Toxicity of the venom
The toxicity (LD
50) of crude EC venom was50 μg/mice. This result showed a high toxicity for the EC venom. In the other hand, the mortality rate
of Echiscarinatus envenomation is 10-20 %, if there is no immediate effective treatment (
30). Therefore, it is necessary to develop an advanced antigen delivery system for the preparation of effective antivenom against the venomous snake specie
Echiscarinatus.
Physicochemical characterization of CS NPs
CS NPs were prepared by ionic cross-linking (ionic gelation) of oppositely charged CS and TPP negative ions. Particle size, particle size distribution, and zeta potential of CS NPs were evaluated using the Zetasizer. In this study, suitable characteristics of CS NPs were achieved by polymer concentration of 2 mg/mL, cross-linker of 1 mg/mL, and stirring rate of 1200 rpm. The particle size, Polydispersity Index (PDI), and zeta potential of CS NPs and venom-loaded CS NPs prepared under optimum conditions showed in
Table 1. SEM images showed that CS NPs had integrated surface and good morphology. These particles were approximately spherical, with an almost homogeneous structure. In addition, SEM images showed that the mean particle size of CS NPs was 110 ± 10 nm and that of venom-loaded CS NPs was 215 ± 20 nm, which were approximately similar to the results of Zetasizer (
Figure 1). It is noteworthy here that the size of nanoparticles increased with association of venom molecules due to the presence of large size molecules in venom composition. These results are in line with previous reports (
8). The results showed that entrapment of venom only slightly enhanced zeta potential of nanoparticles. This could be attributed to the increase of particles size and surface area and its consequences are similar to those previously reported by Huang
et al. (
31).
Figure 2 illustrates the Fourier transform-infrared (FTIR) spectra of (A) EC venom, (B) CS, (C) CS NPs, and (D) venom-entrapped CS NPs. Three characteristic absorption bands observed for CS (
Figure 2B) at 3413, 1630, and 1382 cm
−1 were due to -NH, amide I, and amide III groups, respectively, present in CS (
32). In the CS spectra, the strong and broad band in the 3200-3450 cm
−1 range corresponded to amine and hydroxyl groups (-OH stretching and intermolecular hydrogen bonding). The peak near 2930 cm
−1 was caused by -OH stretching. The intense peak at 1382 cm
−1 was caused by -NH stretching of amide in the fingerprint region of the spectra; symmetric stretching of C-O-C was observed around 1070 cm
−1. Absorption band for carbonyl (C=O) stretching of the secondary amide was observed near 1658 cm
−1. The peak at 570 cm
−1 was caused by the saccharide structure of CS.
The peak at 3413 cm
−1 corresponded to the asymmetric and symmetric stretching vibrations of N-H in pure CS. This peak shifted to lower wave numbers at 3400 cm
−1 and was broader and stronger for CS NPs (
Figures 2C and 2D), indicating hydrogen bonding between these groups and TPP. The peaks for CS and CS NPs were broader in this region because of the contribution of -OH stretching peaks and hydrogen bonding (
33). For CS NPs, the peak at 1630 cm
−1 caused by -NH
2bending vibration shifted to 1645 cm
−1. Knaul observed a similar result for CS film treated with NaH
2PO
4 and attributed it to the linkage between phosphoric and ammonium ions (
34). Therefore, it was assumed that tripolyphosphoric groups in TPP were linked to ammonium group in CS, resulting in an enhancement of the inter and intra-molecular actions in CS NPs.
Characteristic peaks of FTIR spectra of EC venom showed peaks around 1650, 1541and 3305 cm
−1, reflecting the acetylamino I, acetylamino II and NH
2 groups, respectively (
35). Acetylamino I at 1650 cm
−1 and acetylamino II at 1541 cm
−1 of EC venom (
Figure 2A) overlapped amide I at 1649 and 1558 cm
−1 of CS NPs; hence, intensive peaks appeared for venom-loaded CS NPs (
Figure 2D).
FTIR spectra of venom-entrapped CS NPs (
Figure 2D) demonstrated that stretching vibrations of -OH and -NH
2 at 3400 cm
−1 were broader. The intense peak at 1414 cm
−1 belonged to C-N stretching. For venom-loaded CS NPs, the 1650 cm
−1 peak of acetylamino shifted to 1658 cm
−1 perhaps because of the cross-linking between EC venom and CS (
34,
36).
| NPs | Mean diameter, nm (n=3) | PDI | Zeta potential (mV) |
|---|
| CS NPs | 127.9 ± 15 | 0.29 | +19.8 ± 1.92 |
| Venom loaded CS NPs | 182.4 ± 20 | 0.35 | +26.8 ± 1.98 |
| Incubation timemonths | Physicochemical characteristics
| Biological activity |
|---|
| Zeta potential(mV) | Size(nm) | Morphology | LD50(µg/mice) |
|---|
| zero time | +26.8 ± 1.98 | 182.4 ± 20 | Spherical/integral surfacenormal distribution | 50 |
| 2 months | +26.8 ± 1.88 | 182.4 ± 20 | Spherical/integral surfacenormal distribution | 50 |
| 4 months | +20.2 ± 2.11 | 184 ± 40 | Spherical/integral surfaceacceptable size distribution | 50 |
| 6 months | +20.2 ± 2.22 | 240 ± 80 | Semi spherical/integral surfaceslight aggregation | 50 |
| Hyperimmunizationsteps | First hyperimmune plasma
| Second hyperimmune plasma
|
|---|
| Common method | Novel method | Common method | Novel method |
|---|
| Potency (mice LD50/mL) | 12 ± 2.5 | 12 ± 3.0 | 20 ± 2.0 | 36 ± 2.0 |
SEM images: (A) chitosan nanoparticles (CS 2 mg/mL, TPP 1 mg/mL) and (B) EC venom loaded chitosan nanoparticles (CS 2 mg/mL, TPP 1 mg/mL, ECV 500 µg/mL
FTIR spectrums: (A) EC venom, (B) chitosan, (C) chitosan NPs (CS 2mg/mL, TPP 1 mg/mL) and (D) EC venom-loaded CS NPs (CS 2 mg/mL, TPP 1 mg/mL, ECV 500 µg/mL
Effect of initial EC venom concentrations on loading efficiency and capacity (CS 2 mg/mL, TPP 1 mg/mL)
In-vitro release profile of EC venom according to Higuchi’s release kinetic formula from venom loaded NPs (CS 2 mg/mL, TPP 1 mg/mL, ECV 500 µg/mL, LC 87%) and venom-entrapped common system
SEM images of venom-loaded CS NPs in stability test: (A) At 0 time, (B) after 2 months, (C) after 4 months and (D) after 6 months
Evaluation of Loading Capacity (LC) and Loading Efficiency (LE)
As illustrated in
Figure 3, LC and LE increased with an increase in the initial venom concentration (from 300 to 500 μg/mL). However, LC and LE decreased when venom concentration increased to 1000 μg/mL. It might be that enhancing initial concentration of the venom until 500 μg/mL leads to improvement of LE and LC, for the reasons of both chemical interaction and physical entrapment induction. However, higher concentrations of venom by increase of viscosity of medium, relative saturation of chemical interaction sites, coupled with physical limitation for entrapment spaces resulted in a decrease of LE and LC. It could be understood that, increase in viscosity of medium made the encapsulation of venom more difficult because the enhanced viscosity might result in a reduced diffusion rate of venom in the chitosan solution. The same explanation was used to discuss the decrease in LE of dexamethasone (
37), LE and LC of BSA (
38) and lysozyme (
39) in CS NPs by higher concentrations of the mentioned agents.
Owing to a suitable LC and LE, an initial concentration of 500 μg/mLwas selected as the optimum venom concentration for preparing venom-entrapped CS NPs. The LE and LC, with this initial venom concentration were 94 and 87%, respectively (
Figure 3).
In-vitro release profile of venom-loaded CS NPs and traditional system
In-vitro release profile of venom-entrapped CS NPs was evaluated using NPs, prepared under optimum conditions (2 mg/mL CS , 1 mg/mL TPP and 500 μg/mL venom initial concentration), with an LC of 87%, and PBS pH of 7.4 as a release medium (
40). The release patterns of venom-entrapped CS NPs and traditional emulsion system are shown in
Figure 4. The venom-entrapped CS NPs demonstrated an initial slow release of the venom in the first 16 h and then a relatively constant release rate until 168 h. Ultimately, approximately 70% of the venom was released from venom-loaded CS NPs within 8 days. As illustrated in
Figure 4, the common venom-loaded adjuvant system indicated a high burst release of about 40% of entrapped venom at the zero time, and 71% of venom was released rapidly for 8 h. From the results of release profile of venom from CS NPs, it is speculated that EC venom is mainly entrapped in NPs and only a small amount of venom is adsorbed on the surface of NPs (
41).
The results demonstrated a suitably sustained release profile for venom from venom-loaded CS NPs prepared in this study and very fast release from emulsion system. The rapid release of venom from common emulsion system could result to high concentration of venom in the injection site and consequently, serious local lesions. Conversely, the immune system will be in contact with the venom for a short period, because of rapid release and degradation of the released venom by enzymes of body fluids. One important situation in vaccine delivery systems from the point of immunogenicity is a sustained release of antigen from NPs. Therefore, this system can serve as a potential and useful effective adjuvant in the preparation of an anti-venom.
Venom release profiles from venom-loaded CS NPs were assessed by different release kinetics: zero order, first order, Higuchi model, Korsmeyer-Peppas model, and Hixson-Crowell model. Obtained data showed that this is closest to Higuchi model. Higuchi in 1961 put forth the first mathematical model to describe drug release from a matrix system. Although the model was initially conceived for planar systems, it was later extended to different geometrics and porous systems (
42).
Release profile of venom-loaded CS NPs (
Figure 4) indicated that CS NPs with a huge large surface area could adsorb EC venom, thus allowing the venom to be released easily in the first few hours and at a constant rate later because of the slow degradation of CS NPs, and consequently the release of entrapped venom (
11).
Accelerated stability studies
Biological stability of EC venom encapsulated in CS NPs was measured using the Finney method based on a method used for venom before loading. The biological activity of the venom was expressed in terms of LD
50 (
25). For physicochemical stability, average particle size, surface potential, and morphology were measured. The results are summarized in
Table 2.SEM images of venom-loaded CS NPs in stability test at zero time, after 2, 3, 4 and 6 months are shown in
Figures 5A, 5B, 5C and 5D, respectively. The results of the accelerated stability studies showed that venom-entrapped CS NPs had a highly favourable biological and acceptable physicochemical stability for 6 months. After 6 months, the zeta potential of venom-loaded CS NPs decreased slightly (
Table 2), resulting in a slight aggregation of venom-loaded CS NPs (
Figure 5D). However, the biological activity of the venom released from CS NPs after 6 months was similar to zero time and the venom remained intact during accelerated stability study as shown in
Table 2.
The results of this study revealed good physicochemical and biological stability of venom loaded NPs (
43). At this point , it is important to notice the school of thought of the effect of freeze drying on enhancing stability of venom entrapped NPs (
44).
Lethality neutralization potency of hyperimmune plasma
In this study, both the hyperimmunization procedures showed the same lethality neutralization resulted in the first stage of hyperimmunization. After the second stage of hyperimmunization of animals, by using a similar dose of antigen in both methods, the novel system showed higher potency (~ 2 fold) for neutralizing the venom than the conventional system (
Table 3). The mean venom lethality neutralizing titer in the novel system group was significantly greater than the traditional adjuvant groups (
P < 0.05).
These results indicated that in addition to having favourable features such as biodegradability, biocompatibility, ease of preparation, good stability, and long-term preservation of antigens without changes in their biological and physiological properties, the novel antigen delivery system could elicit a good immune response and produce hyperimmune plasma, having high potency to neutralize the venom compared with that obtained using conventional adjuvants. Moreover, the conventional antigen delivery system with W/O emulsion has some setbacks, such as instability, complex preparation process, time consuming, expensive, adverse reactions at injection site (such as scars and pain) in animals, and damage to loaded antigens (
3,
45-
47).