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. 2019 Feb 6;107(5):1031–1041. doi: 10.1002/jbm.a.36619

Development of bifunctional oriented bioactive glass/poly(lactic acid) composite scaffolds to control osteoblast alignment and proliferation

Sungho Lee 1, Aira Matsugaki 1, Toshihiro Kasuga 2, Takayoshi Nakano 1,
PMCID: PMC6593822  PMID: 30675975

Abstract

During the bone regeneration process, the anisotropic microstructure of bone tissue (bone quality) recovers much later than bone mass (bone quantity), resulting in severe mechanical dysfunction in the bone. Hence, restoration of bone microstructure in parallel with bone mass is necessary for ideal bone tissue regeneration; for this, development of advanced bifunctional biomaterials, which control both the quality and quantity in regenerated bone, is required. We developed novel oriented bioactive glass/poly(lactic acid) composite scaffolds by introducing an effective methodology for controlling cell alignment and proliferation, which play important roles for achieving bone anisotropy and bone mass, respectively. Our strategy is to manipulate the cell alignment and proliferation by the morphological control of the scaffolds in combination with controlled ion release from bioactive glasses. We quantitatively controlled the morphology of fibermats containing bioactive glasses by electrospinning, which successfully induced cell alignment along the fibermats. Also, the substitution of CaO in Bioglass®(45S5) with MgO and SrO improved osteoblast proliferation, indicating that dissolved Mg2+ and Sr2+ ions promoted cell adhesion and proliferation. Our results indicate that the fibermats developed in this work are candidates for the scaffolds to bone tissue regeneration that enable recovery of both bone quality and bone quantity. © 2019 The Authors. journal Of Biomedical Materials Research Part A Published By Wiley Periodicals, Inc. J Biomed Mater Res Part A: 107A: 1031–1041, 2019.

Keywords: biomaterial, bioactive glass, bone anisotropy, electrospinning, bone quality

INTRODUCTION

Bone is a highly calcified tissue consisting of collagen fibrils and biological apatite (BAp) with several hierarchical levels from nano to microscale.1 Importantly, the multiscale structure of bone tissue exhibits highly anisotropic properties associated with collagen fibril orientation and the direction of the c‐axis of BAp crystals.2, 3 The anisotropic microstructure of bone tissue is one of the most important “bone quality” indices, which mainly governs the mechanical performance of bone tissue rather than bone mass (“bone quantity”).4 During the bone regeneration process, the recovery of anisotropic bone microstructure is significantly delayed compared to the bone mineral density (BMD) restoration, which induces severe mechanical dysfunction.4 The development of bifunctional biomaterials with controllable “bone quality” and “bone quantity” is therefore necessary for the recovery of highly ordered healthy bone tissue. Control of cell alignment is a valuable strategy for constructing anisotropic bone matrices; collagen/apatite matrix alignment depends on the osteoblast orientation.5 Moreover, the degree of BAp c‐axis orientation shows a dependence on the directional distribution of osteoblasts.6 Accordingly, directional and quantitative control of osteoblasts can be determinative for achieving satisfactory bone tissue with both “quality” and “quantity.”

Bioglass® introduced the concept of bioactive materials; chemical cues from the material indicate enhanced metabolism and accelerated healing of damaged bone.7, 8 Xynos et al. reported that the dissolved silicate, calcium, and orthophosphate ions from Bioglass® stimulated human osteoblast proliferation by increasing the production of insulin‐like growth factor II (IGF‐II).9, 10, 11 Magnesium ions promote cell adhesion, proliferation, differentiation, and subsequent mineralization.12, 13, 14, 15 The expression of various integrin family members, which are a class of adhesion proteins, was increased by Mg2+ ions.13 Strontium ions have several effects on the stimulation of osteoblast proliferation and differentiation and the inhibition of preosteoclast differentiation.16, 17, 18 Sr2+ ions increase the mRNA levels of c‐fos and egr‐1, which are involved in cell proliferation.16 They also promote the metabolism of osteoblasts due to activation of calcium‐sensing receptors,16, 19 and increase alkaline phosphatase (ALP) activity,20 which is a marker for osteoblast differentiation. Osteoprotegerin (OPG) was upregulated by Sr2+ ions and accompanied the downregulation of receptor activators of nuclear factor kappa B (RANK) ligand expression, which involve differentiation of pre‐osteoclasts.18

Electrospinning is a useful method for fabricating fibrous scaffolds, which can be applied to biomimetic templates for cell adhesion, proliferation, differentiation, and mineralization of damaged tissue. Obata et al. reported the use of poly(L‐lactic acid) (PLLA) micro‐fibermats containing silicon‐doped vaterite for guided bone regeneration (GBR) membranes.21 Proliferation of osteoblasts on the fibermats was improved by dissolved silicate ions. In vivo, newly formed bone was observed over 4 weeks, and the defect was covered after 12 weeks. Fibroblasts (NIH3T3) on the oriented nanofiber scaffold were elongate and aligned parallel to the fibers, and their gene expression upregulated associated with actin production, action polymerization, and focal adhesion formation than random one.22 Human mesenchymal stem cells (hMSC) on PLLA aligned nano‐fibermats were highly oriented in the direction of the collector, where the cells were stretched along the long axis of the nanofibers.23, 24 Subsequently, the collagen fibril bundles produced by hMSC were aligned in the direction of the cell adhesion (i.e., the nano‐fiber direction). Tujunen et al.25 reported that mouse osteoblast‐like cells on PLLA/siloxane‐doped vaterite aligned micro‐fibermats were oriented in the fiber orientation direction and elongated along the microfiber.

The aim of this study is to create a novel bifunctional biomaterial for bone tissue regeneration, which achieve recovery of both bone quality (oriented bone microstructure) and bone quantity (bone mass). The oriented fibermats were prepared with bioactive glass/PLLA composites by electrospinning an anisotropic scaffold to control cell alignment. PLLA, which is the most widely used biodegradable polymer in the biomaterials field, was chosen for fabrication of the oriented fibermat. The glasses in the composites were prepared by substituting the CaO in Bioglass® (45S5) with MgO and SrO to improve bone regeneration with the dissolved ions from the glasses. Herein, a fundamental investigation on the design of oriented bioactive glass/PLLA fibermats for biomedical applications is reported, evaluating their anisotropic morphology, ion‐releasing ability, and cell behavior on the fibermats.

MATERIALS AND METHODS

Preparation of the bioactive glasses

Glasses with compositions of 46.1SiO2·24.4Na2O·26.9MO·2.6P2O5 (mol%, M = Ca, Mg, or Sr, denoted by BGM) were prepared by melt quenching. Glass batches were prepared by mixing SiO2 (99.0%), Na2CO3 (99.5%), CaCO3 (99.5%), MgO (99.0%), SrCO3 (98.0%), and NaH2PO4 (99.0%). All the reagents were purchased from Kishida Chemical Co. The batches were melted in a platinum crucible at 1500°C for 30 min and quenched by pressing with two stainless steel plates. The glasses were examined using laser Raman spectroscopy in between 220 and 1300 cm−1 (NRS‐5100, JASCO). The resulting glasses were pulverized using an automatic alumina mortar, and the powders were stored in a desiccator. The resulting powders were observed by field emission gun electron microscopy (SEM, JSM‐6500, JEOL) with an accelerating voltage of 15 kV after coating the samples with an amorphous osmium layer using an osmium coater (Neoc CS, Meiwafosis Co. Ltd.). Particles diameter were measured using the ImageJ software (NIH).

Preparation of the composite pellets

BGM powders were mixed with PLLA (LACEA, molecular weight of 140 kDa, Mitsui Chemical) by a melt‐blending method using a kneader (PBV‐0.1, Irie Shokai) at 190°C for 10 min, resulting in BGM/PLLA composite pellets. The volume ratios of BGM powders in the composites were set to 10 and 30 vol.%. The volumes of PLLA and BGM powders were calculated from their density. The densities were measured by an Archimedes' method using acetone and water as immersion fluid for BGM and PLLA, respectively, at 25°C (n = 3). Molecular weight distributions of the composites were determined by gel permeation chromatography (GPC, Prominence, Shimadzu) using a KF‐806L column (Shodex). For detection, a Shimadzu refractometer RID‐10A was used. Chloroform (99.7%, HPLC grade, Wako Pure Chemical) was used as the eluent flowing at 1 mL·min−1 at 35°C. The composites were manually injected (20 μL) at a concentration varying between 10 and 15 mg·mL−1. Average molecular weights and distributions were determined against a linear polystyrene calibrant.

Preparation of the oriented fibermats

The oriented fibermats with the composites were prepared by an electrospinning method, and that with PLLA was prepared as a control for cell proliferation test. The composite pellets and PLLA were dissolved in chloroform (99.0%, Wako Pure Chemical) at 14 wt.% PLLA to prepare the solution for electrospinning. In our preliminary experiments, this ratio was found to be optimal for preparing the oriented fibermats. In case of 10 vol.% BGMg composite, the pellet was dissolved in chloroform at 10 wt.% PLLA, since the 14 wt.% solution could not be ejected from the syringe. The viscosities of the prepared solutions were measured using a vibration‐type viscometer (VM‐10A‐M, Sekonic Co.). Subsequently, the prepared solutions were loaded into a syringe pump (FP‐1100, Melquest, Japan) with an 18 gauge syringe needle, which was set at a discharge rate of 0.15 mL·min−1. A high‐voltage supply (HARb‐40P0.75, Matsusada Precision Inc.) was used to apply voltages of 16 kV at the needle tip. The distance between the needle tip and the drum collector was maintained at 200 mm. The drum collector (diameter 30 mm) was rotated at 3000 rpm (4.7 m·s−1). The obtained fibermats were denoted by BGM x, where BGM is sample code for the bioactive glass and x (x = 10 or 30) is the vol.% of BGM in the composite. The electrospinning was carried out at room temperature (approximately 25°C) and approximately 40% relative humidity.

Morphology of the fibermats

The morphology of the prepared fibermats was observed by SEM with an accelerating voltage of 3 kV after coating the samples with an amorphous osmium layer using an osmium coater. Fiber diameter and the angle (θ) between the fiber and collector rotation direction were measured using the ImageJ software (NIH).

Ion‐releasing behavior of the fibermats

To characterize the ion‐releasing behavior from the fibermats, samples of 14 mm diameter and 120–160 μm thickness were soaked in 10 mL of 50 mM Tris buffer solution (TBS, pH 7.40, 37°C) for 9 days. The concentrations of Si, P, Ca2+, Mg2+, and Sr2+ ions in the TBS were measured by inductively coupled plasma optical emission spectroscopy (ICP‐OES, Agilent 720 ICP, Agilent Technologies). The fraction of weight released of various elements in TBS were calculated as follows;

Release percentage%=a×VsolutionMsample×Wglass×Frac,a (1)

where a is the concentration of the element of interest in mg·L−1, Vsolution is the volume of soaked solution in L, Frac,a is the nominal weight fraction of the element in the glass, Msample is weight of the sample in mg, and Wglass is the wt.% of the glass in the fibermat. After soaking in TBS for 9 days, the fibermats were analyzed by X‐ray diffractometry (XRD, X'pert PRO, Phillips) using Cu Kα radiation.

Osteoblast proliferation on the fibermats

Fibermats with 8 mm diameter were prepared for osteoblast tests. A PLLA oriented fibermat was used for the control. The samples were soaked in 70% ethanol for 30 s and subsequently dried under ultra violet (UV) light for 30 min for sterilization. The cells were cultured in alpha‐minimum essential medium (α‐MEM, with l‐glutamine and phenol red, Invitrogen) containing 10% fetal bovine serum (FBS, Invitrogen). The samples were placed into 48 well plates (n = 4), and mouse osteoblast‐like cells (MC3T3‐E1 cells) were seeded by adding 0.5 mL of the culture medium containing cells at a concentration of 3 × 104 cells·mL−1. The culture medium was replaced after 1 day of culturing. After 1 and 3 days of culturing, the samples were washed with phosphate buffered saline (PBS), and 0.5 mL of α‐MEM (no phenol red) and 50 μL of Cell Count Reagent SF (Nacalai Tesque) were added to the samples. After 2 h of incubation (37°C, 5% CO2), the absorbance at 450 nm was evaluated using a microplate reader (Multiskan FC, Thermo Scientific). The number of cells was calculated by a standard curve between the number of cells and the absorbance of the resulting medium.

Primary osteoblast isolation and culture on the fibermats

Primary osteoblasts were isolated from newborn mouse calvariae as described in our previous report.26 Briefly, calvariae from newborn C57BL/6 mice were excised under aseptic conditions, placed in ice‐cold α‐MEM, and then the fibrous tissues around the bone were gently removed. The calvariae were then subjected to a series of collagenase (Wako Pure Chemical)/trypsin (Nacalai Tesque) digestions at 37°C for 15 min each. The first two digests were discarded, since fibroblasts were mixed.27 The supernatants of digests 3–5 were neutralized with α‐MEM and pooled. The pooled solutions were filtered using a 100 μm mesh. The filtrates were centrifuged, and the resulting pellets were resuspended in α‐MEM containing 10% FBS. The population of obtained cells was verified by real‐time reverse transcription polymerase chain reaction (RT‐PCR, Step‐one, Applied Biosystems). The positive expression of typical osteoblast markers, collagen type I, ALP, and bone sialoprotein were confirmed, indicating the successful isolation of osteoblastic cell population in the present method. Fibermats with 14 mm diameter were prepared. The samples were soaked in 70% ethanol for 30 s and subsequently dried under UV light for 30 min for sterilization. The samples were placed into 24 well plates (n = 4), and primary osteoblast cells were seeded by adding 1.0 mL of the culture medium containing cells at a concentration of 3 × 104 cells·mL−1. The culture medium was replaced after 1 day.

Fluorescence imaging of primary osteoblast

Primary osteoblasts were cultivated for 3 days on the samples, and the cells were fixed with 4% formaldehyde in PBS for 20 min. After washing three times with PBS‐0.05% Triton X‐100 (PBST), the cells were incubated in PBST containing 1% normal goat serum (NGS) for 30 min to block nonspecific antibody binding sites. Subsequently, the cells were incubated with mouse monoclonal antibodies against vinculin (Sigma‐Aldrich) at 4°C for 12 h. The cells were incubated with Alexa Fluor® 546‐conjugated anti‐mouse IgG (Invitrogen) and Alexa Fluor® 488‐conjugated phalloidin (Invitrogen). Finally, the cells were washed and mounted in Fluoro‐KEEPER Antifade Reagent with DAPI (Nacalai Tesque). Fluorescent images were taken using a fluorescence microscope (BZ‐X700, Keyence). The cell orientation angle (θ) against the collector rotation direction was analyzed using the Cell Profiler software (Broad Institute Cambridge).

Quantitative analysis for the degree of fiber and cell orientation

To evaluate the degrees of fiber and cell arrangement, the orientation order parameters FD and CD were calculated, where FD and CD are the degrees of fiber and cell alignment, respectively.28 This system was derived using a distribution function n(θ), which is defined as the number of measured fibers or cells at the angle θ. The expected value of the mean square cosine <cos 2 θ>, FD, and CD were calculated as follows;

<cos2θ>=02πcos2θnθ02πnθ (2)
FDorCD=2<cos2θ>0.5 (3)

FD and CD take values ranging from −1 (fiber or cell completely aligned perpendicularly to the collector rotation direction), to 0 (fiber or cell oriented randomly), to 1 (fiber or cell completely aligned parallel to the collector rotation direction).

Statistical analysis

Statistical significance was assessed by one‐way ANOVA, followed by Tukey's post hoc test. A significance of p < 0.05 was required for rejection of the null hypothesis.

RESULTS

Glass and composite characterization

Densities of BGMg, BGCa, BGSr, and PLLA were 2.59, 2.72, 3.04, and 1.25 g/cm3, respectively. Pulverized BGMg, BGCa, and BGSr diameters were approximately 2.7, 3.0, and 2.8 μm, respectively, and their distribution were shown in Figure 1. The particle diameter distribution between BGM showed no significant difference. Laser Raman spectra of BGM are shown in Figure 2A. The following Raman bands corresponding to the silicate Q Si n (n = 0–3) groups29, 30 and orthophosphate (Q P 0) group31, 32 were observed: the symmetric stretching mode of Q Si 3 (~1030 cm−1), symmetric stretching mode of Q Si 2 (~970 cm−1), symmetric stretching mode of Q Si 1 (~910 cm−1), symmetric stretching mode of Q Si 0 (~850 cm−1), Si‐O stretching linkages (~640 cm−1), and symmetric stretching mode of the non‐bridging oxygen in Q P 0 (~950 cm−1). BGMg may contain low amount of Q Si 4 (< 2%), which simulated by molecular dynamics.33 However, the band corresponding to the asymmetric stretching of Q Si 4 (~1160 cm−1)34 was not observed for BGM in this work. The spectra between 800 and 1200 cm−1 were fitted with Gaussian functions, and integrated portions of the Q Si n (n = 0–3) groups are shown Figure 2B. The integrated portion of Q Si 0 for BGMg was 2.4%, while those of BGCa and BGSr were 8.3 and 8.5%, respectively. The percentage of non‐bridging oxygen (NBO) in the silicate groups of BGM were calculated using the following equation:

NBOinQSinofBGM%=n=034n×QSinBGM4×n=03QSinBGM×100 (4)

where n is number of bridging oxygen in Q Si n group, and QSinBGM is integrated portions of the Q Si n groups in BGM, which shown in Figure 2B. The values of BGMg, BGCa, and BGSr were 35.7%, 42.7%, and 44.0%, respectively. The NBO percentage indicates that the oxygen was in a SiO4 tetrahedron, not connected to other SiO4 tetrahedra.

Figure 1.

Figure 1

Powder diameter distribution of (A) BGMg, (B) BGCa, and (C) BGSr. Bar graphs represent appearance frequency and solid line represent cumulative frequency.

Figure 2.

Figure 2

(A) Raman spectra for BGM and (B) integrated portion of the Q Si n groups in BGM.

Number‐average molecular weights (M n), weight‐average molecular weights (M w), and polydispersity indices (PDI, M w/M n) of PLLA and the composites are shown in Table 1. The viscosities of the solutions for electrospinning are also shown in Table 1, where the solutions were prepared with concentrations of 14 wt.% of PLLA in chloroform. The 10 vol.% BGMg composite was dissolved in chloroform at 10 wt.% of PLLA for electrospinning, with a viscosity of 1.4 Pa·s. The composites containing BGMg were found to have larger M n values compared to those of the composites containing BGCa and BGSr. The composites containing 10 vol.% of glass powders had larger M n values and solution viscosities, and smaller PDI values than those of the 30 vol.% samples.

Table 1.

Molecular Weights and Polydispersity Indices (M w/M n) of BGM/PLLA Composites with 10 or 30 vol.% of BGM and Viscosities of their Solutions with 14 wt.% of PLLA in Chloroform

Samples M n/kDa M w/kDa M w/M n Viscosity/Pa·s
PLLA 51.4 94.9 1.8 1.3
BGMg 10 vol% 31.7 57.8 1.8 3.7
30 vol% 23.0 54.8 2.4 2.3
BGCa 10 vol% 20.0 32.9 1.6 1.4
30 vol% 15.9 41.0 2.6 1.3
BGSr 10 vol% 26.4 52.3 2.0 2.0
30 vol% 19.0 47.1 2.5 1.2

Morphology of the fibermats

SEM images and fiber orientation angle histograms of the fibermats are shown in Figure 3. The fibers were aligned with the collector rotation direction (parallel to the yellow arrows), and the fiber orientation angles were distributed about a center of zero. The calculated FD values and diameters of the fibermats are shown in Figure 4. The FD of BGMg10 was significantly larger than the others (p < 0.01), whereas the FD values showed no significant differences between BGMg30, BGCa x, and BGSr x. The fiber diameters of BGMg10, BGMg30, BGCa10, BGCa30, BGSr10, and BGSr30 were 6.6, 4.8, 4.9, 3.4, 6.9, and 3.3 μm, respectively. The diameters of the fibers containing 10 vol.% of BGM were larger than those of 30 vol.% fibers. The FD and fiber diameter of the PLLA fibermat were 0.97 and 9.6 μm, respectively.

Figure 3.

Figure 3

SEM images of (A) BGMg10, (B) BGCa10, (C) BGSr10, (D) BGMg30, (E) BGCa30, and (F) BGSr30. Arrows indicate the collector rotation direction. Fiber orientation angle histograms for (G) BGMg10, (H) BGCa10, (I) BGSr10, (J) BGMg30, (K) BGCa30, and (L) BGSr30. Error bars represent the standard deviation.

Figure 4.

Figure 4

(A) Fiber orientation degree of BGM x, and (B) fiber diameter of BGM x. Error bars represent the standard deviation, and n.s. represent non‐significant difference between the samples.

Ion‐releasing behavior of the fibermats

Ion‐releasing behaviors of BGM x in TBS are shown in Figure 5A–D. The released amount of Si, divalent (Mg2+, Ca2+, and Sr2+), and Na+ ions showed increasing trends with increased soaking time. The P ion releasing behaviors of the samples were significantly different. The amount of P ions released for BGMg x increased to almost 100% with increased soaking time, whereas that of BGSr10 increased to approximately 65%, and those of BGCa10 and BGSr30 were approximately 30%, irrespectively the soaking time. Notably, the P ion releasing behavior of BGCa30 decreased to 0% with increased soaking time. The amounts of divalent ions released for BGCa30 and BGSr30 were smaller than those of the other BGM x. XRD patterns of BGM x after soaking in TBS for 9 days are shown in Figure 5E. BGCa x and BGSr x showed XRD peaks corresponding to Ca10(PO4)6(OH)2 (HA, ICCD card: 74–0566) and Sr5(PO4)3OH (Sr‐HA, ICCD card: 33–1348), respectively. The XRD peak intensities of BGCa30 and BGSr30 were larger than those of BGCa10 and BGSr10, respectively.

Figure 5.

Figure 5

Percentages of the amount of released (A) Si, (B) P, (C) divalent (Mg, Ca, and Sr), and (D) Na ions in TBS from BGM x. Error bars represent the standard deviation. (E) XRD patterns of BGM x after soaking in TBS for 9 days.

Cell behavior on the fibermats

The cell numbers on BGM x are shown in Figure 6. BGMg x showed significantly larger cell numbers than PLLA at all sampling times, and those of BGSr x were significantly larger at 3 days. BGCa10 and BGCa30 showed significantly larger values than PLLA at 3rd and 1st day, respectively. Fluorescence images of the cells and cell orientation angle histograms are shown in Figure 7. The cells were aligned in the fiber oriented direction (i.e., the collector rotation direction), and the cell orientation angles were distributed about a center of zero. Calculated cell orientation degree (CD) values on the fibermats are shown in Figure 8. The CD values of BGMg10, BGCa10, and BGSr10 were larger than those of BGMg30, BGCa30, and BGSr30, respectively: that is, the CD values of the fibers containing 10 vol.% of BGM were larger than those of the 30 vol.% fibers.

Figure 6.

Figure 6

Cell numbers after 1–3 days on BGM x. Error bars represent the standard deviation.

Figure 7.

Figure 7

Fluorescence images of osteoblasts cultured on (A) BGMg10, (B) BGCa10, (C) BGSr10, (D) BGMg30, (E) BGCa30, and (F) BGSr30. Arrows indicate the collector rotation direction. Green: F‐actin, blue: nuclei, and red: vinculin. Cell orientation angle histograms for (G) BGMg10, (H) BGCa10, (I) BGSr10, (J) BGMg30, (K) BGCa30, and (L) BGSr30. Error bars represent the standard deviation.

Figure 8.

Figure 8

Cell orientation degree of BGM x. Error bars represent the standard deviation.

DISCUSSION

The Raman band intensity of BGMg was smaller than those of BGCa and BGSr, which was also noted by Karakassides et al.31 and Morikawa et al.35 Raman bands corresponding to Q Si n and Q p 0 were red‐shifted (moved to lower frequencies) in the order: BGMg, BGCa, and BGSr. This can be explained by the field strength. Dietzel suggested that the field strength (F), which is the simplified Coulomb's force of the ions in glass, is defined as follows36, 37:

F=Zcd2valance/Å2 (4)

where Z c is the ionic charge and d is the interatomic distance between the cation and oxygen. The F values of Mg, Ca, and Sr were 0.53 or 0.46 (four‐fold or six‐fold coordination), 0.33, and 0.28, respectively.36 The bonding strength decreased in the order Mg‐O, Ca‐O, and Sr‐O, causing the observed differences in the silicate and phosphate stretching vibration frequencies.31, 35 The NBO contents in BGMg was larger than BGCa, and BGSr. According to Dietzel, Mg can be classified by the intermediates, which can switch role network modifier and former.36, 37 Watts et al. reported that Mg can enter a silicate network as MgO4 tetrahedral units, which can act as a network former.38 Thus, Mg in BGMg acts as a network former to enter the silicate network; which means that Mg is less effective at breaking the silicate chains than Ca and Sr. Consequently, BGMg showed a smaller NBO content than those of BGCa and BGSr.

The M n of the composite pellets decreased from that of PLLA, since absorbed water in the glass powder break the PLLA polymer chain during the melt‐blending process. The absorbed water in the glass powder was bonded to the NBO in the glass structure. Accordingly, BGMg contained less absorbed water than BGCa and BGSr did, since the NBO content of BGMg was less than that of the others. Thus, the M n of the composite containing BGMg was larger than those of BGCa and BGSr. Similarly, the composites containing 10 vol.% of the glass powder had larger M n values than those of the 30 vol.% composites, because they contained less glass powder (i.e., containing less amount of NBO). Generally, when a polymer with a larger M n is dissolved in a solvent, its viscosity will be higher than a solution of the same polymer with a smaller M n.39 Correspondingly, the viscosity of the solutions had larger values for BGMg composites than those of the BGCa and BGSr solutions. Also, the composites containing 10 vol.% of the glass powder showed larger viscosities than the 30 vol.% composites.

In electrospinning, polymer fibers are formed by the creation and elongation of an electrified fluid jet.40 The velocities of the jets measured using a high framerate video camera were in the range from 0.5 to 5 m·s−1.40 A collector speed of 4.7 m·s−1 was used in this work; accordingly, the fibers could be collected while elongating in the collector rotation direction. If the solution formed a stable jet during the electrospinning conditions, the resulting fibers showed oriented morphologies. The composites containing 10 vol.% of BGM formed stable jets during electrospinning, whereas the 30 vol.% composites formed branched fluid jets. Generally, jet instability induces a branched fluid jet;39 the composites with 30 vol.% BGM formed unstable jets more easily than the 10 vol.% composites due to their larger PDI values and because they contained larger amounts of glass powder. Branched fluid jets can be induced by the random angle distribution of the fibers, since there is an angular difference from the primary jet. This may also lead to larger FD values for the fibermats containing 10 vol.% of BGM than those of the 30 vol.% composites. A branched jet forms by ejecting smaller jets from the surface of the primary jets, which have smaller diameters than the primary jet.39 Thus, BGMg30, BGCa30, and BGSr30 had smaller fiber diameters and larger FD values than those of BGMg10, BGCa10, and BGSr10, respectively.

The released amounts of divalent and P ions from BGCa x and BGSr x were smaller than that of BGMg x, owing to precipitation of HA and Sr‐HA, respectively. No XRD peaks were observed for BGMg x, since the Mg2+ ions inhibited the precipitation of apatite.41 The released amounts of Si ions from BGCa30 and BGSr30 were smaller than those of the others, due to formation of an Si‐OH gel layer,42, 43, 44 which induced apatite formation.45 The released amounts of P and divalent ions from BGCa30 and BGSr30 were smaller than those of BGCa10 and BGSr10, respectively. That is, large amount of the ions from BGCa30 and BGSr30 were used for precipitation of HA and Sr‐HA than those of BGCa10 and BGSr10, respectively. Thus, XRD intensities of BGCa30 and BGSr30 were larger than those of BGCa10 and BGSr10, respectively. BGMg x showed similar/larger Si release percentage compare with the others, since Si‐O‐Mg bonds weaken the glass network structure and the resistance to hydrolysis38, 46, 47 despite lower NBO content in BGMg. The released amounts of divalent (i.e., Mg2+, Ca2+, and Sr2+) and Si ions from the fibermats increased with increased soaking time, which is expected to improve bone regeneration.

The cell numbers of BGMg x were significantly larger than those of the control after 1 and 3 days of culturing. This was caused by the dissolved Mg2+ ions from the BGMg x, which improved cell adhesion and proliferation.12, 13, 14, 15 BGSr x showed a significantly larger cell number after 3 days of culturing compared to that of the control, since the dissolved Sr2+ ions from BGSr x improved proliferation.

In our previous report, primary osteoblasts on oriented collagen substrate were aligned parallel to the collagen fiber orientation.6 Cell produced collagen matrix oriented in the direction of cellular elongation, and the c‐axis of deposited apatite crystals showed preferential alignment along the direction of the newly synthesized collagen fibers6. Thus, control of the osteoblast alignment can construct the bone tissue anisotropy depending on the alignment of the cells themselves: that is, strongly orientated osteoblasts can produce the anisotropic bone tissues. Sun et al. reported that the cells adhered to a single fiber when the diameter of fiber was larger than 10 μm, whereas the cells adhered to several fibers and spread when the diameter of the fibers was <10 μm.48 In this study, the osteoblasts adhered on the fabricated microfibermats elongate their stress fiber along the fibermats, because the dynamics of actin organization is strictly regulated by the spatial geometry involving the scaffold curvature.49 In microfibermats, the fiber diameter with >10 μm could helpful to improve cell alignment by inhibiting cells spread between fibers.48 That is, the orientation degree of cells adhered to a single fiber can be easily controlled by controlling the morphology of the fibermats. BGMg10, BGCa10, and BGSr10 showed larger CD values than those of BGMg30, BGCa30, and BGSr30, respectively, since the fiber diameters of the 10 vol% BGM fibermats were larger than those of the 30 vol.% fibermats. Notably, the cells on BGMg10 and BGSr10, whose fiber diameters were larger than 6 μm, adhered to some single fibers, resulting in CD values that were larger than those of the other samples. These results indicate that we can manipulate the cell orientation and proliferation freely by controlling the fiber diameter and the ionic species released from the bioactive glasses.

CONCLUSION

A novel bifunctional biomaterial, which can control osteoblast orientation as well as cell proliferation, was established. The oriented BGM x/PLLA composite fibermats enabled cell alignment along the fibers and promoted cell proliferation due to the released ions from the bioactive glasses. The degree of fiber orientation was successfully controlled by modulating the content of the bioactive glasses and fiber diameters. The cell proliferation was significantly upregulated by the release of Mg2+ and Sr2+ ions from the bioactive glasses. The cell orientation was determined by the cell recognition of the fiber orientation and adherence along single fibers or the formation of cell branches protruding across multiple fibers. The obtained results not only indicated that the fabricated composites could control the cytoskeletal arrangement of osteoblasts along the fiber direction, but also, the controlled release of ions successfully improved osteoblast proliferation. These findings can lead to the development of innovative multifunctional biomaterials suitable for tissue regeneration treatments by the optimization of the structural properties of the scaffolds and inorganic ion element release.

ACKNOWLEDGMENTS

This work was supported by Grants‐in‐Aid for Scientific Research from the Japan Society for Promotion of Science (Grant Numbers JP16K14403, JP18H03844, JP18H05254, and JP17H06224).

Lee S, Matsugaki A, Kasuga T, Nakano T. 2019. Development of bifunctional oriented bioactive glass/poly(lactic acid) composite scaffolds to control osteoblast alignment and proliferation. J. Biomed. Mater. Res. Part A 2019:107A:1031–1041.

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