2.1. PHB-Based Microspheres
Two types of PHB-based microspheres were prepared, namely MS-1, which contained macroscopic pores, and MS-2, which did not contain such pores (see
Section 4.2.1). These microspheres were either drug-free or loaded with SVN. Then, the respective microbeads were used as fillers for the fabrication of composite PVACGs. The appearance of both MS-1 and MS-2 microspheres in the dry state is shown in
Figure 1 (optical microscopy) and
Figure 2 (SEM-images).
Numerous rounded cavities (pores) with a diameter of 2–20 μm are observed on the surface of the MS-1 matter (
Figure 2a). Such macropores are known [
41] to be formed as a result of the entrapment of small drops of the aqueous phase into the organic phase (solution of PHB in chloroform) during emulsification of the PHB/chloroform solution in aqueous solution of ammonium carbonate. In the case of the absence of ammonium carbonate in the aqueous phase, the resulting PHB microspheres did not contain “so large” pores (
Figure 2b). The presence of macroscopic pores in the bulk of MS-1 particles increases their inner surface, thus increasing their absorption capacity toward relatively hydrophobic substances. At the same time, the absence of macropores, in addition to decreasing the amount of the loaded substance in the microspheres, could influence the kinetics of the release of substances from MS-2, slowing down the rate of release for drugs entrapped into such particles.
The size of MS-1 beads (
Figure 1a and
Figure 2a) was several times larger compared to that of the MS-2 particles (
Figure 1b and
Figure 2b). The images obtained with an optical stereomicroscope (
Figure 1) were analyzed using an Image J program.
Figure 3 shows the Gaussian distribution of particle diameters (µ). The respective values of the Gaussian function coefficients, mathematical expectation (σ), and standard deviation (R
2) are presented in
Table 1.
It was found that the average diameter of MS-1 was 299 µm and of MS-2 was 75 µm. The sizes of MS-2 were within a narrower range, while the diameters of MS-1 had a much larger deviation. Therefore, at the same mass of spherical PHB particles, the number of microspheres without macroscopic pores, i.e., MS-2 matter, will be greater than the number of MS-1 particles with macroscopic pores.
2.2. Physico-Mechanical Properties of the Filler-Free and Composite PVA Cryogels
Physico-mechanical characteristics of cryogels are important parameters of these materials. It is possible to tailor the gel strength of PVACGs for the imitation of a wide range of biological soft tissues [
6,
10]. For this reason, such materials are attractive for application as prosthetic cartilages [
13,
14,
15], blood vessels [
42], heart valves [
43], and various implants [
10,
26].
In the present study, upon the formation of composite cryogels, the concentration of the gel-forming polymer, i.e., PVA, was varied, while the mass of PHB-based particles entrapped into the cryogel bulk was identical for all types of microspheres. It was found earlier [
34] that when wet PHB-based microspheres are dispersed in the initial solutions of PVA, their distribution over the cryogel matter after its formation is sufficiently uniform; therefore, wet microspheres of preliminary measured moisture content were used. Moreover, the absence of particle cohesion in the initial suspension can also indicate that the distribution of dispersed particles in the gel matrix could be without the presence of some agglomerates of the respective microspheres. It is clear that this assumption requires experimental confirmation, which requires appropriate time and the use of independent methods for the elucidation of the micro- and macrostructure of the composite cryogels under discussion. We have already begun such studies, and their results will be published. The compositions of the corresponding feed solutions and suspensions are given in
Table 2, and the compression moduli of elasticity (E) of the respective filler-free and composite PVACGs are illustrated by the diagrams in
Figure 4.
The growth of the rigidity of filler-free PVA cryogels with increasing concentrations of the gel-forming polymer is well known [
4]. In turn, the ability of some fillers to increase the gel strength of PVACGs indicates that such dispersed fillers, the PHB microspheres in our case (
Figure 4), act as so-called “active” fillers [
44]. This effect is associated with the higher rigidity of the particles of the discrete phase compared to the continuous phase, and the effect is also provided by good compatibility of these two phases [
45]. Thus, the data obtained in the present study testify that the entrapment of relatively hydrophobic PHB microspheres into the matrix of PVA cryogels did not cause deterioration in the mechanical properties of the resultant composite cryogels. Therefore, the use of MS-2 had a somewhat greater effect on the elastic modulus of the composite samples compared to that of the MS-1-filled PVACGs, which is probably due to the difference in the size of filler microbeads and, accordingly, the number of particles per unit volume of PVA cryogel, thus, in the case of MS-2 filler, increasing the contact area of the matrix with dispersed particles.
2.4. Lease of Ibuprofen Sodium Salt
In contrast to simvastatin, which was incorporated into PHB microspheres during their formation, the sodium salt of ibuprofen was introduced into the already-formed cryogel samples. This approach was motivated by the observation that only a small fraction of ibuprofen sodium salt remained in the particles when introduced during the process of microsphere formation (~1–3% for MS-1 and ~17–19% for MS-2). This “loss” is attributed to the leaching of ibuprofen sodium salt at various stages of PHB particle formation. Therefore, composite cryogel samples were saturated with solutions of this drug within a certain time (
Figure 7).
The amount of Na-IBPF incorporated into the gel matrix was determined by measuring the optical absorption of the liquid overlaying the cryogel. Knowing the initial concentrations of the solutions and the concentration during and after sample saturation, the amount of ibuprofen sodium salt in the cryogels was quantified (
Figure 7). Notably, the amount of drug in solution ceased to change significantly after approximately 24 h. The ~2.1 mL PVA cryogel samples without filler absorbed a smaller amount of Na-IBPF (~0.375 mg) compared to composite samples (~0.75 mg for samples filled with MS-1 and ~1 mg for those filled with MS-2). Different drug uptakes by composite cryogels and unfilled PVA cryogels arise from the presence of PHB microspheres, which facilitate drug absorption. Furthermore, the difference between the composite cryogels that contained MS-1 and MS-2 is attributable to the larger surface area of MS-2, which enhances drug absorption. The greater amount of non-porous microspheres per unit volume of the composite also increases the interaction area, providing greater drug binding.
Figure 8 presents a plot of Na-IBPF release from PVA cryogels. The kinetics of drug release from loaded cryogel samples was analyzed using first-order (1), Higuchi (2), and Peppas–Korsmeyer (3) models, applied to the nonlinear portions of the curves.
where M
t is the amount of drug released at the time t, M
∞ is the drug amount released at the infinite time, and k
1 is the first-order constant [
55].
where M
t is the amount of drug released at the time t, M
∞ is the drug amount released at the infinite time, and k
h is the release constant of Higuchi [
55,
56].
where M
t/M
∞ is the fraction of drug released at each time point (t), K is the constant of incorporation of structural modifications and geometrical characteristics of the system (also considered the release velocity constant), and n is the exponent of release (related to the drug release mechanism) in function of time. For cylindrical samples, n ≤ 0.45—Fickian diffusion; n > 0.45—non-Fickian mechanisms (anomalous transport) [
55,
57].
The selection of these models is justified, as they elucidate the mechanism of drug release. In our case, the release profiles correspond to the first-order model, particularly for the unfilled PVA cryogels (
Table 3). High values of the coefficient of determination for the Higuchi model (
Table 3) indicate that drug release predominantly exhibits a diffusion character according to the Fick’s law. The values of the release rate index n from the Peppas–Korsmeyer model for all studied PVA cryogel samples were less than 0.45 (
Table 3), further confirming that the release mechanism is driven by Fickian diffusion. Other release mechanisms are minimally impactful in this scenario, as the cryogel samples are already in a swollen state, allowing for only slight a relaxation of the polymer chains, with no observed dissolution processes or erosion of PHB microspheres. The kinetic constant K from the Peppas–Korsmeyer model suggests a decreased drug release rate in the presence of PHB microspheres in the PVA cryogel matrix, particularly evident with MS-2 particles.
To determine the diffusion coefficients of the drug in the carrier matrix, we used the equation derived from Fick’s second law for cylindrical samples [
56,
58,
59]:
where M
t is the amount of drug released at the time t, M
∞ is the drug amount released at the infinite time, D is the diffusion coefficient of drug in the carrier matrix, and R is the radius of the sample.
Considering that the Higuchi model (2) is based on the Fick’s law, then
From here, the diffusion coefficients (D) of the ibuprofen sodium salt were calculated (the radius of the samples was 0.75 cm):
Unfilled PVA Cryogel | 1.81 × 10−5 cm2/s |
PVA cryogel filled with MS-1 particles | 1.64 × 10−5 cm2/s |
PVA cryogel filled with MS-2 particles | 1.58 × 10−5 cm2/s |
The study of the release kinetics of ibuprofen sodium salt from both unfilled PVA cryogel samples and composite PVA cryogels filled with PHB microspheres showed that the slowest release occurred from the samples containing MS-2. The size, distribution, and density of microspheres per unit volume of cryogel play a critical role in modulating the release rate by enhancing the interaction between the drug and filler particles and prolonging the release from the composite cryogel matrix.
To further elucidate the release kinetics of ibuprofen sodium salt from the PVA cryogel samples, we employed the Weibull function (6), a well-established tool for analyzing drug release mechanisms from various polymer matrices, which allows the assessment of the influence of the matrix on the drug release [
55,
60,
61,
62,
63].
where M
t/M
∞ is the fraction of dissolved matter released from the matrix during time t; parameters a and b are constants.
The constant b is generally regarded as a descriptor of the gel matrix structure, serving as an indicator of the release kinetics related to the matrix characteristics [
62]. A b value less than 0.35 indicates a highly disordered space, which is significantly different from a percolation cluster. When the matrix has a fractal cluster structure, b values fall between 0.35 and 0.39. If b is between 0.39 and 0.69, diffusion takes place within a fractal or disordered substrate that is separate from the percolation cluster. In contrast, a b value of 0.69 to 0.75 suggests a clearly defined geometric (Euclidean) matrix structure [
62].
The analysis of Na-IBPF release from PVA cryogels (
Figure 9) via the Weibull function corroborates the conclusions derived from earlier models. The sodium salt of ibuprofen is released most rapidly from the samples without microspheres, whereas the presence of PHB microparticles exerts a prolonging effect on the release process. This conclusion is supported by the coefficient a (
Table 4), representing the release rate constant [
62]. The parameter b for all samples falls within the range of 0.39–0.69, suggesting that diffusion transpires in a disordered substrate. Furthermore, while b describes the matrix structure, it can also indicate interactions between the gel matrix and the releasing agent, with higher values of b reflecting weaker interactions [
64]. Notably, the highest b values correspond to samples lacking PHB microspheres (
Table 4). Consequently, the presence of spherical PHB particles in the PVA cryogel matrix contributes to slowing down the release of ibuprofen sodium salt, which is attributed to drug adsorption on the surface of the microspheres; thus, a greater number of microspheres per unit volume of cryogel correlates with increased drug adsorption.
Due to the pronounced “burst” effect (
Figure 9) [
65], which is observable within the first 6 h of release and attributed to the high solubility of the drug in water, and the presence of a network of interconnected macropores in cryogels, these materials may be particularly beneficial in scenarios requiring rapid drug delivery to the target.
2.5. Simvastatin Release
Simultaneously with the formation of PHB microspheres, simvastatin was introduced into the system at a concentration of 4.35 mg per gram of the polymer. Spectrophotometric monitoring of the process revealed that 1 g of dry MS-1 contained 3.76 ± 0.74 mg of simvastatin (~86%), while dry MS-2 contained 4.17 ± 0.57 mg (~96%). The observed loss of the drug compared to the initial amount is likely attributable to partial leaching during various process stages, such as preparation of the primary emulsion, solidification of PHB through chloroform evaporation from the microdroplet phase, and subsequent rinsing of the resultant microspheres with water. Reference samples of PVA cryogels without PHB microspheres were loaded with a comparable amount of simvastatin (~4.17 mg) by dissolving it in the initial aqueous solution of PVA.
The kinetics of simvastatin release from composite cryogels containing MS-1 and MS-2 was investigated using unfilled PVA cryogels as control samples (
Figure 10). The release profiles were analyzed using the Higuchi (2), Peppas–Korsmeyer (3), and zero-order models (7).
where t is time, M
t is the amount of drug released at the time t, M
∞ is the drug amount released at the infinite time, and k
0 is a constant of apparent velocity of dissolution [
61,
62].
The release profiles aligned more closely with the zero-order model (
Table 5), except for the first hours of the release, which exhibited a minor “burst” effect. This “burst” effect is likely attributable to the fact that during the preparation of microsphere suspensions in PVA solutions, some amount of simvastatin could diffuse into the cryogel matrix. In the case of unfilled cryogels, the “burst” effect is related to the reduction in the diffusion path that the compound must pass to exit the cryogel. High values of the R
2 coefficients obtained from the Higuchi model (
Table 5) indicate that the drug release process is primarily diffusion-based, adhering to Fick’s law. For all studied samples, n ≤ 0.45 (
Table 5) testifies that the release mechanism is predominantly governed by Fickian diffusion.
Using Equations (4) and (5), the diffusion coefficients of simvastatin were determined (the radius of the samples was 0.75 cm):
Unfilled PVA Cryogel | 2.58 × 10−8 cm2/s |
PVA cryogel filled with MS-1 particles | 4.24 × 10−8 cm2/s |
PVA cryogel filled with MS-2 particles | 1.85 × 10−8 cm2/s |
The data indicate that the release of simvastatin from both unfilled and composite PVA cryogels is characterized by a prolonged release profile, with no more than 30% of the substance released over a period of 350 h. The slowest release of simvastatin occurred from the samples containing MS-2. This difference in the kinetics of simvastatin release from samples with PHB microspheres of varying porosity can be explained by the necessity for drug molecules to diffuse through the microsphere phase first. In the case of MS-2, this process occurs at a significantly slower rate than with MS-1, as indirectly confirmed by the values of the kinetic constant K (
Table 5), which reflects the structural and geometric characteristics of the matrix as well as the release rate.
When dealing with simvastatin, which is poorly soluble in water, the absence of a pronounced “burst” effect is evident (
Figure 10), with approximately 5% of the drug being released in the first hours. Subsequently, the release profile is more consistent with a monophasic release for both unfilled cryogels and composite cryogels containing MS-2, suggesting that a steady-state concentration of the drug can be maintained within the therapeutic range over an extended duration.
It should be noted that that the degradation of PHB particles, which may influence simvastatin release, occurs over a significantly extended timeframe (~6–10 weeks) [
66]; by this point, the release of simvastatin is presumed to have ceased.
The reasons for the faster release of simvastatin from MS-1 cryogels compared to other samples remain to be elucidated, with further investigation necessary to uncover the precise mechanism.