Preparation and characterization of the SLNs
Establishment of electrostatic interactions between amphotericin and DSPG provides an approach to overcome the poor solubility of polyenes in organic solvents. In this study, suspended dispersion of AMB in organic solvents (i.e. combination of methanol and dichloromethane) was completely dissolved in the presence of acidified DSPG and resulted in formation of an orange transparent solution without presence of any colloidal or suspended particles indicating formation of AMB-DSPG complex. The concentration of AMB-DSPG complex was evaluated by HPLC and reported as 960 ± 14.21 µg mL-1 while the concentration of equal amount of AMB dissolved in the same organic solvents in the absence of DSPG was reported as 345 ± 5.76 µg mL-1 indicating significant role of complexation in enhancing the solubility of AMB in the organic solvents.
In this study, fractional factorial design was employed for preparation of the SLNs to evaluate all the main effective and possible binary interactions to determine which independent variables and interactions have significant influence on the defined responses. In this case, 11 formulations of AMB-loaded SLNs were prepared by solvent emulsification-evaporation method, using a 25- fractional factorial design accompanying with three center points. The values of independent variables and the related experimental data in suggested formulations (
i.e. F1-F11) are summarized in
Table 2.
In this study, analysis of responses performed using design-expert software showed that dependent variables including particle size (Y1) and pdI (Y2) were both fitted to 2-factorial interaction (2-FI) model with the model
p-value of 0.0161 and 0.0023, respectively. The values of R2, adjusted R2, Adeq precision, SD and CV% are summarized in
Table 3.
Size of the nanoparticles
Particles with mean diameter ranging from 176.7 ± 5.09 nm to 393.6 ± 47.5 nm were obtained in various suggested runs as shown in
Table 2. Statistical analysis performed by Design-Expert® based on fractional factorial design was applied to establish the best significant fitted model for prediction of the size of particles. The characteristics of fitted model are summarized in
Table 3. The analysis of variance for data revealed that the linear coefficients of the all independent factors, except factor E, and interaction coefficients of BC and BE were significant (
p < 0.05). The coefficients of significant variables on particle size (Y1) have been shown in Equation 3 as follows:
Y1 = +219.46 + 21.84A - 18.76B + 32.44C - 38.24D - 15.94BC - 34.66BE
(Equation 3)
Where:
Y1: Particle size;
A: Coefficient of GMS/Lecithin
concentration ratio;
B: Coefficient of PEG 400 concentration (%);
C: Coefficient of Tween 80 concentration (%);
D: Coefficient of emulsifying time (h);
E: Coefficient of cooling time (h);
BC: Interaction coefficient of B and C;
BE: Interaction coefficient of B and E;
As shown in the equation, both coefficients of A and C showed a positive effect on the size of nanoparticles (Y1). It means that particle size would be expected to be increased with increasing either concentration ratio of GMS/Lecithin (A) or concentration of Tween 80 (C). GMS, as the central core, forms the lipid matrix of the SLNs. Therefore, it is sensible that an increased particle size can be observed with higher concentration ratios of GMS/lecithin (
27). This phenomenon was in well accordance with previous studies which showed the dependency of the size of SLNs on the concentration of GMS as the lipid matrix and it was previously reported that increased amount of GMS caused an increase in particle size which can be explained in terms of tendency of the lipid to coalesce at high concentration. Based on Stoke’s law, the difference in density between internal and external phase can interpret this behavior (
28). Moreover, the study of Mehnert and Mader demonstrated that particle size of SLNs would be increased by increasing the lipid content of nanoparticles (
29). This can be due to a decrease in homogenization efficiency by increasing the viscosity of inner phase followed by increasing the lipid concentration (
27,
30).
In this study, tween 80 was selected as the surfactant and as indicated in Equation 3, the positive sign of the related coefficient demonstrates that increased level of tween 80 can lead to particle size increasing of the prepared SLNs. This can be justified by considering that the high concentration of surfactants causes an increase in viscosity of aqueous phase which in turn, reduces the homogenization efficiency and consequently decreases the tendency for particles breakdown (
31). Moreover, high concentrations can promote aggregation of the surfactant molecules at the surface of particles along with establishment of loops and tails which consequently leads to bridging between the nanoparticles and promotes aggregation. The studies performed by Tiyaboonchai
et al. revealed an increase in particle size of SLNs followed by increasing the concentration of surfactant (
32). In some studies it was suggested that in increased concentration of surfactants, establishment of strong intermolecular interaction via hydrogen bonds between surfaces of prepared SLNs can lead to particle size increasing and tendency of aggregation in nanoparticles (
33).
As confirmed by Equation 3, concentration of PEG 400 (B) as well as emulsification time (D) had negative effects on the particle size (Y1). It means that the particle size would be expected to be decreased with increasing either concentration of PEG 400 or emulsification time. Polyethylene glycol (PEG), through its characteristics, can act as an hydrophilic shield in SLNs and other drug carriers and consequently reduces the surface tension of SLNs and can lead to a decrease in particle size (
34). Furthermore, PEG 400 can provide favorable conditions to establish a more stable and dispersed formulation of nanoparticles (
22). In accordance with this observation, Liu
et al. (
33) have suggested PEG 400 as the ideal co-surfactant to prepare diclofenac-loaded SLNs with a relative smaller particle size. Negative sign of the coefficient of factor D (
i.e. emulsification time) demonstrates that increased duration of homogenization cycle can lead to decrease in particle size, since generated shear force can have more available time for particles breakdown (
31).
As can be seen in Equation 3, BC and BE as the binary interactions showed a significant effect on particle size of the SLNs. In order to study the interaction patterns between variables, 3D response surface curves were plotted by model prediction of the particle size (Y
1) at different levels of the effective two variables while keeping the other variables at their center levels (
Figure 2). As shown in
Figure 2a, although in lowest value for cooling time (
i.e. 0.25 h), the size of particles was slightly increased followed by increasing the concentration of PEG 400 from 0.0% to 3.0%, in highest value for cooling time (
i.e. 2.0 h) a sharp decrease in the size of particles was observed followed by increasing the concentration of PEG 400. Moreover, it is obvious from the figure that in the absence of PEG 400, size of the SLNs was sharply increased by increasing the cooling time from 0.25 h to 2.0 h while in highest concentration of PEG 400, a decrease in the size of the particles was observed due to increase in cooling time.
As shown in
Figure 2b, in lowest concentration of tween 80 (
i.e. 0.25%), increasing the concentration of PEG 400 from 0.0% to 3.0% had no significant effect on the size of the particles while in highest concentration of tween 80 (
i.e. 4.0%), a sharp decrease in the size of the SLNs was observed followed by increasing the concentration of PEG 400. On the other hand, as can be seen in the figure, in absence of PEG 400, the size of particles was sharply increased by increasing the concentration of tween 80 from 0.25% to 4.0%. The same trend with slower rate was observed for increasing the size of particles due to increase in concentration of tween 80 in the presence of high concentration of PEG 400 (
i.e. 3.0%).
PdI of the nanoparticles
As shown in
Table 2, the experimentally observed PdI is ranged from 0.17 ± 0.015 to 0.491 ± 0.03. Homogeneity of nanosuspensions becomes higher as the PdI approach to zero (
30). Statistical analysis performed by Design-Expert® based on fractional factorial design was applied to establish the best significant fitted model for prediction of the PdI. The characteristics of the best fitted model are summarized in
Table 3. Analysis of variance for data revealed the linear coefficients of the all independent factors except factor C, and interaction coefficients of B.C and B.E were significant (
p < 0.05). The coefficients of the significant variables on pdI (Y2) have been shown in Equation 4 as follows:
Y2 = +0.30 - 0.055 A - 0.022 B - 0.027D + 0.033E + 0.022BC - 0.075BE
(Equation 4)
Where:
Y2: PdI of Particles;
A: Coefficient of GMS/ Lecithin
concentration ratio;
B: Coefficient of PEG 400 concentration (%);
C: Coefficient of Tween 80 concentration (%);
D: Coefficient of emulsifying time (h);
E: Coefficient of cooling time (h);
BC: Interaction coefficient of B and C;
BE: Interaction coefficient of B and E;
As confirmed by Equation 4, three factors including concentration ratio of GMS/Lecithin (A), concentration of PEG 400 (B), and emulsification time (D) had negative effects on PdI of the nanoparticles (Y2). It means that PdI would be expected to be decreased by increasing either factor A, B or D while cooling time as factor E revealed a positive effect on PdI of the particles.
As can be seen in Equation 4, BC and BE as the binary interactions showed a significant effect on PdI. In order to study the interaction patterns between variables, 3-D response surface curves were plotted by model prediction of the PdI at different levels of the effective two variables while keeping the other variables at their center levels. The 3-D response surface plots of observed PdI are provided in
Figure 3.
As shown in
Figure 3a, although in the absence of PEG 400, PdI of the nanoparticles was slightly decreased by increasing the concentration of tween 80 from 0.25% to 4.0%, in high concentration of tween 80 (
i.e. 4%) the alteration in the PdI due to increase in concentration of PEG 400 from 0.0% to 3.0% was not significant. Moreover, it is obvious in the figure that in low concentration of tween 80 (
i.e. 0.25%) the polydispersity of the particles was sharply decreased followed by increasing the concentration of PEG 400 from 0.0% to 3.0%.
As illustrated in
Figure 3b, in the absence of PEG 400, PdI of the nanoparticles was sharply increased by increasing in cooling time from 0.25 h to 4.0 h. On the other hand, in highest concentration of PEG 400 (
i.e. 3.0%) a slight decrease in PdI of the particles was observed. Moreover, in lowest value for cooling time (
i.e. 0.25 h), PdI of the particles was observed to increase by increasing the concentration of PEG 400 from 0.0% to 3.0% while in highest values for cooling time (
i.e. 2.0 h) a sharp decrease in PdI of the SLNs was observed followed by increasing the concentration of PEG 400.
Optimization and model validation
Optimization of the physicochemical characteristics of the SLNs was carried out according to statistical analysis of the experimentally obtained data using fractional factorial design. The criteria for dependent variables (
i.e. size and PdI) were previously stated as the constrains in
Table 1. The optimized conditions for preparation of the SLNs which were predicted by the Design-Expert® software using modeling and regression analysis, are shown in
Table 4. To determine the model validation and calculation of the appropriate prediction error, the suggested optimized formulation was prepared and characterized experimentally (n = 5). The observed responses and value of predicated errors are indicated in
Table 5. As shown in the table, the calculated prediction errors were well below 10% for all items demonstrating the proper predictability, efficiency and adequacy of the fitted models. EE%, DL% and zeta potential are critical parameters for evaluation of physicochemical characteristics of submicron systems. Accordingly, EE% of the optimized SLNs formulation was calculated and determined as high as 89.3 ± 3.47% which demonstrates that the AMB-DSPG complexes can be successfully loaded into the nanostructures. Drug loading (DL%) is ordinarily defined in percent related to the lipid phase that was determined to be 2.76 ± 0.32 (
Table 5). Zeta potential of the particles considered as an indicator for prediction of the stability of the colloidal dispersion (
35). Accordingly, particle aggregation is less likely to occur in high zeta potentials (either positive of negative) due to high electrostatic repulsion forces between particles (
36). Therefore, nanoparticles with zeta potential values greater than +20 mV or less than -20 mV exhibit high degrees of stability (
37). As shown in
Table 5, zeta potential of the optimized SLNs was determined as -30.16 ± 1.6 mV which can ensure proper stability for the AMB loaded SLNs. According to the previous studies, the negative charge of zeta potential is related to the lipids that incorporate into the SLNs structure (
38,
39). In this study, surface accumulation of GMS as the main lipid in the structure of the SLNs resulted in high negative zeta potential of the nanoparticles.
Lyophilization of the nanoparticles
The effect of freeze drying process in the presence of the cryoprotectant (
i.e. sucrose 5% w/v) on physicochemical characteristics of the SLNs including particle size, PdI and zeta potential was investigated and the appropriate results are illustrated in
Figure 4. Previous studies revealed that di-saccharides such as sucrose are more efficient cryoprotectant compared to mono-saccharides and consequently exhibit higher efficiency in conserving the physicochemical features of nanoparticles during lyophilization (
40,
41).
As shown in
Figure 4a, although the size of the SLNs was slightly increased from 187 ± 11.97 nm to 203 ± 16.49 nm during lyophilization, statistical analysis of data using two independent sample t-test revealed no significant differences in the size of the nanoparticles before and after freeze-drying (
p-value > 0.05).
Figure 4b revealed that the PdI of the nanoparticles was significantly increased from 0.188 ± 0.028 to 0.241 ± 0.036 during the lyophilization (
p-value < 0.05). Determination of zeta potential is an effective method to consider the eventual interactions between the cryoprotectant molecules and the nanoparticles surface (
42,
43). It was showed that the zeta potential of the particles was significantly decreased from -30.16 ± 1.6 mV to -26.24 ± 1.71 mV (
p-value < 0.05) due to accumulation of the sucrose molecules at the surface of the nanoparticles which can lead to establishment of hydrogen bonds and consequently masking the negative charges of the lipids (
Figure 4c) (
44,
45).
Preparation and Characterization of DPI
In this study, lyophilization technique was employed to prepare the DPI formulations. For this purpose, various concentrations of lactose (i.e. 1, 5, 10, 15 and 20%w/v) as the inhalational carrier were applied to provide the intended dispersions. Each formulation was freeze dried over a period of 72 h and analyzed by Anderson cascade impactor.
As can be observed in
Table 6, analysis of the results showed that by increasing the lactose concentration in the SLNs dispersions, the particle size of the DPIs was increased. Pisponen
et al. suggested that the observed particle size increasing of DPI formulations followed by increase in lactose concentration can be due to classical nucleation theory (
46). Lactose is one of the major factors initiating the nucleation process in a solution. Accordingly, in a more concentrated solution of lactose nuclear growth can be promoted and more lactose molecules crystallized.
DPIs with particle size values above 5µm and below 1 µm cannot access the peripheral airways properly. This is due to their immediate elimination after deposition in oral cavity (
i.e. > 5 µm) and their little and slow deposition which is affected by Brownian motion (
i.e. < 1 µm) (47). Therefore, the optimal size for pulmonary drug delivery of the particles is in the range of 1µm to 5 µm in aerodynamic diameter. Fine particle fraction (FPF) is defined as the percentage of particles with aerodynamic diameter between 1 µm to 5 µm which can access to the alveoli. As indicated in
Table 6, the calculated FPFs were 35.71 ± 1.81%, 53.96 ± 3.67%, 72.57 ± 4.33%, 54.99 ± 3.04%, and 22.03 ± 2.53% in various DPI formulations containing lactose 1%, 5%, 10%, 15% and 20% w/v, respectively. It was revealed that the highest FPF% was obtained using lactose 10% and therefore, this formulation was suggested to be efficient for drug delivery to the peripheral airways.
In-vitro release study
The
in-vitro release of AMB from the optimized SLNs and also DPI formulations was evaluated in phosphate buffer saline (PBS) adjusted to a pH value of 7.4. The results are illustrated in
Figure 5. As shown in the figure, 58.23 ± 4.89% and 61.22 ± 5.70% of entrapped AMB was released from the optimized SLNs over a period of 24 h and 48 h, respectively indicating a slow and sustained release behavior.
In-vitro release of AMB from the dry powders was also determined using formulation of 10 %w/v of lactose and the similar sustained release behavior was obtained. Similarly, various studies reported slow and sustained release behavior of drugs encapsulated into SLNs preparations (
48-
50). Therefore, SLNs are suggested as suitable carriers for prolonged and sustained drug release (
36) and this can be achieved when drug is homogenously dispersed into the lipid matrix and can only be released through diffusion (
47). Moreover, in the study performed by Kushwaha
et al., it was suggested that the slow release of drug from SLNs may be due to increased diffusional distance and hindrance effects of lipid shells which prevent surrounding aqueous medium to penetrate inside the particles and release the encapsulated through dissolution mechanism (
50).
The drug release data were fitted to various mathematical kinetic models including zero order, first order, Higuchi, Hixon–Crowell and Korsmeyer-Pepas using Sigma-plot® software (version 10.0.0.54). As shown in
Table 7, release kinetic of the both optimized SLNs formulation and DPI preparation were best fitted to the first order kinetic model. In this study, the sustained release of AMB from the optimized SLNs describes the diffusion of the drug from homogenous matrix system which is in well accordance with fickian diffusion mechanism explained by the first order release kinetic model. The studies performed by Priyanka and Hasan revealed first order release kinetic of all montelukast-loaded SLNs formulations (
51). Moreover, the study of Kakkar
et al. showed first order release kinetic of curcumin from SLNs (
52).
Morphology of the particles
Scanning electron micrographs of the SLNs and DPI formulations are illustrated in
Figure 6. As shown in
Figure 6a, the SEM images revealed a spherical shape and smooth surface particles with diameters in accordance with data obtained by photon correlation spectroscopy (PCS). The DPI samples using formulation of 10% w/v of lactose were also examined and the SEM images showed a cubic shape and smooth surface particles (
Figure 6b). No sign of aggregation was detected in the SEM images.
Chemical structure of (a) amphotericin B; (b) DSPG, (ChemDraw Ultra v. 7.0 software).
3D plots of effective binary interactions on particle size, (a) BE interaction, (b) BC interaction
3D plots of effective binary interactions on pdI, (a) BC interaction, (b) BE interaction
Influence of lyophilization on SLNs characteristics, (a) particle size (nm) (b) pdI (c) zeta potential (mV). Data represent Mean ± SD, n = 5. *Results are significantly different, p < 0.05.
Cumulative AMB release profile from the SLNs and DPI formulation (PBS, pH 7.4, n = 3).
SEM images of the particles, (a) optimized SLNs; (b) DPI formulation
| Independent variables (factors) | Levels
|
|---|
| -1 | +1 |
|---|
| A: GMS/Lecithin ratio | 0.25 | 3 |
| B: PEG 400 (w/v%) | 0 | 3 |
| C: Tween 80 (w/v%) | 0.25 | 4 |
| D: Emulsifying time (h) | 0.25 | 3 |
| E: Cooling time (h) | 0.25 | 2 |
| Dependent variables (responses) | Constrains |
| Y1 = size (nm) | Minimize |
| Y2 = pdI | Minimize |
Dependent variables (responses)
| Independent variables (factors)
| Formulation no. |
|---|
| Y2(mean ± SD) | Y1 (nm)(mean ± SD) | E | D | C | B | A |
|---|
| 0.30 ± 0.01 | 178.20 ± 6.70 | 2.00 | 0.25 | 0.25 | 3.00 | 0.25 | F1 |
| 0.22 ± 0.04 | 203.00 ± 8.40 | 0.25 | 0.25 | 0.25 | 0.00 | 3.00 | F2 |
| 0.22 ± 0.01 | 190.20 ± 4.80 | 0.25 | 3.00 | 0.25 | 3.00 | 3.00 | F3 |
| 0.24 ± 0.01 | 181.90 ± 5.30 | 1.13 | 1.63 | 2.13 | 1.50 | 1.63 | F4 |
| 0.49 ± 0.03 | 176.70 ± 5.09 | 2.00 | 3.00 | 0.25 | 0.00 | 0.25 | F5 |
| 0.17 ± 0.01 | 178.30 ± 4.10 | 2.00 | 3.00 | 4.00 | 3.00 | 3.00 | F6 |
| 0.25 ± 0.02 | 190.00 ± 2.82 | 1.13 | 1.63 | 2.13 | 1.50 | 1.63 | F7 |
| 0.24 ± 0.03 | 201.00 ± 4.24 | 1.13 | 1.63 | 2.13 | 1.50 | 1.63 | F8 |
| 0.21 ± 0.02 | 179.60 ± 12.44 | 0.25 | 3.00 | 4.00 | 0.00 | 0.25 | F9 |
| 0.42 ± 0.10 | 256.00 ± 60.81 | 0.25 | 0.25 | 4.00 | 3.00 | 0.25 | F10 |
| 0.37 ± 0.02 | 393.60 ± 47.50 | 2.00 | 0.25 | 4.00 | 0.00 | 3.00 | F11 |
| Adeq Precision | adjusted R-Squared | R-Squared | CV | Best fitted model | Response factor |
|---|
| 25.0130 | 0.9792 | 0.9954 | 4.5300 | 2FI | Particle size |
| 64.4350 | 0.9970 | 0.9993 | 1.9200 | 2FI | pdI |
| Desirability | Predicted dependent variables (responses) | Optimized Independent Variables |
|---|
| 0.86 | Y2 = PdI | Y1 = size (nm) | E: Cooling time (h) | D: Emulsification time (h) | C: Tween 80 (w/v%) | B: PEG 400 (w/v%) | A: GMS/ Lecithin |
| 0.172 | 174.63 | 0.27 | 2.78 | 2.11 | 0.15 | 2.46 |
Optimized SLNs characteristics
| Dependent variable (responses)
|
|---|
| DL (%) | EE (%) | Zeta (mV) | pdI | Size (nm) |
|---|
| Observed response (Mean ± SD) | Observed response (Mean ± SD) | Observed response (Mean ± SD) | Prediction Error (%) | Observed response (Mean ± SD) | Prediction Error (%) | Observed response (Mean ± SD) |
| 2.76 ± 0.32 | 89.30 ± 3.47 | -30.16 ± 1.60 | + 8.51 | 0.188 ± 0.028 | + 6.63 | 187.04 ± 11.97 |
| Fine Particle Fraction (FPF) (%) Mean ± SD | Drug deposition (%)
| Lactose (%) | No. |
|---|
| Stage 8 (0.52 µm) Mean ± SD | Stage 7 (0.93 µm) Mean ± SD | Stage 6 (1.55 µm) Mean ± SD | Stage 5 (3.5 µm) Mean ± SD | Stage 4 (5.0 µm) Mean ± SD | Stage 3 (9.8 µm) Mean ± SD | Stage 2 (14.8 µm) Mean ± SD | Stage 1 (21.3 µm) Mean ± SD |
|---|
| 35.71 ± 1.81 | 32.54 ± 3.62 | 26.50 ± 3.42 | 6.48 ± 1.31 | 2.73 ± 0.62 | 2.44 ± 0.86 | 0.67 ± 0.12 | ND1 | ND1 | 1 | 1 |
| 53.96 ± 3.67 | 25.87 ± 4.72 | 24.61 ± 2.65 | 17.93 ± 3.42 | 11.42 ± 3.15 | 9.27 ± 2.38 | 4.68 ± 1.47 | 1.31 ± 0.18 | ND1 | 5 | 2 |
| 72.57 ± 4.33 | 10.31 ± 3.57 | 23.52 ± 4.11 | 27.10 ± 3.95 | 21.95 ± 4.83 | 4.39 ± 2.52 | 5.61 ± 1.83 | 2.24 ± 0.68 | 2.93 ± 0.73 | 10 | 3 |
| 54.99 ± 3.04 | 2.63 ± 0.96 | 10.88 ± 2.75 | 18.43 ± 3.52 | 25.68 ± 2.41 | 11.46 ± 3.78 | 17.13 ± 3.27 | 7.49 ± 1.59 | 8.74 ± 2.86 | 15 | 4 |
| 22.03 ± 2.53 | ND1 | 4.94 ± 1.21 | 7.37 ± 3.64 | 9.72 ± 2.31 | 15.53 ± 3.64 | 18.90 ± 2.75 | 22.83 ± 3.56 | 20.37 ± 3.63 | 20 | 5 |
| Fitted Theoretical Models | R2
| Adjusted R2
| constants
|
|---|
| SLNs | DPIs | SLNs | DPIs | SLNs | DPIs |
|---|
| Zero Order | 0.0000 | 0.0000 | 0.0000 | 0.0000 | _ | _ |
| First order | 0.9862 | 0.9861 | 0.9839 | 0.9838 | K1 = 0.176 | K1 = 0.176 |
| Hixon-Crowell | 0.0000 | 0.0000 | 0.0000 | 0.0000 | _ | _ |
| Higuchi | 0.7925 | 0.7922 | 0.7765 | 0.7762 | Kh = 0.1951 | Kh = 0.1952 |
| Korsmeyer-Pepas | 0.8466 | 0.8464 | 0.8348 | 0.8346 | Kp = 0.269 n = 0.385 | Kp = 0.269 n = 0.385 |