Abstract
It is difficult to fabricate chitosan-wrapped coaxial nanofibers, because highly viscous chitosan solutions might hinder the manufacturing process. To overcome this difficulty, our newly developed method, which included the addition of a small amount of gum arabic, was utilized to prepare much less viscous chitosan solutions. In this way, coaxial polyvinyl alcohol (PVA)/chitosan (as core/shell) nanofiber membranes were fabricated successfully by coaxial electrospinning. The core/shell structures were confirmed by TEM, and the existence of PVA and chitosan was also verified using FT-IR and TGA. The tensile strength of the nanofiber membranes was increased from 0.6-0.7 MPa to 0.8-0.9 MPa after being crosslinked with glutaraldehyde. The application potential of the PVA/chitosan nanofiber membranes was tested in drug release experiments by loading the core (PVA) with theophylline as a model drug. The use of the coaxial PVA/chitosan nanofiber membranes in drug release extended the release time of theophylline from 5 minutes to 24 hours. Further, the release mechanisms could be described by the Korsmeyer-Peppas model. In summary, by combining the advantages of PVA and chitosan (good mechanical strength and good biocompatibility respectively), the coaxial PVA/chitosan nanofiber membranes are potential biomaterials for various biomedical applications.
1 Introduction
Electrospinning is a commonly used technology to obtain polymer nanofibers with diameters in the range of several nanometers to micrometers [1, 2, 3, 4]. During the electrospinning process electrostatic repulsion is used to overcome the surface tension of a solution droplet at the needle tip, thus stretching the droplet to form a jet, which dries while flying toward a collector, to produce nanofibers [5]. The accumulation of electrospun nanofibers forms a membrane with high porosity and specific surface area. This membrane is suitable for use in tissue engineering, drug release and separation process [6]. Coaxial electrospinning is a modified electrospinning method which uses a blunt-tip coaxial needle to extrude core and shell solutions without mixing during electrospinning, thus producing nanofibers with a core/shell structure [7, 8, 9, 10]. There are several advantages associated with the core/shell structure. For example, by using a material easy to be electrospun as core layer, another material, which cannot be electrospun alone, may have a chance to be spun successfully as shell layer. On the other hand, if the core layer contains drugs, the outer shell layer can act as a barrier to give a slow and sustained drug release. Furthermore, the mechanical properties of the coaxial nanofibers can be improved by choosing a material with good strength as the core layer. Therefore, in the application of tissue engineering, natural materials with good biocompatibility can be used as shell layer material to wrap the core material with low biocompatibility but good mechanical strength, thus generating biocompatible coaxial nanofibers that also possess suitable strength.
In the present study, polyvinyl alcohol (PVA) and chitosan were selected as major core and shell materials, respectively. PVA is a water-soluble polymer that can be used as an excipient for drug delivery. PVA is also a material easy to be electrospun and thus can be used as core material for coaxial electrospinning [11, 12]. Chitosan is a natural basic polysaccharide composed of glucosamine and N-acetyl glucosamine [13]. It has been used in drug delivery, tissue engineering, and other biomedical applications because it is biocompatible, biodegradable and antimicrobial. Chitosan is soluble in acidic solution but the chitosan solution becomes highly viscous when its concentration goes high, making the preparation of chitosan nanofibers by electrospinning quite problematic. To overcome this difficulty, chitosan has to dissolve in high concentration of acetic acid or organic solvents such as trifluotoacetic acid (TFA) and hexafluoroisopropanol (HFIP) [14, 15, 16]. However, TFA and HFIP are highly corrosive and expensive. To prevent the use of TFA and HFIP, we employed our newly developed method (i.e., the addition of gum arabic) to prepare a solution with a high chitosan content but a much lower viscosity, thus making the electrospinning process feasible [17, 18]. Gum arabic is a branched biopolymer. In our previous research, we found that gum arabic can interact with chitosan to form globe-like microstructures and thus remarkably decrease the viscosity of the resulting chitosan solution [19].
Similarly, this research demonstrated that the addition of a small amount of gum arabic significantly decreased the viscosity of chitosan solutions even though chitosan was dissolved in a mild (5 wt%) aqueous acetic acid solution. The chitosan solution thus prepared was then used as the shell solution in the coaxial electrospinning while the PVA solution was selected as the core solution. The parameters affecting the electrospinning process such as the flow rates and compositions of core and shell solutions were optimized. The mechanical properties and the application of the coaxial PVA/chitosan nanofiber membranes were also investigated.
2 Materials and methods
2.1 Materials
Chitosan (molecular weight: about 300 kDa; degree of deacetylation: about 90%) was purchased from Kiotek Co. (Taipei, Taiwan). Polyvinyl alcohol (PVA) (degree of hydrolysis: 98.5-99.2%) was supplied by Chang Chun Petrochemical Co. Ltd (Taiwan). Gum arabic, acetic acid and other chemicals of reagent grade were purchased from Sigma-Aldrich (St. Louis, MO, USA).
2.2 Preparation of solutions
The abbreviations and compositions of various PVA and chitosan solutions prepared in this study are shown in Table 1. PVA solutions were prepared by dissolving PVA in 90 °C water. 8, 10 and 12 wt% PVA solutions were prepared and designated as P8, P10 and P12, respectively. The preparation of chitosan solutions suitable for electrospinning was carried out by using our newly developed method [17, 18, 19]. Our method included the addition of a small amount of gum arabic (10 wt% of chitosan) that significantly decreased the viscosity of chitosan solutions when using a mild aqueous acetic acid solution as a solvent. To prepare various chitosan solutions, chitosan powder was dissolved in acetic acid solution, and then gum arabic (10 wt% of chitosan) was added into the solution to greatly decrease the viscosity of chitosan solution. 4, 6, 8, 10 and 12 wt% chitosan solutions (containing gum arabic) were prepared using 5, 10 or 20 wt% aqueous acetic acid solution as a solvent. These chitosan solutions were designated as Cm-n (m representing the concentration of chitosan and n representing the concentration of acetic acid). For example, C4-5 represents a chitosan solution containing 4wt% chitosan, 0.4wt% gum arabic and 5 wt% acetic acid.
The abbreviations and compositions of various PVA and chitosan solutions
Composition (wt%) | ||||||
---|---|---|---|---|---|---|
Abbreviation | ||||||
Chitosan | Gum arabic | Acetic acid | PVA | H2O | ||
PVA solutions | P8 | - | - | - | 8 | 92 |
P10 | - | - | - | 10 | 90 | |
P12 | - | - | - | 12 | 88 | |
P10-20 | - | - | 20 | 10 | 70 | |
Chitosan solutions | C4-5 | 4 | 0.4 | 5 | - | 90.6 |
C6-5 | 6 | 0.6 | 5 | - | 88.4 | |
C8-5 | 8 | 0.8 | 5 | - | 86.2 | |
C10-5 | 10 | 1.0 | 5 | - | 84.0 | |
C12-5 | 12 | 1.2 | 5 | - | 81.8 | |
C4-10 | 4 | 0.4 | 10 | - | 85.6 | |
C6-10 | 6 | 0.6 | 10 | - | 83.4 | |
C8-10 | 8 | 0.8 | 10 | - | 81.2 | |
C1O-10 | 10 | 1.0 | 10 | - | 79.0 | |
C12-10 | 12 | 1.2 | 10 | - | 76.8 | |
C4-20 | 4 | 0.4 | 20 | - | 75.6 | |
C6-20 | 6 | 0.6 | 20 | - | 73.4 | |
C8-20 | 8 | 0.8 | 20 | - | 71.2 | |
C1O-20 | 10 | 1.0 | 20 | - | 69.0 | |
C12-20 | 12 | 1.2 | 20 | - | 66.8 |
2.3 Characterization of solutions
A pH meter (model 420A, Orion, USA) was used to determine the pH of various solutions. The viscosity of various solutions was measured by a viscometer (model DV-II+, Brookfield, USA), and the rotation speed of spindle was fixed at 2 rpm. The conductivity and surface tension of various solutions were also measured by using a conductivity meter (model COND6 plus, Eutech, Singapore) and a tesiometer (model 514-B, Itoh Seisakusho, Japan), respectively.
2.4 Coaxial electrospinning of solutions
Coaxial electrospun nanofibers with core/shell structures were fabricated by using an electrospinning unit (Jyi-Goang Enterprise, Taipei, Taiwan). The blunt-tip coaxial needle was composed of a 23G (i.d. 0.33 mm, o.d. 0.63 mm) inner needle concentrically mounted on an 18G (i.d. 0.96 mm, o.d. 1.26 mm) outer needle. PVA and chitosan solutions were loaded in two individual syringes and fed by two separate syringe pumps. The applied voltage and working distance between needle tip and collector were 25 KV and 15 cm, respectively. The environmental temperature and relative humidity were controlled at 32 °C and 40-50%.
2.5 Analysis of coaxial nanofibers
A scanning electron microscope (SEM, JSM-5310, Jeol, Japan) and a transmission electron microscope (TEM, JEM-1230, Jeol, Japan) were used to observe the morphology of coaxial nanofibers. Fourier transform infrared spectroscopy (FT-IR) analysis was carried out using an FT-IR spectrometer (Spectrum One, Perkin-Elmer, USA).
Thermal behavior of various samples was investigated by a thermogravimetric analysis meter (TGA, model Pyris 1, Perkin-Elmer, USA). For TGA analysis, about 5 mg sample was hold at 50 °C for 20 min to remove residual water in the sample, and then was heated from 50 °C to 600 °C at a rate of 10 °C/min. The process of TGA analysis was under continuous nitrogen purge at a rate of 20 ml/min.
2.6 Mechanical properties of coaxial nanofiber membranes
To analyze mechanical properties of nanofiber membranes, the membranes were cut into a dumbbell shape, and the thicknesses of membranes were measured with a micrometer. The mechanical properties including tensile strength (stress at maximum load) and elongation (strain at maximum load) were measured with a tensile strength instrument (model LRX, Lloyd, Hampshire, UK). The stretching rate of the measurement was 10 mm/min.
2.7 Drug release experiments
The application potential of the PVA/chitosan coaxial nanofiber membranes was tested in drug release experiments when the core (PVA) was loaded with theophylline (5 mg/ml) as a model drug. For comparison purposes, conventional (non-coaxial) PVA nanofiber membranes were also fabricated and used as controls. The theophylline containing nanofiber membranes were crosslinked with glutaraldehyde vapor for 8 hours, followed by drying in a vacuum oven for 12 hours. The drug release experiments were carried out by immersing the nanofiber membranes in phosphate-buffered saline (PBS). PBS samples (1 ml) were withdrawn periodically at predetermined time intervals and the theophylline concentrations in the PBS samples were determined using a spectrophotometer (model U-2001, Hitachi, Japan) at 274 nm. The “percentage of drug released” was calculated using the following formula:
Since theophylline was initially present in the core (PVA), the shell (chitosan) acted as a barrier to the release of theophylline. It was expected that the use of drug-loaded coaxial nanofiber membranes would give a gradual and sustained drug release. However, several phenomena such as nanofiber swelling, disintegration, and drug diffusion were involved in the release of theophylline. To investigate these anomalous transport phenomena, a semi-empirical model called “Korsmeyer-Peppas model” was utilized to correlate the theophylline release from the coaxial nanofiber membranes because the above-mentioned anomalous phenomena were considered in this model, as shown below [20, 21, 22]:
where Mt is the cumulative amount of drug at any time t, M∞ is the cumulative amount of drug at the last time of the measurement, k is the release rate constant, and n is the release exponent. To obtain the parameters of release kinetics (k and n), data obtained from drug release experiments were plotted as log percentage of drug released vs. log time [21, 23].
3 Results and discussion
3.1 Properties of PVA and chitosan solutions
To search for polymer solutions suitable for electrospinning, the pH, surface tension and conductivity of various PVA and chitosan solutions were determined, as shown in Table 2. The pH of PVA solutions slightly decreased as the concentration of PVA increased, probably due to the residual acetyl groups in PVA that might be hydrolyzed to yield acetic acid. On the other hand, since chitosan is a basic polysaccharide, increasing the concentration of chitosan elevated the pH of chitosan solutions (containing chitosan, gum Arabic, and acetic acid) (Table 2).
The pH, surface tension and conductivity of various PVA and chitosan solutions
Sample | pH | Surface tension (mN/m) | Conductivity (S/m) | |
---|---|---|---|---|
PVA solutions | P8 | 6.01 | 51.43±1.10 | 0.065±0.000 |
P10 | 5.95 | 50.13±0.77 | 0.074±0.000 | |
P12 | 5.74 | 48.15±0.29 | 0.083±0.000 | |
Chitosan solutions | C4-5 | 3.29 | 44.82±0.44 | 0.543±0.001 |
C6-5 | 3.45 | 44.67±1.33 | 0.731±0.001 | |
C8-5 | 3.91 | 44.55±0.63 | 0.921±0.002 | |
C10-5 | 4.17 | 43.36±0.35 | 1.002±0.001 | |
C12-5 | 4.63 | 42.30±0.21 | 1.150±0.002 | |
C4-10 | 3.19 | 43.11±0.66 | 0.545±0.000 | |
C6-10 | 3.39 | 42.69±0.27 | 0.717±0.001 | |
C8-10 | 3.61 | 42.03±0.44 | 0.870±0.001 | |
C10-10 | 3.72 | 41.44±0.21 | 0.937±0.001 | |
C12-10 | 4.00 | 40.72±0.96 | 1.060±0.002 | |
C4-20 | 2.65 | 38.37±1.47 | 0.460±0.001 | |
C6-20 | 2.82 | 36.96±0.95 | 0.606±0.002 | |
C8-20 | 3.07 | 35.66±0.84 | 0.746±0.001 | |
C10-20 | 3.12 | 34.70±0.20 | 0.854±0.003 | |
C12-20 | 3.21 | 33.57±0.74 | 0.895±0.004 |
During the electrospinning process electrostatic repulsion is used to overcome the surface tension of a solution droplet at the needle tip [24], suggesting that both surface tension and conductivity may influence the morphology of nanofibers. As shown in Table 2, surface tension of various PVA and chitosan solutions decreased while the concentrations of PVA and chitosan increased. The use of acetic acid solution at higher concentrations also decreased the surface tension of chitosan solutions, since the surface tension of pure acetic acid (27.08 mN/m) [25] is lower than that of pure water (71.97 mN/m). As for theconductivity of solutions, increasing the concentrations of PVA and chitosan improved the conductivity of solutions, especially for chitosan (Table 2). Since PVA is a relatively neutral polymer, however, chitosan is a basic polysaccharide which contains positive charge in an acidic solution, thus enhancing the conductivity of solutions.
The viscosity of polymer solutions plays an important role in electrospinning. A low-viscosity polymer solution implies less entanglement of polymer chains in the solution which may lead to poor electrospinning, resulting in the formation of beads or spindle-like structures. However, if solution viscosity is too high, the solution will become too sticky to be electrospun. Figure 1 shows the influence of concentration on the viscosity of PVA and chitosan solutions. As shown in Figure 1(a), the viscosity of PVA solutions increased as the concentration of PVA increased, possibly due to more entanglement of polymer chains. Figure 1(b) shows a similar trend for chitosan solutions. It should be noted that without the addition of gum arabic in chitosan solution, the viscosity of chitosan solution dramatically increased when the concentration of chitosan solution increased to 8 wt% (hollow symbols in Figure 1(b)). Therefore, the preparation of high-content (10-12 wt%) chitosan solutions would be impossible unless using our newly developed method, i.e., the addition of a small amount of gum arabic (10 wt% of chitosan) to greatly decrease the viscosity of chitosan solutions (solid symbols in Figure 1(b)) [17, 18]. Gum arabic is a branched biopolymer. In our previous research, we found that gum arabic can interact with chitosan to form globe-like microstructures and thus remarkably decrease the viscosity of the resulting chitosan solution [19]. As a result, the use of our newly developed method (i.e., the addition of gum arabic) to prepare a chitosan solution with a high chitosan content (up to 12 wt%) but a much lower viscosity made the following electrospinning process feasible. Figure 1(b) also shows that the viscosity of chitosan solutions can be further lowered by decreasing the concentration of acetic acid from 20 to 5 wt%.

Viscosity of: (a) PVA solutions, (b) chitosan solutions, prepared as shown in Table 1. Chitosan was dissolved in 5 wt%, 10 wt%, or 20 wt% aqueous acetic acid solutions containing gum arabic (solid symbols). For comparison, the viscosity of chitosan solutions without gum arabic (hollow symbols) was also measured.
3.2 Influence of process parameters
Process parameters affecting the coaxial electrospinning such as the flow rates and compositions of core and shell solutions were investigated and optimized.
3.2.1 Flow rate ratio of core and shell solutions
Figure 2 shows the SEM images of coaxial PVA/chitosan (P10/C8-20 as core/shell) nanofibers prepared under different flow rate ratios of core and shell solutions. Nanofibers with better morphology were found when flow rate ratios of core:shell solutions were 0.15:0.15 and 0.15:0.3 (mL/h). Further increase in the flow rate of shell (chitosan) solution might interrupt the formation of PVA nanofibers. Repeating the experiment indicated that the best flow rate ratio of core:shell solution was 0.15:0.15 (mL/h) which was then utilized to carry out the following experiments.

SEM images of coaxial PVA/chitosan (P10/C8-20 as core/shell) nanofibers prepared under the same core flow rate (0.15 mL/h) but different shell flow rates (0.15-0.9 mL/h). Flow rates are designated on the top of each image by “core: shell” flow rates (mL/h). (Scale bar = 60 μm)
3.2.2 Composition of core (PVA) solution
Figure 3(a) shows the SEM images of coaxial PVA/chitosan nanofibers prepared using different core (PVA) solutions (P8, P10, P12) but the same shell solution (C8-20). No nanofibers were found in P8/C8-20 group since the viscosity of P8 solution was too low to form nanofibers (see Figure 1(a)). Few nanofibers were found in P12/C8-20 group since the viscosity of P12 solution was slightly too high and thus not favorable for nanofiber formation. In contrast, more nanofibers were found in P10/C8-20 group and thus P10 was selected as the composition of core solution for coaxial electrospinning in this research.

SEM images of coaxial PVA/chitosan (as core/shell) nanofibers prepared using: (a) different core solutions but the same shell solution (C8-20), (b) the same core solution (P10) but different shell solutions. The core and shell flow rates were the same (0.15 mL/h). (Scale bar = 60 μm)
3.2.3 Composition of shell (chitosan) solution
Figure 3(b) shows the SEM images of coaxial PVA/chitosan nanofibers prepared using the same core solution (P10) but different shell solutions (C4-20, C6-20, C8-20, C10-20, C12-20). Few nanofibers were found in P10/C10-20 and P10/C12-20 groups since the viscosity of C10-20 and C12-20 solutions was quite high and thus not favorable for nanofiber formation. In contrast, more nanofibers were found in P10/C4-20, P10/C6-20, and P10/C8-20 groups and thus these three groups were selected as the compositions of shell solutions for further investigation.
3.2.4 Concentration of acetic acid
One of the parameters affecting electrospinning is the solvent utilized to prepare a polymer solution [26]. It was found that better coaxial nanofibers were obtained when the solvent of core solution was more similar to the solvent of shell solution [27]. So far the solvents of core (PVA) and shell (chitosan) solutions were water and 20 wt% aqueous acetic acid solution, respectively. In order to make these two solvents more similar to each other, two methods were considered. The first method was to replace the solvent of core solution by 20 wt% aqueous acetic acid solution. The second method was to replace the solvent of shell solution by water, but it was unfeasible because chitosan was water-insoluble. The alternative method was to use acetic acid solution at lower concentration (5 or 10 wt%) as the solvent of shell solution.
About the first method, Figure 4(a) shows the SEM images of coaxial PVA/chitosan nanofibers obtained when the solvents of core and shell solutions were the same (20 wt% aqueous acetic acid solution). However, very few nanofibers were found in these groups (P10-20/C4-20, P10-20/C6-20 and P10-20/C8-20), indicating that acetic acid solution might not be a suitable solvent for PVA.

SEM images of coaxial PVA/chitosan (as core/shell) nanofibers prepared using: (a) the same core solution (P10-20) but different shell solutions, (b) the same core solution (P10) but different shell solutions. The core and shell flow rates were the same (0.15 mL/h). (Scale bar = 60 μm)
About the second method, Figure 4(b) shows the SEM images of coaxial PVA/chitosan nanofibers obtained when acetic acid solution at lower concentration (5 or 10 wt%) was utilized as the solvent of shell (chitosan) solution. When the concentration of acetic acid decreased to 10 wt%, nanofibers were found only in P10/C8-10 group (see the second row in Figure 4(b)). When the concentration of acetic acid decreased further to 5 wt%, nanofibers were found in P10/C8-5 and P10/C10-5 groups (see the third row in Figure 4(b)). In comparison with the results of nanofibers obtained using 20 wt% acetic acid solution as the solvent of shell solution (see the first row in Figure 4(b)), a similar amount of nanofibers but less beads and spindle-like structures were found when using 5 wt% acetic acid solution as the solvent. Hence, P10/C8-5 and P10/C10-5 groups were selected for further investigation.
3.3 Characteristics of coaxial PVA/chitosan nanofibers
Figure 5 shows the TEM images of various coaxial PVA/chitosan (as core/shell) nanofibers. The coaxial structures of electrospun nanofibers can be found in all five groups. However, among these chitosan-wrapped coaxial nanofibers better coverage of chitosan was present in P10/C8-5 group.

TEM images of various coaxial PVA/chitosan (as core/shell) nanofibers. (Scale bar = 0.1 μm)
To confirm the existence of PVA and chitosan, FT-IR analysis was carried out, as shown in Figure 6. PVA shows a characteristic peak at 3248 −1 (O–H stretching) and two peaks at 2923 cm−1 (C–H stretching) and 1077 cm−1 (C–O stretching). On the other hand, chitosan shows a peak at 1647 cm−1 (C=O stretching) and another peak at 1581 cm−1 (N–H bending). Gum arabic shows a peak at 1610 cm−1 (COO-symmetric stretching) [28]. Coaxial P10/C8-5 nanofiber membrane shows characteristic peaks of PVA at 3273 cm−1 (O–H stretching), 2925 cm−1 (C–H stretching) and 1080 cm−1 (C–O stretching), and also characteristic peaks of chitosan at 1661 cm−1 (C=O stretching) and another peak at 1584 cm−1 (N–H bending). P10/C10-5 nanofiber membrane shows similar results, thus confirming the existence of PVA and chitosan in coaxial nanofibers.

FT-IR spectra of PVA, chitosan, gum arabic, coaxial P10/C8-5 nanofiber membranes, and coaxial P10/C10-5 nanofiber membranes.
3.4 Thermal properties of coaxial PVA/chitosan nanofibers
TGA thermograms of PVA powder, chitosan powder and coaxial nanofibers (P10/C8-5 and P10/C10-5) are shown in Figure 7. According to the literature, the thermal degradation of PVA is approximately a two-step degradation [29], which is consistent with the PVA curve in Figure 7. The thermal degradation of chitosan is also a two-step degradation. In the first step, 50% weight loss occurs between 220°C and 320°C [30], which is also consistent with the chitosan curve in Figure 7. Interestingly, if comparing all four TGA curves in Figure 7, the P10/C8-5 curve is more similar to the chitosan curve while the P10/C10-5 curve is more similar to the PVA curve. The reason could be that the shell solution of P10/C8-5 was less viscous than that of P10/C10-5 andit might be easier to form coaxial P10/C8-5 nanofibers with better coverage of chitosan. Hence in comparison with P10/C10-5, the TGA thermogram of P10/C8-5 is more similar to that of chitosan. On the contrary, P10/C10-5 might have a thinner coverage of chitosan, thus making the TGA thermogram of P10/C10-5 more similar to that of PVA.

TGA thermograms of PVA, chitosan, coaxial P10/C8-5 nanofiber membranes, and coaxial P10/C10-5 nanofiber membranes.
3.5 Mechanical properties of coaxial PVA/chitosan nanofiber membranes
To enhance the mechanical properties of coaxial PVA/chitosan (P10/C8-5 and P10/C10-5) nanofiber membranes, the membranes were crosslinked by glutaraldehyde for 8 hours [31]. Figure 8 shows the mechanical properties (tensile strength and elongation) of coaxial P10/C10-5 and P10/C8-5 nanofiber membranes (uncrosslinked and crosslinked). The tensile strength (stress at maximum load) of P10/C8-5 and P10/C10-5 membranes increased from 0.77 and 0.66 MPa to 0.91 and 0.83 MPa, respectively (Figure 8(a)). The tensile strength of P10/C8-5 (uncrosslinked and crosslinked) was higher than that of P10/C10-5, possibly due to the better coverage of shell (chitosan) layer (see the second row in Figure 5) that enhanced the tensile strength of P10/C8-5 especially after crosslinking.

Mechanical properties of coaxial P10/C10-5 and P10/C8-5 nanofiber membranes: (a) Tensile strength (stress at maximum load), (b) elongation (strain at maximum load).* p< 0.05.
As shown in Figure 8(b), crosslinking also caused a slight decrease in the elongation (strain at maximum load) of P10/C8-5 and P10/C10-5 membranes, i.e., from 87% and 102% down to 77% and 92% (still ductile), respectively. Taken together, coaxial P10/C8-5 and P10/C10-5 nanofiber membranes exhibited favorable mechanical properties (good tensile strength and good ductility), but P10/C8-5 membranes were better and thus utilized in the following drug release experiments.
3.6 Drug release from coaxial PVA/chitosan nanofiber membranes
Theophylline is a small molecule drug (a bronchodilator) and can be easily released from a dense film [32]. The use of coaxial PVA/chitosan (P10/C8-5) nanofiber membranes in drug release was carried out by loading the core (PVA) with theophylline (5 mg/ml) as a model drug. For comparison purposes, conventional (non-coaxial) PVA (P10) nanofiber membranes loaded with theophylline were also prepared. Figure 9 shows the release profiles of theophylline from coaxial P10/C8-5 nanofiber membranes and also from non-coaxial P10 nanofiber membranes. During the first 3 minutes, 95% of theophylline was released from P10 membranes (Figure 9(b)). In contrast, 95% release of theophylline from P10/C8-5 (as core/shell) membranes was prolonged to 24 hours (Figure 9(a)). In Figure 9(c), both P10/C8-5 and P10 were confirmed as nanofiber membranes, but the average diameter of P10/C8-5 nanofibers (about 620 nm) was larger than that of P10 nanofibers (about 506 nm). Since theophylline was initially present in the core (PVA), the shell (chitosan) acted as a barrier, thus slowing down the release of theophylline. Besides, due to the larger nanofiber diameter, the specific area of P10/C8-5 nanofibers should be smaller than the specific area of P10 nanofibers. The smaller specific area also caused the release of theophylline from P10/C8-5 membranes to become slower. The drug release behavior of coaxial P10/C8-5 nanofiber membranes might be divided into three stages. The first stage was the swelling of nanofibers that gave a burst release of theophylline. The second stage was the disintegration of nanofiber membranes that gave a continuous theophylline release at a rate lower than the first stage. The third stage was the gradual diffusion of theophylline from the core that permeated through the shell of nanofibers and eventually reached equilibrium [33]. In the third stage, the chitosan shell layer was a barrier of mass transfer and thus decreased the release rate of theophylline.

The release profiles of theophylline (as a model drug) from coaxial P10/C8-5 nanofiber membranes and from conventional (non-coaxial) P10 nanofiber membranes, and the SEM images of membranes: (a) from 0 to 24 hours, (b) the initial 120 minutes * p < 0.05, (c) The SEM images of P10/C8-5 and P10 nanofiber membranes. (Scale bar = 60 μm)
As described above, several phenomena such as nanofiber swelling, disintegration, and drug diffusion were involved in the release of theophylline. To investigate these anomalous transport phenomena, a semi-empirical model called “Korsmeyer-Peppas model” was utilized to correlate the theophylline release from coaxial P10/C8-5 nanofiber membranes because the above-mentioned anomalous phenomena were considered in this model (see Section 2.7) [20, 21, 22, 23]. To obtain the parameters of release kinetics (k and n), the initial 65% of theophylline release data shown in Figure 9(b) were plotted as log drug release (%) vs. log time (min) [21, 23]. By fitting the theophylline release data with the Korsmeyer-Peppas model, the release rate constant (k) of 65.34 and release exponent (n) of 0.54 were obtained with a correlation coefficient (r2) of 0.979, as shown in Table 3. In Korsmeyer-Peppas model, for drug release from swellable cylindrical systems n ≤ 0.45 corresponds to Fickian diffusion, 0.45<n < 0.89 corresponding to anomalous (non-Fickian) transport [23]. The release exponent (n) of 0.54 obtained in this study suggests that the release mechanisms of theophylline from coaxial P10/C8-5 nanofiber membranes may involve several anomalous transport phenomena including nanofiber swelling and disintegration as well as drug diffusion.
The parameters of release kinetics (k, n) obtained by using the Korsmeyer-Peppas model to correlate the theophylline release data
Korsmeyer-Peppas model | |
---|---|
Release rate constant (k) | 65.34 |
Release exponent (n) | 0.54 |
*Correlation coefficient (r2): 0.979
4 Conclusion
By adding a small amount of gum arabic to prepare much less viscous chitosan solutions, coaxial PVA/chitosan electrospun nanofiber membranes with core/shell structures were successfully fabricated in this research. The core/shell structures were confirmed by TEM. The existence of PVA and chitosan in the nanofiber membranes was established by FT-IR analysis. Among several groups of PVA/chitosan (as core/shell) nanofiber membranes prepared in this study, P10/C8-5 membranes showed a higher tensile strength than P10/C10-5 and other membranes possibly due to the better coverage of shell (chitosan) layer. The use of coaxial P10/C8-5 nanofiber membranes in drug release extended the release time of theophylline from 5 minutes to 24 hours. Further, the Korsmeyer-Peppas model was selected to fit the data of theophylline release, giving a release exponent (n) of 0.54, suggesting that the release mechanisms may involve several anomalous transport phenomena including nanofiber swelling and disintegration as well as drug diffusion. In brief, by combining the advantages of PVA and chitosan (good mechanical strength and good biocompatibility respectively), coaxial PVA/chitosan nanofiber membranes have great potential in many biomedical applications.
Acknowledgement
Ting-Yun Kuo and Cuei-Fang Jhang contributed equally to the present work. This study was financially supported in part by the Ministry of Science and Technology, Taiwan (grants: MOST 104-2221-E-002-174 & MOST 105-2221-E-002-202).
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- Modeling and Simulation for an 8 kW Three-Phase Grid-Connected Photo-Voltaic Power System
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- Application of the optimal homotopy asymptotic method to nonlinear Bingham fluid dampers
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- Analysis of Drude model using fractional derivatives without singular kernels
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- An unsteady MHD Maxwell nanofluid flow with convective boundary conditions using spectral local linearization method
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- New analytical solutions for conformable fractional PDEs arising in mathematical physics by exp-function method
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- Quantum mechanical calculation of electron spin
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- CO2 capture by polymeric membranes composed of hyper-branched polymers with dense poly(oxyethylene) comb and poly(amidoamine)
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- Chain on a cone
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- Multi-task feature learning by using trace norm regularization
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- Superluminal tunneling of a relativistic half-integer spin particle through a potential barrier
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- Neutrosophic triplet normed space
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- Lie algebraic discussion for affinity based information diffusion in social networks
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- Radiation dose and cancer risk estimates in helical CT for pulmonary tuberculosis infections
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- A comparison study of steady-state vibrations with single fractional-order and distributed-order derivatives
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- Some new remarks on MHD Jeffery-Hamel fluid flow problem
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- Numerical investigation of magnetohydrodynamic slip flow of power-law nanofluid with temperature dependent viscosity and thermal conductivity over a permeable surface
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- Charge conservation in a gravitational field in the scalar ether theory
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- Measurement problem and local hidden variables with entangled photons
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- Compression of hyper-spectral images using an accelerated nonnegative tensor decomposition
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- Fabrication and application of coaxial polyvinyl alcohol/chitosan nanofiber membranes
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- Calculating degree-based topological indices of dominating David derived networks
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- The structure and conductivity of polyelectrolyte based on MEH-PPV and potassium iodide (KI) for dye-sensitized solar cells
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- Chiral symmetry restoration and the critical end point in QCD
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- Numerical solution for fractional Bratu’s initial value problem
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- Structure and optical properties of TiO2 thin films deposited by ALD method
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- Quadruple multi-wavelength conversion for access network scalability based on cross-phase modulation in an SOA-MZI
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- Application of ANNs approach for wave-like and heat-like equations
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Study on node importance evaluation of the high-speed passenger traffic complex network based on the Structural Hole Theory
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- A mathematical/physics model to measure the role of information and communication technology in some economies: the Chinese case
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Numerical modeling of the thermoelectric cooler with a complementary equation for heat circulation in air gaps
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- On the libration collinear points in the restricted three – body problem
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- Research on Critical Nodes Algorithm in Social Complex Networks
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- A simulation based research on chance constrained programming in robust facility location problem
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- A mathematical/physics carbon emission reduction strategy for building supply chain network based on carbon tax policy
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- Mathematical analysis of the impact mechanism of information platform on agro-product supply chain and agro-product competitiveness
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- A real negative selection algorithm with evolutionary preference for anomaly detection
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- A privacy-preserving parallel and homomorphic encryption scheme
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Random walk-based similarity measure method for patterns in complex object
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- A Mathematical Study of Accessibility and Cohesion Degree in a High-Speed Rail Station Connected to an Urban Bus Transport Network
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Design and Simulation of the Integrated Navigation System based on Extended Kalman Filter
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Oil exploration oriented multi-sensor image fusion algorithm
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Analysis of Product Distribution Strategy in Digital Publishing Industry Based on Game-Theory
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Expanded Study on the accumulation effect of tourism under the constraint of structure
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Unstructured P2P Network Load Balance Strategy Based on Multilevel Partitioning of Hypergraph
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Research on the method of information system risk state estimation based on clustering particle filter
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- Demand forecasting and information platform in tourism
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Physical-chemical properties studying of molecular structures via topological index calculating
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Local kernel nonparametric discriminant analysis for adaptive extraction of complex structures
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- City traffic flow breakdown prediction based on fuzzy rough set
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Conservation laws for a strongly damped wave equation
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Blending type approximation by Stancu-Kantorovich operators based on Pólya-Eggenberger distribution
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Computing the Ediz eccentric connectivity index of discrete dynamic structures
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- A discrete epidemic model for bovine Babesiosis disease and tick populations
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- Study on maintaining formations during satellite formation flying based on SDRE and LQR
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Relationship between solitary pulmonary nodule lung cancer and CT image features based on gradual clustering
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- A novel fast target tracking method for UAV aerial image
- Special issue on Nonlinear Dynamics in General and Dynamical Systems in particular
- Fuzzy comprehensive evaluation model of interuniversity collaborative learning based on network
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- Conservation laws, classical symmetries and exact solutions of the generalized KdV-Burgers-Kuramoto equation
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- After notes on self-similarity exponent for fractal structures
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- Excitation probability and effective temperature in the stationary regime of conductivity for Coulomb Glasses
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- Comparisons of feature extraction algorithm based on unmanned aerial vehicle image
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- Research on identification method of heavy vehicle rollover based on hidden Markov model
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- Classifying BCI signals from novice users with extreme learning machine
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- Topics on data transmission problem in software definition network
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- Statistical inferences with jointly type-II censored samples from two Pareto distributions
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- Estimation for coefficient of variation of an extension of the exponential distribution under type-II censoring scheme
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- Analysis on trust influencing factors and trust model from multiple perspectives of online Auction
- Special Issue on Advances on Modelling of Flowing and Transport in Porous Media
- Coupling of two-phase flow in fractured-vuggy reservoir with filling medium
- Special Issue on Advances on Modelling of Flowing and Transport in Porous Media
- Production decline type curves analysis of a finite conductivity fractured well in coalbed methane reservoirs
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- Flow Characteristic and Heat Transfer for Non-Newtonian Nanofluid in Rectangular Microchannels with Teardrop Dimples/Protrusions
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- The size prediction of potential inclusions embedded in the sub-surface of fused silica by damage morphology
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- Research on carbonate reservoir interwell connectivity based on a modified diffusivity filter model
- Special Issue on Advances on Modelling of Flowing and Transport in Porous Media
- The method of the spatial locating of macroscopic throats based-on the inversion of dynamic interwell connectivity
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- Unsteady mixed convection flow through a permeable stretching flat surface with partial slip effects through MHD nanofluid using spectral relaxation method
- Special Issue on Advances on Modelling of Flowing and Transport in Porous Media
- A volumetric ablation model of EPDM considering complex physicochemical process in porous structure of char layer
- Special Issue on Advances on Modelling of Flowing and Transport in Porous Media
- Numerical simulation on ferrofluid flow in fractured porous media based on discrete-fracture model
- Special Issue on Advances on Modelling of Flowing and Transport in Porous Media
- Macroscopic lattice Boltzmann model for heat and moisture transfer process with phase transformation in unsaturated porous media during freezing process
- Special Issue on Advances on Modelling of Flowing and Transport in Porous Media
- Modelling of intermittent microwave convective drying: parameter sensitivity
- Special Issue on Advances on Modelling of Flowing and Transport in Porous Media
- Simulating gas-water relative permeabilities for nanoscale porous media with interfacial effects
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- Simulation of counter-current imbibition in water-wet fractured reservoirs based on discrete-fracture model
- Special Issue on Advances on Modelling of Flowing and Transport in Porous Media
- Investigation effect of wettability and heterogeneity in water flooding and on microscopic residual oil distribution in tight sandstone cores with NMR technique
- Special Issue on Advances on Modelling of Flowing and Transport in Porous Media
- Analytical modeling of coupled flow and geomechanics for vertical fractured well in tight gas reservoirs
- Special Issue on Ever-New "Loopholes" in Bell’s Argument and Experimental Tests
- Special Issue: Ever New "Loopholes" in Bell’s Argument and Experimental Tests
- Special Issue on Ever-New "Loopholes" in Bell’s Argument and Experimental Tests
- The ultimate loophole in Bell’s theorem: The inequality is identically satisfied by data sets composed of ±1′s assuming merely that they exist
- Special Issue on Ever-New "Loopholes" in Bell’s Argument and Experimental Tests
- Erratum to: The ultimate loophole in Bell’s theorem: The inequality is identically satisfied by data sets composed of ±1′s assuming merely that they exist
- Special Issue on Ever-New "Loopholes" in Bell’s Argument and Experimental Tests
- Rhetoric, logic, and experiment in the quantum nonlocality debate
- Special Issue on Ever-New "Loopholes" in Bell’s Argument and Experimental Tests
- What If Quantum Theory Violates All Mathematics?
- Special Issue on Ever-New "Loopholes" in Bell’s Argument and Experimental Tests
- Relativity, anomalies and objectivity loophole in recent tests of local realism
- Special Issue on Ever-New "Loopholes" in Bell’s Argument and Experimental Tests
- The photon identification loophole in EPRB experiments: computer models with single-wing selection
- Special Issue on Ever-New "Loopholes" in Bell’s Argument and Experimental Tests
- Bohr against Bell: complementarity versus nonlocality
- Special Issue on Ever-New "Loopholes" in Bell’s Argument and Experimental Tests
- Is Einsteinian no-signalling violated in Bell tests?
- Special Issue on Ever-New "Loopholes" in Bell’s Argument and Experimental Tests
- Bell’s “Theorem”: loopholes vs. conceptual flaws
- Special Issue on Ever-New "Loopholes" in Bell’s Argument and Experimental Tests
- Nonrecurrence and Bell-like inequalities
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Three-dimensional computer models of electrospinning systems
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Electric field computation and measurements in the electroporation of inhomogeneous samples
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Modelling of magnetostriction of transformer magnetic core for vibration analysis
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Comparison of the fractional power motor with cores made of various magnetic materials
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Dynamics of the line-start reluctance motor with rotor made of SMC material
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Inhomogeneous dielectrics: conformal mapping and finite-element models
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Topology optimization of induction heating model using sequential linear programming based on move limit with adaptive relaxation
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Detection of inter-turn short-circuit at start-up of induction machine based on torque analysis
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Current superimposition variable flux reluctance motor with 8 salient poles
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Modelling axial vibration in windings of power transformers
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Field analysis & eddy current losses calculation in five-phase tubular actuator
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Hybrid excited claw pole generator with skewed and non-skewed permanent magnets
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Electromagnetic phenomena analysis in brushless DC motor with speed control using PWM method
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Field-circuit analysis and measurements of a single-phase self-excited induction generator
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- A comparative analysis between classical and modified approach of description of the electrical machine windings by means of T0 method
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Field-based optimal-design of an electric motor: a new sensitivity formulation
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Application of the parametric proper generalized decomposition to the frequency-dependent calculation of the impedance of an AC line with rectangular conductors
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Virtual reality as a new trend in mechanical and electrical engineering education
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Holonomicity analysis of electromechanical systems
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- An accurate reactive power control study in virtual flux droop control
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Localized probability of improvement for kriging based multi-objective optimization
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Research of influence of open-winding faults on properties of brushless permanent magnets motor
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Optimal design of the rotor geometry of line-start permanent magnet synchronous motor using the bat algorithm
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Model of depositing layer on cylindrical surface produced by induction-assisted laser cladding process
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Detection of inter-turn faults in transformer winding using the capacitor discharge method
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- A novel hybrid genetic algorithm for optimal design of IPM machines for electric vehicle
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Lamination effects on a 3D model of the magnetic core of power transformers
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Detection of vertical disparity in three-dimensional visualizations
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Calculations of magnetic field in dynamo sheets taking into account their texture
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- 3-dimensional computer model of electrospinning multicapillary unit used for electrostatic field analysis
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Optimization of wearable microwave antenna with simplified electromagnetic model of the human body
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Induction heating process of ferromagnetic filled carbon nanotubes based on 3-D model
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering ISEF 2017
- Speed control of an induction motor by 6-switched 3-level inverter