Open Access Article
Ahmed M.
Agiba
a,
Luis Gerardo
Rodríguez Huerta
a,
Nicolás A.
Ulloa-Castillo
b,
Francisco J.
Sierra-Valdez
a,
Saeed
Beigi-Boroujeni
a,
Omar
Lozano
*cd and
Alan
Aguirre-Soto
*ab
aSchool of Engineering and Sciences, Tecnologico de Monterrey, Monterrey 64849, Nuevo León, Mexico. E-mail: alan.aguirre@tec.mx
bCenter for Innovation in Digital Technologies, School of Engineering and Sciences, Tecnologico de Monterrey, Monterrey 64849, Nuevo León, Mexico
cInstitute for Obesity Research, Tecnologico de Monterrey, Monterrey 64849, Nuevo León, Mexico. E-mail: omar.lozano@tec.mx
dSchool of Medicine and Health Sciences, Tecnologico de Monterrey, Monterrey 64849, Nuevo León, Mexico
First published on 26th December 2024
Liposomes are employed for the delivery of molecular cargo in several classes of systems. For instance, the embedding of loaded liposomes in polymeric fibrous scaffolds has enabled the creation of hybrid materials that mimic biological membranes. Liposomes with unmodified surfaces have been predominantly integrated into fibers, which leads to instabilities due to interfacial incompatibility. In addition, electrospinning has been almost exclusively employed for fiber fabrication, which limits the potential for scale-up production. Here, we present the fabrication of hybrid biomimetic materials by fusing polymer-coated liposomes to force-spun microfibers to increase the stability of the hybrid materials and enhance the sustained release of the cargo. L-α-Phosphatidylcholine liposomes were coated with chitosan or polyethylene glycol (PEG). The nano-differential scanning calorimetry results confirm that polymer coating does not affect the phase transition temperature (Tm) of the liposomes, where only the model drug, quercetin, reduced Tm. Centrifugal spinning was employed to fabricate hydrophobic polycaprolactone (PCL) microfibers at various polymer concentrations and using various solvents and spinning parameters to increase the yield at the lowest fiber diameter. The highest microfiber production rate obtained occurred at a 20% (w/v) PCL concentration in 50
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50 (v/v) chloroform and methanol solution with an average fiber diameter of 584.85 ± 26.30 nm. The non-chemical fusion of the polymer-coated liposomes and the fibrous scaffolds was promoted by immersion at T > Tm, under ultrasonication. We hypothesize that the fusion is driven by hydrophobic interactions between the liposomes and the fibers, which merge the materials through the lipid bilayer. The fused hybrid material solved the burst release problem observed when adhering plain liposomes to nanofibers. Both PEG and chitosan yielded a sustained release, where the release rate with the former was faster. These results demonstrate that the fusion of polymer-coated liposomes and microfibers enables more effective blending of the loaded carriers into the polymer microfibers. Ultimately, the fused liposome/microfiber hybrids are stable matrices and enhance the sustained release of molecular cargo.
On the other hand, polymeric fibers with nano- and micro-scale size features have been used as delivery systems on their own by loading molecular cargo into their porous structure, Fig. 1a.3 Their tunable porosity, high surface-to-volume ratio, and release rates make them interesting alternatives for molecular release. Three fiber production techniques are available, namely, electrospinning, centrifugal, and electro-centrifugal spinning.4 Electrospinning is the oldest and most widely used technique, based on the electrostatic pulling of polymers out from solution. Centrifugal spinning enables the high-throughput production of polymeric fibrous scaffolds or mats through the application of centrifugal forces, as depicted in Fig. 1b. The fiber production rates with centrifugal spinning exceed 1 g min−1, which is significantly higher than that of equivalent electrospinning devices, 0.1 g min−1.5 Moreover, centrifugal spinning enables the production of high-quality fibrous mats from either polymeric solutions or melts, as well as from conductive and non-conductive polymers.6,7 The surface morphology and the mechanical properties of the obtained fibers are determined by the polymer viscoelasticity, solvent surface tension, solvent evaporation rate, spinneret angular velocity and aspect ratio, spinneret orifice distance to the collector, orifice radius and orientation, and solvent fill volume.4,5 Fibers produced by electrospinning or centrifugal spinning have both been reported to be directly loaded with molecular cargo during and after the spinning process. Utilizing the porosity and swelling of the polymer materials, molecules have been embedded within the fibers for the subsequent release. Nevertheless, the release kinetics profiles obtained with these approaches are generally limited to relatively short dose periods for a small set of molecular cargo chemistries.
The loading of liposomes into fibrous scaffolds has been exploited to combine the benefits of both the liposomal and polymer carriers (Fig. 1a).8 Most reports describe the combination of plain liposomes and electrospinning, where the lipids are dissolved along with the polymers before the application of the electromagnetic field. However, liposome loading into fibers is challenged by aggregation, degradation, hydrolysis, and phospholipid oxidation.9–11 These challenges have been tackled to some extent through optimization of the lipid-to-polymer ratio and the spinning parameters. In contrast, only one study was found on the use of centrifugal spinning for fiber fabrication and subsequent adhesion of liposomes for the release of molecular cargo. Rampichová et al. prepared fibrous scaffolds of polycaprolactone (PCL) by centrifugal spinning with adhered liposomes.12 The problem is that the authors documented an uncontrolled burst release (∼15 min) of the incorporated molecule. Further work was suggested to fabricate more stable materials that can sustain the release of cargo at a constant rate for longer.
In this work, we present the fusion of polymer-coated liposomes with polymeric fibrous scaffolds (Fig. 1b) through a scalable procedure that merges centrifugal spinning and fiber immersion (Fig. 1c). We propose that the fusion of the polymer-coated liposomes and the microfibers is driven by hydrophobic forces during immersion of both materials under ultrasound at a temperature over the phase transition temperature of the liposomes. No reports were found on the combination of fibers fabricated by centrifugal spinning with polymer-coated liposomes. Liposomes conformed by L-α-phosphatidylcholine (PC) vesicles and cholesterol are loaded with quercetin (QR) as a model hydrophobic drug and cetyltrimethylammonium bromide (CTAB) as a bioenhancer. Loaded liposomes were coated with chitosan or polyethylene glycol. The polymer-coated liposomes are intended to stabilize the lipid bilayer during fusion with hydrophobic PCL microfibers. The hybrid materials were characterized, and their drug release kinetics were compared against plain and coated liposomes. QR is a naturally occurring antioxidant flavonoid with a variety of biological activities, including anticancer, anti-inflammatory, cardiovascular disease prevention, and hepatoprotective activity.13 However, the therapeutic use of QR is limited due to its poor aqueous solubility, chemical instability, and low bioavailability, which greatly restricts its therapeutic potential as a functional active ingredient.14 Encapsulating phytochemicals in liposomes remains cumbersome.15 Therefore, the hybrid materials presented here are proposed as a framework for the encapsulation and subsequent sustained release of challenging molecular cargo via a scalable fabrication process.
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1 (v/v) mixture of chloroform and methanol in a 500 mL rotary evaporator round-bottom flask containing 150 mg of QR (Table S1 and Fig. S1†). The organic phase was slowly removed in a rotary evaporator (Witeg Labortechnik GmbH, Germany) at 40 °C and 150 rpm, and a thin lipid film was formed on the flask inner surface. The dry lipid film was hydrated with 15 mL of purified water at 40 °C containing the CTAB bioenhancer for 45 minutes. The resulting liposomes were sequentially placed in an ultrasonic bath (Branson CPX-952-238R, Branson Ultrasonics Corp., USA) for 2 hours and then stored in 30 mL amber-colored glass bottles sealed with parafilm in a refrigerator at 2–8 °C for overnight maturation.
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1), and mechanically stirred at 10
000 rpm for 30 minutes.17 The coated liposomes were then placed in an ultrasonic bath for 5 minutes and then stored in 30 mL amber-colored glass bottles sealed with parafilm in the refrigerator at 2–8 °C until further use.
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50 (v/v) mixture of chloroform and methanol stirred for 2 hours (Table S1†). Solutions were stored at room temperature until further use. Two milliliters of the PCL solution were injected into a dual-orifice spinneret of a Forcespinning® FiberLab L1000 (FibeRio Technology Corporation, USA) instrument equipped with two disposable needles (BD Precision Glide, 30 G × 1/2) and rotated at 9000 rpm for 50 seconds. The temperature and relative humidity were set to be 34 °C and 37–41%, respectively.
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20 (v/v) ratio and measured in a zeta cell. The viscosity was measured using a digital viscometer (Brookfield DV-II + PRO, Brookfield Engineering Laboratories, Inc., USA) using spindle 61 (LV1) at 60 rpm and 37 °C.
000 rpm for 30 minutes. The supernatant was filtered through a 0.22 μm pore-size nylon syringe filter (Thermo Fisher Scientific, USA) and analyzed for the free drug, in which the concentration of QR was determined using a UV-Vis spectrophotometer (Cary 7000, Agilent Technologies, Santa Clara, CA, USA). The calibration is detailed in Table S2 and Fig. S2† for the calculation of entrapment efficiency (EE%) and drug loading capacity (LC%).
An EE% of 96.82 ± 0.007% was obtained with the chitosan-coated liposomes. In contrast, 96.39 ± 0.002% of the quercetin was encapsulated with the PEG-coated liposomes. The LC% was 9.381 ± 0.01% and 8.794 ± 0.003% for the chitosan and PEG coatings, as shown in Fig. S3a and Table S3.† Despite the high drug entrapment efficiency, the loading capacity of liposomes was limited because it depends on the drug/lipid ratio and the available space in the lipid bilayer.26
The key challenge with liposome stability is liposome aggregation, a sign of low physical stability during storage. Following 3 months of storage at 2–8 °C, the coated liposomes showed good colloidal stability, as indicated by negligible variations (p < 0.05) in zeta potential, PDI, and particle size (Table S3†). This is explained by the high concentration of cholesterol in liposomes, which improves the integrity of the liposomal membrane and serves as a stabilizer.
To further evaluate the stability of the lipid bilayer as a function of the molecular cargo and polymer coating, thermograms were obtained for each liposomal suspension as shown in Fig. 2. L-α-PC exhibited a wide and bimodal gel-liquid thermogram. However, the addition of cholesterol to the liposomes (LP) caused a slight shift to higher temperatures, indicating increased lateral cohesion and stability of the lipid bilayer, as in biological membranes.27 Cholesterol preserved the bimodal phase transition, suggesting the absence of lipid remodeling. In contrast, when QR was anchored into the lipid bilayer, it weakened lipid-to-lipid interactions, as evidenced by the gel-liquid phase transition shifting to lower temperatures.28 Furthermore, the unimodal phase transition peak demonstrated that QR caused a homogeneous distribution of lipid species. Moreover, PC/Chol/QR/CTAB showed that the CTAB bioenhancer was encapsulated by liposomes without affecting their structural stability. The characterization of the Tm of modified and loaded liposomal suspensions is frequently absent in previous publications on the fabrication of complex materials for molecular release. In this work, these results are important as they confirm that the final liposomal suspensions were in a fluidized phase at room temperature, which will facilitate their fusion into the PCL fibers.
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50 (v/v) methanol/chloroform solvent produced uniformly sized, small-diameter bead-free microfibers, as shown in Table S4.† The production of PCL fibers was performed using various spinning parameters: spinneret velocity (5000–9000 rpm) and spinning time (50–150 seconds). No fibers were produced below 5000 rpm within 50–150 seconds because these rotational speeds were insufficient to eject all the polymeric solution from the spinneret, resulting in no fiber formation. However, at 7000 rpm for 50 seconds, a low yield of fibers with many beads was produced. As the spinneret velocity increased to 8000 rpm, the fiber production rate increased. However, some beading of the fibers was still observed. By increasing the spinneret velocity to 9000 rpm for 50 seconds, bead-free microfibers with a uniform size distribution were obtained. This rotational speed resulted in continuous PCL microfibers. Thus, a spinneret velocity of 9000 rpm and a spinning time of 50 seconds were selected as optimal operating conditions for producing homogeneous forcespun PCL microfibers with uniform diameters.
O aryl ketonic stretch absorption was detectable at 1666 cm−1. The C
C aromatic ring stretch bands were detectable at 1610, 1560, and 1510 cm−1. The in-plane bending band of C–H in the aromatic hydrocarbon was detectable at 1317 cm−1, and out-of-plane bending bands were detectable at 933, 820, and 600 cm−1. The peaks at 1263, 1200, and 1165 cm−1 were assigned to the C–O stretching in the aryl ether ring, the C–O stretching in phenol, and the C–CO–C stretch and bending in ketone, respectively.30 The characteristic peak in the FT-IR spectra of chitosan (Fig. S4c†) is 3447 cm−1, which was attributed to NH2 and OH groups stretching vibration. The peaks at 1657 and 1598 cm−1 were linked to the CONH2 and NH2 groups, respectively. The PEG absorption bands are shown in Fig. S4d:† 958 cm−1 and 2880 cm−1, which were attributed to the C–H and CH2 groups, respectively. The triplet at 1150 cm−1, 1110 cm−1, and 1060 cm−1 is assigned to the C–O–C groups.31 The spectra of L-α-PC contain characteristic peaks at 2930 cm−1 (CH2 stretching), 1737 cm−1 (C
O stretching), and 1461 cm−1 (C–H bending of CH3), Fig. S4e.† Peaks at 3394 cm−1 (O–H stretching); 2930 cm−1 (CH2 stretching); 1463 cm−1 (C–C aromatic stretching) and 1365 cm−1 (C–O stretching) were confirmed for cholesterol-containing samples. The FT-IR spectra of CTAB showed a characteristic peak at 3335 cm−1 for stretching vibrations of the ammonium group in CTAB. The peaks at 2930 cm−1 and 2854 cm−1 were attributable to two different C–H band vibrations of the CH2 group in CTAB.32 For the polymer-coated liposomes, the main functional peaks of chitosan and PEG-4000 were observed in the FT-IR spectra.
To identify the chemical interaction between liposomes and microfibers, the FT-IR spectra of QR- and CTAB-co-loaded liposomes and the fused liposome/microfiber constructs were compared, as shown in Fig. S4f.† The FT-IR spectra of PCL showed characteristic peaks at 2951 cm−1 and 2866 cm−1, which were attributed to C–H stretching; 1725 cm−1, which was attributed to C
O stretching vibration; and 1158 cm−1, which was attributed to C–O–C stretching vibration. There was no difference in PCL in the solid and fiber states. The main functional peaks of plain liposomes, chitosan, PEG-4000, and PCL were observed in the FT-IR spectra of the hybrid materials.
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| Fig. 4 TGA curves of plain fibers against the chitosan and polyethylene glycol (PEG) containing hybrid materials. | ||
To further understand the drug release mechanisms of polymer-coated liposomes, drug release data were analyzed using the Korsmeyer–Peppas kinetic model (Table S6†). The chitosan-coated liposomes yielded a release equation where n = 0.585, K = 5.587, and R2 = 0.930, indicating that the release mechanism follows anomalous (non-Fickian) diffusion, which is a combination of both diffusion and erosion mechanisms. In contrast, the equation for the release with the PEG-coated liposomes follows n = 0.802, K = 4.465, and R2 = 0.981, indicating that the release mechanism is near-zero-order release (case-II transport), implying that the drug is released primarily through swelling and erosion mechanisms. Thus, the PEG-coated liposome showed a better controlled release profile than the chitosan-coated liposome, as ideal controlled release systems frequently aim for zero-order release.35
The drug release from the liposome/microfiber hybrids was evaluated in PBS of pH 7.2 at 37 °C. Both hybrid materials showed lower drug release rates as compared to the coated liposomes alone, which is expected from the additional diffusional barrier. Notably, the liposome/microfiber hybrids displayed a gradual and prolonged drug release for 120 hours. The total amount of QR released after 120 hours of drug release was 42.656 ± 4.07% for the hybrid material with chitosan and 80.405 ± 3.67% for the hybrid material with PEG (Fig. 5).
To understand the drug release kinetics of liposome/microfiber hybrids, data obtained from drug release testing were analyzed using zero-order release kinetics, the Higuchi square release model, and the Korsmeyer–Peppas kinetic model. The hybrid materials follow zero-order release, with R2 values equal to 0.9966 and 0.9954 for chitosan- and PEG- containing hybrids, respectively. The release from the chitosan-containing hybrid follows n = 1.205, K = 0.134, and R2 = 0.999, indicating that the release mechanism is a pure super case-II transport mechanism due to the erosion of the polymeric fibrous structure.36 Similarly, the release from the PEG-containing hybrid was fitted to n = 1.178, K = 0.284, and R2 = 0.994, indicating that the release mechanism is also a pure super case-II transport mechanism in which the drug release from the hybrid is controlled by the erosion of the polymeric fibrous structure (Table 1).37,38 Overall, the PEG-coated liposome exhibited a near-zero-order controlled release, whereas the PEG-containing hybrids follow Higuchi release. The addition of the liposomes into the microfibers increased controlled release characteristics, resulting in zero-order release profiles and a super case-II transport mechanism.
| Formula code | Linear fit | R 2 | K | SSD | n |
|---|---|---|---|---|---|
| a Coefficient of determination (R2); rate constant (K); sum of the squared difference (SSD); release exponent (n). n ≤ 0.45: Fickian diffusion (case-I transport); 0.45 < n < 0.89: anomalous (non-Fickian) diffusion; n ≃ 0.89: zero-order release (case-II transport); n > 0.89: super case-II transport. | |||||
| LP–QR–CTAB–CH–NF | y = 1.19x − 0.85 | 0.999 | 0.134 | 0.806 | 1.205 |
| LP–QR–CTAB–PEG–NF | y = 1.33x − 0.84 | 0.994 | 25.338 | 105.248 | 1.178 |
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50 (v/v) solvent mixture of methanol and chloroform. The average fiber diameter was 584.85 ± 26.30 nm, which was adequate for loading the coated liposomes. Nano-DSC and SEM support that liposomes were adequate to fuse into the microfibrous scaffold. The total amount of QR released after 120 hours of drug release was 42.656 ± 4.07% and 80.405 ± 3.67% for the chitosan- and PEG-containing hybrid materials, respectively. Their release mechanism is a pure super case-II transport mechanism in which the drug release from the hybrid materials is controlled by the erosion and swelling of the polymeric microfibers. These findings demonstrate that liposome/microfiber hybrid materials produced through a scalable process can outperform plain liposomes in terms of stability and sustained release.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4na00835a |
| This journal is © The Royal Society of Chemistry 2025 |