3.1 Determination of EE and EC
As shown in Fig. 1, with the addition of FFVPF in the system increasing from 2.5 mg to 10 mg, EE of FFVPF in CS-TPP NPs increased first and then decreased. When the addition levels of short peptides were 5 mg and 7.5 mg, EE reached 94.10 ± 0.79% and 94.58 ± 0.23%, respectively, and there was no significant difference between them (P > 0.05). CS-TPP composite peptide-loaded NPs with EE higher than 94% were obtained. In the commercialization of food, high encapsulation rate also means lower transportation cost of functional factors [20]. The increasing peptide content makes EE increase continuously, in accordance with previous studies [21, 22]. The electrostatic interaction between polypeptide and CS-TPP carrier may lead to high EE. With the increase of polypeptide content, the LE is higher, which is caused by the increase of the ratio of polypeptide to carrier in NPs. Subsequently, due to the limitation of the loading capacity of NPs, the chemical potential of drug diffusion to the solution increased, and the increase rate of LE gradually tended to smooth-out, which was similar to the experimental results of Hosseini et al. [23].
3.2 Determination of particle size, zeta potential and PDI
Table 1 summarizes the effects of FFVPF addition on the particle size and PDI of CS-TPP NPs. The size of NPs affects the biocompatibility and activity. NPs with a small size are easier to be taken up by the cells, so they can function efficiently [24]. The NPs with the size of < (smaller than) 200 nm are difficultly filtered by spleen, while those > (larger than) 300 nm can be easily captured by phagocytic cells [25, 26]. Accordingly, the small size of the NPs obtained in this study may lead to a longer circulation. As the core content increased from 2.5 mg to 10 mg, the particle size gradually decreased from 175.67 ± 1.36 nm to 146.33 ± 3.59 nm. The causes of this phenomenon are as follows: with the increase of the amount of core material, the relative concentration of CS in the wall material decreases, and the number of - NH3+ on the surface of NPs decreases, which may lead to the weakening of intramolecular repulsion force, so as to reduce the particle size of generated NPs [27]. In particular, the particle size of blank NPs is smaller than that of all NPs loaded with FFVPF, which was similar to the experimental results of embedding eugenol essential oil by Hasheminejad et al. [28], which is possibly due to the surface adsorption.
The suitable NPs have uniform particle size distribution [29]. PDI was used to characterize the uniformity of particle size in the system. A larger PDI value represents a large difference in material size and wide particle size distribution in the system. Generally, if the PDI is less than 0.3, it can be considered that the particle size distribution of the system is narrow. The PDI of blank NPs and peptide-loaded NPs measured by DLS ranged from 0.2 to 0.25, showing a suitable and narrow particle size distribution (PDI < 0.3), which confirmed the formation of homogeneous and monodisperse NPs and peptide-loaded NPs.
Zeta potential is an important index of aqueous nanoparticle systems. For NPs stabilized by electrostatic interaction, the absolute value of zeta potential greater than 30 mV is a necessary condition for the stability of the system [30]. The poor surface charge might cause some problems, such as aggregation and lower peptide absorption into NP. The changes of zeta potential with the addition of short peptide FFVPF are shown in Table 1. CS-TPP NPs have strong positive charge, and the zeta potential values range from + 33 mV to + 36 mV, which are greater than 30 mV, indicating that the system is sufficiently stable. Zeta potential decreased with the increase of FFVPF addition. The results obtained by Zetasizer revealed that, due to the presence of amine groups on the surface of CS NPs, the surface charge is positive. The adsorption of peptides on the particles will reduce the surface positive charge of the cationic chitosan molecules, resulting in a decrease in Zeta potential. Therefore, CS-TPP is suitable as a peptide delivery system. The addition amount of FFVPF was set to 5 mg in the following experiments.
3.3 Phisyochemical characterization of CS-TPP NPs
3.3.1 FTIR analysis results
Fig. 2A indicates the FTIR spectra of CS, FFVPF, CS-TPP blank NPs and CS-TPP FFVPF NPs. The NPs added with 5 mg FFVPF were selected for characterization based on their high encapsulation efficiency, good particle size and zeta potential. Interaction of FFVPF with CS-TPP NPs led to some structural changes in FTIR spectra. Also, FTIR spectra confirmed the interaction between peptides and synthetic NPs.
The strong broad peak at 3433.14 cm-1 in the CS spectrum is attributed to the hydrogen bond O-H stretching vibration. The peak value of C-O-C asymmetric tensile vibration is about 1100 cm-1. The absorption band at 1604.71 cm-1 is attributed to the N-H bending mode in the chitosan primary amine 10 (Fig. 2A(a). In CS-TPP blank NPs, the peak at 1654.85 cm-1 (C=O stretching vibration in amide I area) and the N-H bending vibration peak at 1604.71 cm-1 of amine I at 1604.71 cm-1 shifted to 1577.70 cm-1 and 1413.76 cm-1, respectively [31, 32]. Also, the peak at 1043.44 cm-1 indicates that the tripolyphosphate group of TPP is connected to the amine group of chitosan (Fig. 2A (b). CS is a cationic polysaccharide, its amino group is positively charged, while the phosphate group of TPP is negatively charged, and the two form NPs based on electrostatic interaction. The FTIR spectra of peptides and peptide-loaded CS NPs are shown in Fig. 2A (c-d). In previous studies, it has been determined that the peptide binds to the chitosan hydroxyl group through its carbonyl group and forms a carboxyl group [33]. The spectrum of peptide loaded CS-TPP NPs (Fig. 2A (c) shows some differences from CS-TPP NPs, which means the formation of peptide NPs complex. Compared with (b) and (c), except that the positions of O-H stretching vibration peaks are different at about 3400 cm-1, the number and position of peaks in the infrared spectrum of NPs loaded with short peptides have no significant change compared with blank NPs, and no new vibration peaks are generated, but at 1577.70 cm-1, 1413.76 cm-1 in the functional group area and 1043.44 cm-1, 1014.51 cm-1 in the fingerprint area The peak type at 649.98 cm-1 is similar and the peak intensity is enhanced, which means that the embedded short peptide does not produce new chemical groups in NPs, but increases the number of some existing groups. Therefore, the main force of CS-TPP NPs embedding short peptide FFVPF is hydrogen bond. The short peptide characterized by Fig. 2A (d) has a peak at 1670.28 cm-1, which belongs to the amide I band, and it has double peaks at 746.42 cm-1 and 700.13 cm-1 in the fingerprint area, which represents the phenylpropane in the peptide. The monosubstituted benzene ring on the amino acid R group, but these peaks did not appear in the NPs loaded with short peptides. The difference in infrared spectra between (c) and (d) indicates that the short peptides were successfully embedded in the NPs.
3.3.2 XRD measurements
XRD analysis can identify the crystalline phase of the substance, and judge that the substance belongs to an amorphous or crystalline structure. The characterization results of XRD are shown in Fig. 2B. The two peaks at 10.6° and 19.96° in CS (a) are the typical peaks of its crystal structure, while the short peptide FFVPF in Fig. 2B(b) shows two broad steamed bread-like peaks at 7.62° and 19.88°, indicating that it belongs to amorphous form. Comparing with (a) and (c), the peak of CS at 19.96° decreased after cross-linking with TPP. Both (c) and (d) showed sharp and narrow peaks, the XRD patterns of the samples showed sharp peaks at 2θ = 8.86, 17.8, 26.82, 30.96 and 36.04 angles (Fig. 2B(a), which characterized the crystalline properties of the NPs. CS-TPP NPs have strong reflection, corresponding to the crystal morphology. The crystallization peaks in CS-TPP FFVPF NPs increased (Fig. 2B (d), indicating a slight increase in the crystallization properties in NPs. This structural modification may be related to the intermolecular and/or intramolecular network structure of CS, cross-linked via TPP counterions [34].
3.3.3 TEM measurements
The TEM was utilized to assess the shape, size, and uniformity of the NPs. This monograph clearly shows that the nanoparticles were spherical in shape. Fig. 3 shows the spherical shape of FFVPF loaded CS-TPP NPs under TEM measurement which were approximately 100 to 200 nm. In this case, some NPs are clustered together in a compact structure. CS and TPP were aggregated under the interaction of surface groups to form new particles of constant size and rearrange to form a denser structure [35]. Fig. 3 (b-c) enlarges the scale to 500 nm and 200 nm respectively, the number of particles in the field of vision decreases, and it can be seen that the surface morphology of NPs is basically smooth with slight sharp corners. The NPs exhibited almost homogeneous morphology, which can be due to mild preparation conditions.
3.4 Nanoparticles stability
3.4.1 PH stability
Fig. 4 (a) shows the retention rate of FFVPF loaded CS-TPP NPs of stability testing under different pH conditions. In this chart, it can be seen that the retention rate of FFVPF is almost 100% at pH 4 - 6, and the stability of the NPs is high without leakage. When the pH was adjusted to 7, the retention rate decreased to 77.97 ± 1.15%. At the same time, it can be observed that the transmittance of nanoparticle suspension decreases and flocculation precipitation occurs. If the pH was continuously adjusted to 8, the retention rate continued to decrease and the precipitation continued to increase. In a highly acidic environment with a pH of 2 to 3, the retention rate of NPs dropped to about 80%, but the liquid could maintain high transparency without precipitation. This is due to the protonation and mutual repulsion of free amino groups on CS chain caused by high concentration of acid, resulting in the dissolution and swelling of CS NPs [36]. Conversely, an alkaline environment will reduce the protonation of CS and destroy the cross-linking between CS and TPP, leading to core material leakage [18]. In addition, the pH of the human gastric juice environment is about 2.0, and the pH of the intestinal juice environment is about 7.5. The retention rate of short peptides can reach more than 70% in this range. In conclusion, the CS-TPP FFVPF NPs can not only be applied to food systems with a pH of 4 to 6, but also help to improve the stability of FFVPF in the gastrointestinal tract.
3.4.2 Temperature stability
NPs may undergo heat treatment during food processing and storage. Studying the stability of NPs at different temperatures is conducive to finding appropriate processing methods and storage conditions. We evaluated the effects of different temperature treatments on the stability of NPs (Fig. 4(b). It can be observed that the retention rate below 65℃ is close to 100%, the CS-TPP system loaded FFVPF stability at 65℃ and below. Temperature sensitivity is one of the most important characteristics of drug delivery technology [37]. When researchers used thermogravimetric analysis to characterize the thermal stability of CS-TPP encapsulated peptides, they found that the encapsulated peptides had higher thermal stability compared with the free peptides. The cross-linking of CS and TPP also made CS thermal stability be improved [38]. Danish et al. [39] used CS-TPP system to embed tripeptide LKP and explored the effect of temperature on the stability of nanoparticles through accelerated stability testing. The results showed that the system remained stable at 60℃, but when the temperature reached 70℃, the particle size and PDI of NPs changed significantly, and the phenomenon of instability will appear, which was consistent with the results of this experiment. Therefore, the CS-TPP system loaded with FFVPF can adapt to room temperature storage and processing conditions not exceeding 65℃.
3.4.3 Photochemical stability
The photochemical stability of FFVPF loaded CS-TPP NPs is shown in Fig. 4 (c). When the irradiation time increased to 60 min, the retention rate was still more than 90%. The longer UV irradiation time, the lower retention rate of FFVPF. It has been reported that curcumin-loaded zein CS-TPP NPs are sensitive to UV, and its retention rate will decrease with the increase of UV exposure time [19], which is consistent with the results of this experiment. This result is attributed to the fact that the peptide contains aromatic amino acid residues and double bonds that can absorb part of UV light [40], resulting in its degradation and isomerization when subjected to UV irradiation. The above results show that if the CS-TPP system is used in the food industry, the product can withstand the processing process (sterilization, filling, etc.) without avoiding light within 60 min, but it needs to be packaged in dark or dark storage and transportation to avoid the leakage of functional factors.
3.5 Characteristics of in vitro release
Peptide release from the NPs was mesured at different time intervals at 37℃ to evaluate the peptide retention of NPs. As shown in Fig. 5, we observed a approximate burst peptide release by 77.22 ± 2.21% within the initial 120 min, which may be the result of the physical adsorption of peptides on the surface of NPs. Time for 50% peptide release was round 60 min. These behaviors were also observed in adriamycin and BSA loaded CS NPs. In contrast, insulin loaded CS NPs released 100% within 15 min. The phosphate group of NPs has strong peptide binding. There may be two interactions between peptides and NPs: weak surface adsorption leads to initial release, and strong electrostatic contact leads to slow release.
When the time exceeded 120 min, the release rate significantly slowed down, which shows the same trend as the research results of Luo et al. [41] on the in vitro release of CS-TPP NPs. It indicated that the CS-TPP NPs had a good controlled release performance. In section 3.4.1, the stability of CS-TPP NPs at different pH values was investigated, it was found that when pH was greater than 7.0, the stability of NPs decreases, and the retention rate was about 78%. The pH value of in vitro release experiment was also exactly 7.4. The initial sudden release of the core material may be related to the pH of the system, which may be because the alkaline environment will reduce the protonation degree of CS and destroy the cross-linking between CS and TPP. Previous studies have shown that the release characteristics of CS-TPP NPs are related to CS concentration and drug loading. High concentration of CS increased the cross-linking density and reduced the swelling capacity of NPs, thereby slowing down the drug release rate. In addition, the NPs with large drug loading are more prone to initial suddenly release. Danish et al. [39] compared the in vitro release characteristics of CS-TPP NPs loaded with two tripeptides LKP and IPP respectively. The results showed that IPP released faster than LKP in acidic environment, possibly due to the rigidity and steric hindrance of IPP limited its interaction with CS, indicating that the release characteristics of NPs were also related to the drug properties of NPs.