be divided into two main groups (on the basis of contact angle values below 90° and over 90°). At the beginning of the experiment, starch surfaces prepared at 25 °C and 37 °C showed contact angles near 90°; after hydrophobization, contact angles were usually higher than 90°. Conversely, after PC or lysozyme modification, the contact angles were lower. The classification of starches according to the rate of water drop absorption gives temperature dependence. In our previous papers, the fastest rate of water drop absorption (the highest decrease in contact angle, about 0.1 degree/s) was observed for starch prepared at 70 °C after gelatinization [
18,
19,
20]. A fast rate of water drop absorption was found for the water-soluble starches. Untreated starch at 70 °C showed a smaller contact angle than that at room and physiological temperatures. A reason might be the different retrogradation rates of the starch–water systems during film formation. Starch at room temperature before gelatinization shows the highest retrogradation rate of these untreated starches; therefore, the film is less hydrophilic and the contact angle increased [
26,
27].
A comparison of the average values of the contact angles of formamide and diiodomethane for starch-coated plates before hydrophobization is also shown in
Figure 5. For formamide and diiodomethane, the angle values are very close to each other. The hysteresis value of the angle decreases with the decrease in the polarity of the tested liquids (the highest is for water and the lowest is for diiodomethane). Analyzing the above graphs, it can be concluded that the starch preparation temperature has practically no effect on the values of the contact angles of formamide and diiodomethane, while the influence is much greater for the contact angles of water. For the highest tested temperature, there was a decrease in the advancing angle of water by about 15 degrees. In addition, at each of the three temperatures, the angle hysteresis value decreases as the polarity of the liquid decreases.
2.3. Starch System with n-Tetradecane Film
For the systems with the addition of
n-tetradecane, the effect of starch hydrophobization was analyzed. A comparison of the average values of the contact angle of water, formamide, and diiodomethane for starch-coated plates with
n-tetradecane film is shown in
Figure 6. At maximal temperature, both the average value of the contact angle and the hysteresis value depend on the polarity of the liquids used. The more polar the liquid is, the greater the contact angle and hysteresis. In the case of hysteresis, this is caused by differences between the values of the advancing and receding angles. At 70 °C, the hysteresis values of the water and formamide angles are very similar, approx. 10°, and for diiodomethane, they are half as much (about 5°).
As already mentioned, starch in food products also acts as a fat substitute. In low-fat products, when the degree of fat exchange exceeds 70%, the continuous phase of the product changes into an oil-in-water emulsion, changing the rheological properties and corresponding to condensed emulsions. The replacement of fat comes down to the introduction of water in combination with structure-forming additives in the form of hydrocolloids. The addition of starch has a significant impact on the mechanical and rheological properties of products, thanks to the ability of starch to create stable structures in the presence of water and under the influence of temperature. That is why physicochemical studies of oil/water emulsions with starch, as well as studies of the wettability of starch films, before and after hydrophobization are so important from the application point of view. At 37 °C, the lowest value of the contact angle was obtained for water and the highest for diiodomethane. On the other hand, regarding hysteresis, the highest value is obtained for formamide of approx. 13°, while water and diiodomethane were practically at the same level and amounted to approx. 7°. The chemical nature of the probe liquid, the size of its molecules, and the kind of interactions determine the surface penetration. The differences in the values of the contact angles and hysteresis manifest the strength of the solid/liquid interfacial interactions.
Lately, to prove such a comment, the authors’ [
47] independent gradient model was created to illustrate non-covalent interactions between starch and PC. For all studies of the the starch–PC complexes, the oil–water interfacial tension decreased quickly, indicating the adsorption of the complex onto the oil–water interface. There may be a formation of an interfacial layer in the starch–PC complex due to interactions between starch and PC, leading to a decrease in interfacial tension greater than that observed in the presence of single emulsifiers. Starch adsorbed slowly to oil surfaces due to its highly branched macromolecular structure and steric contribution and also formed a more extended organization at the interface and, as a result, a relatively thick layer. It is well known that in the case of water and formamide, the interactions are both dispersive and polar in nature, but for apolar diiodomethane, they are practically only dispersive.
Decreasing contact angles of water indicates that during contact between water and the starch surface, its hydrophilicity increases. The largest hysteresis of water contact angles demonstrates that a water droplet penetrates the deepest into the layer structure and depends on surface preparation temperature. Emulsions prepared with the starch–PC complex had a relatively strong electrostatic repulsion that attenuated the oil droplets merging. No creaming and aggregates were observed in the emulsions prepared with starch–PC complexes, indicating that the low and moderate addition of starch helped stabilize PC-based emulsion during the freeze–thaw treatment. The improved stability may be related to the thickness and density of the interfacial layer formed by the complex. A number of studies supported the general idea that emulsifiers, which form a thick interfacial layer, are able to stabilize emulsions [
47]. Comparing the average values of the contact angle of the tested liquids on the surface of starch-coated plates with and without the
n-alkane film, it can be concluded that in this case, the effect of hydrophobization is also visible, mostly at physiological temperatures (
Figure 6b).
2.4. Starch/Phosphatidylcholine Systems without n-Tetradecane Film
A comparison of the average values of the contact angles of water, formamide, and diiodomethane for starch/PC platelets without
n-tetradecane film at three different temperatures is shown in
Figure 7. As was mentioned earlier, phosphatidylcholine is used, e.g., in pharmaceutical technology due to its unique surface-active properties, and it acts as an emulsifier and a modifier of rheological properties, improving the stability and the consistency of dispersion. Phosphatidylcholine is non-toxic and biodegradable, so it can be used in parenteral nutrition preparations, such as dietary supplements, which lower the concentration of triglycerides and cholesterol in the blood. In addition to drugs, it can be used in the form of ointments, creams, emulsions, or suspensions. It is also important that as a result of combining starch with a phospholipid, the biocompatibility increases because these connections are similar in structure to biological membranes, and they do not cause sensitization or allergic reactions.
After PC treatment, the changes of advancing contact angles are visible, and the effect grows with the temperature increase. Both polar PC groups and patches of native starch are accessible for water during contact with liquid. Hence, the water contact angle can decrease. Due to the polar nature of water, its molecules exhibit a strong tendency to form hydrogen bonding. Therefore, the structural rearrangement of the PC molecules on the starch surface can occur, and the highest increase in the polarity of the starch surface after PC modification is observed. Wang and co-workers proved that the starch–PC complex at weight ratios of 3:7 and 5:5 remarkably improved the freeze–thaw stability of emulsions (no creaming process and creation of aggregates) and stated that it may be related to a thick and dense interfacial layer [
24].
At room temperature (
Figure 7a), the highest value of the contact angle was obtained for the non-polar liquid—diiodomethane and the lowest value was for formamide. In the case of non-polar diiodomethane, the value of the contact angle increased by about 20° compared to starch surfaces. The opposite situation is visible in the case of water, i.e., the average value of the angle is lower by more than half. The smallest value of the angle hysteresis was obtained for formamide, while for water and diiodomethane, the values were practically the same. The plates are definitely more hydrophilic compared to the basic ones. This confirms that a small modification can lead to obtaining systems with completely different properties, and the measurements of contact angles are very sensitive and, therefore, extremely useful parameters in determining such changes in a relatively simple and economical way. The hydrophilization of the starch surface after PC modification is caused by the rearrangement of the hydrophobic monolayer into layers with the polar groups of phospholipid heads exposed toward water drop.
For starch/PC plates without
n-tetradecane film (
Figure 7b), at a starch preparation temperature of 37 °C, the graph looks analogous to that for room temperature (
Figure 7a). A similar situation also occurs in the case of the highest temperature (
Figure 7c), except that the highest value of the contact angle was recorded for water, and not, as in the case of two lower temperatures, for diiodomethane. After exceeding gelatinization, the temperature is completely different, and thus the phospholipid film on the starch surface shows a dissimilar character, which translates to the measured contact angles. The influence of PC is visible, especially for the most polar water and apolar diiodomethane, whose average values of the contact angle changed radically compared to the values of angles measured on plates covered with a layer of starch without modification. Other less sensitive methods would not show these changes, which, once again, confirm the high usefulness of wettability tests. Attractive interactions between starch and PC can cause strong complex formation and, as a result, film condensation and smoothing. Indeed, the low values of angle hysteresis may indicate surface smoothing. During temperature increases the homogeneity of the starch layer increases because the degree of gelatinization grows. An analogous conclusion was also drawn from the decreased values of the roughness parameters in our previous experiment for the same type of starch [
26,
27].
2.6. Comparison of the Hysteresis Angle of Test Liquids for the Starch/Phosphatidylcholine System before and after Hydrophobization vs. Temperature
In the next stage of this research, the hysteresis of water angles on the surface of starch with phosphatidylcholine (S/PC) with and without
n-tetradecane film was compared, depending on the starch preparation temperature. At room temperature (
Figure 9), the hysteresis values of the water angles for the S/PC plates without and with
n-tetradecane film are practically the same and amount to about 13.5°. At a physiological temperature, the hysteresis value for the S/PC plate after hydrophobization is definitely higher (by several degrees) than before hydrophobization.
The increase in attractive interactions between components causes the formation of more and more tightly packed monolayers characterized by lower values of the roughness parameters. Therefore, such condensed films are less permeable for the probe liquids used for the contact angle measurements. These suggestions have been observed in our previous research based on FTIR analyses [
26,
27]. Under the influence of modification with bioactive substances or by temperature increase, a change in the spectra of starch is possible. On the other hand, the authors [
23] described that the inclusion complexes were formed by hydrophobic interactions between the alkyl chain of phosphatidylcholine and the debranched starch helix cavity. The complexes possessed a mass fractal structure, and a semicrystalline structure formed. After complexation, the stability of phosphatidylcholine was significantly improved. Additionally, this study revealed that debranched starch can be used as an effective carrier of phosphatidylcholine for the purpose of improving its stability [
23].
At the highest temperature, the hysteresis value of the water angles for the tested plates without
n-tetradecane film is higher than for the plates with the film. The obtained hysteresis values of the formamide angles for the starch/PC plates without and with
n-tetradecane film, depending on the starch preparation temperature, are shown in
Figure 9b. For PC, modified starch OH stretching and skeletal mode were slightly shifted compared to the native starch. Changes in the intensity of specific bands are found to be the major spectral ones during gelation. Gelatinization is primarily a hydration process, and chain conformation and helicity change when crystallinity and molecular orientation are lost. The signal around 1000 cm
−1 is related to the intermolecular hydrogen bonding of hydroxyl groups or the plasticizing effect of water [
26,
27].
At each of the tested temperatures, the hysteresis values of contact angle for S/PC surfaces after hydrophobization are higher than before. The smallest difference in the angle values was obtained at the physiological temperature, while at 70 °C, the hysteresis value of the formamide angle for such surface with n-tetradecane film is as much as three times higher than for the same plate before hydrophobization.
Completely different relations were obtained in the case of an apolar liquid (
Figure 9c). The hysteresis values of the diiodomethane angles for S/PC plates without
n-tetradecane film are much higher than for the same plates with the film; for example, at room temperature, the hysteresis values after hydrophobization (approx. 3°) are almost five times lower than before (approx. 15°). On this basis, it can be concluded that the change in starch temperature and the presence of
n-tetradecane significantly affect the nature of the tested surface, and furthermore, a lower hysteresis value usually indicates smaller surface heterogeneity and, as a result better system reproducibility. Some other factors influence the surface parameters, such as the presence of unsaturated bonds in molecules and the phase state in which investigated films exist; therefore, FTIR spectra can be useful [
26,
27].
2.7. Starch/Lysozyme Systems without n-Tetradecane Film
As was mentioned earlier, the condensed films are less permeable for the probe liquids used for the contact angle measurements. These suggestions can be observed as an effect of temperature. During gelatinization, the intensity of some bands increases, and new peaks can appear; hence, hydrophilic/hydrophobic changes can be observed from the FTIR spectra differences (
Figure 10). During the gelatinization process, the most hydrophobic parts of the starch chain are directed into the air. However, steric limitations cause some polar groups to be present on the gel surface. The starch gel surface tends to reach maximal hydrophobic character with polar domains created by the functional glucose groups. It is most probable that the branched chain of amylopectin is directed into the air in a gel film. These are the primary results in the preparation of starch products of special properties, which can influence their solubility or polydispersity in aqueous media [
47,
48,
49,
50,
51].
Starch is similar to other polysaccharides that absorb in the region 1200–800 cm
−1. In this region, the average penetration depth is about 2 μm [
26,
27]. Because this value can be smaller than the average size of studied starch granules (1–3 μm), the acquired FTIR spectra are probably representative of only the external part of the starch granules. However, such spectra should be adequate for the starch film and compatible with the profilometer results. FTIR analysis of the untreated starch at three different temperatures is shown in
Figure 10a–c. All spectra show that the absorption bands in the 900–1300 cm
−1 region are sensitive to the gelation of starch, which mainly result from the CO and CC vibrational modes being highly coupled. As the absorptions in this region arise largely from C–O stretchings of the ring, linkages (C–O–C), and COH groups, the positions of these bands are similar in all carbohydrates. The native starch surface shows a typical pattern of Raman bands, i.e., skeletal vibrations below 800 cm
−1, and the glycosidic linkage assigned to the band at about 940 cm
−1. During the temperature increases, the breaking of hydrogen bonds between the chains in the crystallites and hydrophobic bonds may become a major event. Thus, the intensity of some bands changes (
Figure 10b,c). The signal around 1000 cm
−1 is related to the intermolecular hydrogen bonding of hydroxyl groups or the plasticizing effect of water. Absorbance at 1020 cm
−1 is assigned to the vibration of C–O–H deformation and is related to changes in the amorphous and crystalline parts of the starch granule. The bands in the 1015–1025 cm
−1 and 1040–1050 cm
−1 regions are of particular interest because they are associated with the amorphous and crystalline structures of starch, and their ratio can estimate the extent of gelatinization [
26,
27].
The absorption bands at 1150, 1080, and 1017 cm
−1 show a tendency to decrease in the bandwidth during gelation. Their narrowing can be interpreted as an evolution to a more uniform state of the amorphous phase (
Figure 10a–c). The bands at 1080 cm
−1 show the greatest shifts assigned to C–O and C–C stretching and C–C–O bending. During the process of starch gelatinization, the Raman bands are shifted to lower wavenumbers for the CH deformation and the skeletal and CH stretching modes, but for COH deformation, they shift to higher wavenumbers. At room temperature, the Lys-modified starches show differences compared to the native starch (
Figure 10d), but at higher temperatures, the lysozyme effect is less visible (
Figure 10e) because growing temperature affects the changes occurring during the gelatinization process in the system with and without lysozymes. This process is decisive, and biological additives affect the spectrum to a lesser extent. High temperature causes the quantitative denaturation of a native lysozyme within 20 min. The starch surface with the increasing temperature of preparation becomes more hydrophilic. The contact angles decrease with the temperature of starch preparation, which also increases the hydrophilic character of surfaces. In the case of water, the layer structure changes also result in large contact angle hysteresis. The wettability test together with FTIR analysis and optical profilometry are suitable and powerful methods to characterize the morphological and molecular properties of starch and modified starch.
Accurate calculation of the area of the 1017–1022 cm
−1 and 1044–1047 cm
−1 regions and their ratios is commonly used in the literature [
26,
27] to estimate the extent of gelatinization. A lysozyme is an antibacterial substrate belonging to a large group of proteins and glycoside hydrolases. There are enzymes that damage bacterial cell walls by catalyzing the hydrolysis process of 1,4-beta-linkages between N-acetylmuramic acid and N-acetyl-D-glucosamine residues in a peptidoglycan and also between N-acetyl-D-glucosamine residues in chitodextrins. A lysozyme with these functions is recognized as part of the innate immune system, a natural form of protection against Gram-positive pathogens, like
Bacillus and
Streptococcus [
16,
17,
18]. Therefore, covering starch films with lysozymes or their addition to dispersion systems will result in additional desirable properties both in the food and pharmaceutical industries. On the other hand, the immobilization of lysozymes on solid supports has lately shown positive results, as demonstrated by the increased stability and extended half-life of the enzyme in the research by Anastas and co-workers [
5]. Furthermore, the immobilization of the lysozyme improves the ability of the lysozyme to target not only Gram-positive bacteria but also Gram-negative bacteria. The large effect of the lysozyme is noticeable, similar to the case of starch modification with a phospholipid, at 37 °C (
Figure 10e). This may be related to conformational changes that occur in the protein structure on the surface of partially gelatinized starch.
A comparison of the average values of the contact angle of water, formamide, and diiodomethane for plates coated with starch and a lysozyme without
n-tetradecane film is shown in
Figure 11. At room temperature, the value of the contact angle increases with increasing polarity of the liquid used; the highest values were obtained for water, and the lowest for diiodomethane. However, for hysteresis, the relationship was not so clear, and the values obtained are as follows. For water, about 10°, for formamide, as much as 17°, and for diiodomethane, only 6°. Applying an additional layer (lysozyme) to the starch-coated plates increased the contact angle values by several degrees in the case of formamide and diiodomethane, while the average value of the water contact angle decreased by several degrees, which may indirectly indicate an increase in surface hydrophilicity.
At a physiological temperature (
Figure 11b), there is an analogy to measurements at room temperature (
Figure 11a). It is easy to see that the values of the contact angles change in a similar way, i.e., the more polar the liquid is, the higher the values of the contact angles (
Figure 11a). Additionally, the hysteresis value for polar liquids is practically at the same level of about 12°, while for non-polar diiodomethane, it is larger and amounts to about 16°. At a temperature of 70 °C (
Figure 11c), the average values of the contact angles did not change compared to the measurements at lower temperatures (
Figure 11a,b). Noticeable changes are seen in the hysteresis values, which decrease as the polarity of the liquid used decreases. The greatest difference between the advancing and receding angles is for water, and the smallest is for diiodomethane. The starch preparation temperature did not affect the contact angle values in these systems, while the application of protein on the starch increased the contact angles.
2.9. Comparison of the Hysteresis Angle of Test Liquids for the Starch/Lysozyme System before and after Hydrophobization vs. Temperature
In
Figure 13, the hysteresis of water, formamide, and diiodomethane angles on the S/Lys surface with and without
n-tetradecane film was compared depending on the starch preparation temperature. In
Figure 13, at 25 °C and 70 °C, the hysteresis values of the water contact angle for S/Lys plates with
n-tetradecane film are very similar and amount to about 10°. At physiological temperature, the effect of
n-tetradecane is most noticeable. For room and physiological temperature, the hysteresis values are twice as high for the S/Lys plates without
n-alkane film compared to the same plates with the film.
At a temperature of 70 °C, the effect of hydrophobization is more visible; the hysteresis value before hydrophobization is 9°, and after hydrophobization, it is 12°. In addition, it can also be seen that the hysteresis values for the S/Lys plates without
n-tetradecane film decrease with increasing temperature. This can be explained by the easier spreading of the starch solution at higher temperatures and the concomitant decreasing film thickness. The hysteresis of diiodomethane angles of the starch/lysozyme system before and after hydrophobization is shown in
Figure 13c, and these are the smallest hysteresis values that we obtained. As the temperature increases, the hysteresis value for the S/Lys plates with
n-tetradecane film increases, i.e., the effect of hydrophobization also increases. This can be explained by the fact that large surface changes occur under the influence of
n-tetradecane and temperature, which are visible on the basis of contact angle measurements. As the temperature increases, the breaking of hydrogen bonds between the poly-(1 → 4)-glucan chains in the crystallites and hydrophobic bonds may become a major event. The loss of crystallinity may be considered a manifestation of starch gelatinization.
Another currently explored novel application of starch is the immobilization of enzymes, proteins, or drugs to improve the catalytic activity of enzymes used in food technology or to create more efficient drug delivery systems [
19]. The research carried out strictly fits into this trend of potential applications. A detailed description of topographic changes was presented in our previous works [
26,
27]. The roughness and topography of the starch surface were investigated using an optical profilometer (Contour GT-K1, Veeco) measuring topography with high accuracy from a subnanometer up to 10 mm in size. We have performed such measurements in three different sites for glass plates covered with native starch and its modification. Below, we present some sample surfaces (
Figure 14).
The obtained images of the starch surface by profilometer show topographical differences between the native starch surface and that modified by a biological solution. For example, the height distribution shows that the starch surface is covered mostly by patches. The hydrophilization of the starch surface after PC modification is caused by the rearrangement of the hydrophobic monolayer into bilayer patches with the head polar groups exposed toward water drop. Attractive interactions between starch and PC may cause complex formation. This strong association can cause film condensation and smoothing. Indeed, the monolayer of PC on the starch makes the surface smoother. Reduced values of all roughness parameters were obtained compared to the native starch surface; although, in order to explain changes in surface roughness, the type and size of interactions between starch molecules and the additional layer should be taken into account. Due to the polar nature of water, its molecules have a strong tendency to form hydrogen bonds. Therefore, there may be a structural rearrangement of PC or Lys molecules on the starch surface and an increase in the polarity of the starch surface after its modification. This effect decreases as the temperature increases. On the other hand, the lysozyme reduces the hydrophobic nature of the starch surface.
In both cases, during temperature increase, the homogeneity of the starch layer increases because the degree of gelatinization grows. Moreover, one can also find some correlations between the changes in surface roughness and the values of contact angles measured on native and modified starch surfaces. The increase in attractive interactions between both components causes the formation of more and more tightly packed monolayers characterized by lower values of the roughness parameters. Therefore, such condensed films are less permeable for the probe liquids used for the contact angle measurements. The chemical nature of the probe liquid, the size of its molecules, and the kind of interactions determine the surface penetration. It is clear that the differences in the values of the contact angles and hysteresis manifest the strength of the solid/liquid interfacial interactions. It is obviously known that the contact angle measured on such surfaces is of macroscopic quantity, which is, in fact, an averaged (apparent) value of the microscopic contact angles. The reproducibility of the contact angle values and the topography images enable full surface characterization.