Mohammad Masoud Mirhosseini,
Vahid Haddadi-Asl* and
Seyed Shahrooz Zargarian
Department of Polymer Engineering and Color Technology, Amirkabir University of Technology, Tehran, Iran. E-mail: haddadi@aut.ac.ir; Tel: +98 21 64542305
First published on 17th August 2016
Functionalized hydroxyapatite nanoparticles (HA-F127) were synthesized by immobilizing pluronic F127 onto hydroxyapatite nanoparticles (HA). Successful grafting of F127 was evaluated by FTIR, TGA and TEM. XRD was used to study the crystalline structure of neat and functionalized nanoparticles. Grafted F127 chains on the surface of HA formed a core–shell structure. Furthermore, immobilization of F127 chains on the HA surface decreased the agglomeration of modified nanoparticles and improved their dispersion. In the next step, the HA-F127 and unmodified HA were introduced into a PCL/P123 electrospun substrate, and nanocomposites containing 4 wt% nano-filler were obtained. The corresponding properties of these polymer/ceramic nanocomposites, including morphology, thermodynamics, mechanics and biocompatibility, were evaluated. HA-F127/PCL/P123 showed superior mechanical performance, crystallinity percentage and thermal stability. The aforementioned improvements were primarily ascribed to a uniform dispersion of HA-F127 and strong interfacial adhesion between filler and matrix, which resulted from superior chain entanglements and interfacial crystallization of modified HA in the polymer substrate. Nanocomposites containing modified HA organized into a reliable platform for adhesion and proliferation of mouse L929 fibroblast cells. Finally, to analyze the interfacial interactions between phases, molecular dynamics simulation was applied. It was found that strong interfacial interactions exist between HA-F127 and PCL/P123. Consequently, HA-F127/PCL/P123 nanofibrous scaffolds can be considered as a promising candidate for tissue engineering applications.
Hydroxyapatite (HA) is a type of calcium phosphate with the chemical composition Ca10(PO4)6(OH)2 which identically resembles that of natural bone mineral (Ca/P = 1.67). Due to HA's excellent properties, such as bioactivity, biocompatibility, osteoconductivity, nontoxicity, relatively stable degradation and mechanical strength, this bioceramic has found numerous applications as bone substitutes and tissue engineering scaffolds. In particular, HA not only plays a primary role in improving the mechanical properties of the nanocomposites, but also provides a favorable environment for osteoconduction, protein adhesion, and osteoblasts proliferation.4,5
In most cases due to the extremely high surface area in nanocomposites, an improvement of the mechanical and thermo mechanical properties, bioactivity and biocompatibility can be achieved at low filler contents which marks the main advantage of these materials over micro phase reinforced composites (less than 5 wt%).6,7 However, agglomeration and weak interfacial interactions of nano-reinforcements result in reduced stress transfer at the reinforcement-polymer interface and therefore the full potential of these materials cannot be fully exploited. In other words, nano-reinforcements and more especially nanoparticles with great specific surface tend to aggregate in polymer matrix, and the interface between organic polymer and inorganic nanoparticles is often weak because of the incompatibility. Simultaneously, incompatibility and phase separation of nanoparticles agglomerates result in morphology defects and failure at the interface and thus reduces nanocomposite biocompatibility.8,9
In polymer nanocomposites, nanoparticles surface functionalization has been proven to be a pertinent technique which minimizes particle/particle interaction and enhances particle/matrix interaction. Interfacial interaction has a more dominant role in case of nanocomposites, which determines the dispersion and agglomeration formation of the filler within the matrix and the stress transfer along the interface. This in turn dictates the physical properties of the polymer matrix and consequently the macroscopic characteristics of the nanocomposite. In order to improve the inorganic nanoparticles compatibility in polymeric substrates, surface modification with organic molecules seems to be relevant. Resultantly, the surface modified nanoparticles can disperse into polymeric matrix homogeneously. Moreover, the surface modification agent would interact with the matrix by chemical or physical interaction, thus the compatibility could be greatly improved.
Various methods have been utilized to tune the surface properties of HA, including the use of small molecules like silane coupling agents,10 dodecyl alcohol,11 etidronic acid,12 isocyanates,13 organophosphonic acids,14 carboxylic acids15 and polymer chains such as poly(hydroxyethyl methacrylate),16 poly(3-hydroxybutyrate),5 polyethylene glycol,17 poly(methyl methacrylate),18 polypyrrole,19 poly(acrylic acid),20 poly(N-isopropylacrylamide),21 collagen,22 polylactic acid23 and polycaprolactone.24 In these methods, the surface hydroxyl groups of HA directly and covalently bonded with the mentioned molecules and polymer chains following the relevant chemical reaction.
Polycaprolactone (PCL), a semi-crystalline linear polyester, has attracted growing interest for its biomedical applications in bone tissue engineering over the last few decades.25 Moreover pluronic, an ABA-type triblock copolymer consisting of hydrophilic polyethylene oxide (PEO) units and hydrophobic polypropylene oxide (PPO) units arranged in a linear triblock structure (PEO)x–(PPO)y–(PEO)x, has been used in approaches toward increasing blend hydrophilicity.26,27 Our previous study showed that PCL/P123 fibrous scaffolds not only improved hydrophilicity but also elongation at break and ultimate tensile strength of blended samples compared to the neat PCL scaffold. Therefore, the PCL/P123 is a promising polymer matrix for tissue engineering applications.28 The first aim of this study, therefore, was to covalently attach the pluronic F127 to the HA surface via esterification reaction. The structure obtained was studied using Fourier transform infrared (FTIR) spectroscopy, thermogravimetric analysis (TGA), X-ray diffraction (XRD) and transmission electron microscope (TEM). To the best of our knowledge, this is the first report on the attachment of pluronic F127 via covalent bonding to the surface of HA surface. The second aim was to embed neat and modified HA in the PCL/P123 solution and electrospun the resulted suspensions. Corresponding properties were evaluated, including morphology, mechanical and thermodynamics. Furthermore, to evaluate the influence of surface modification on the HA/polymer interactions at atomic level, molecular dynamic simulations were designed and evaluated.
Thermogravimetric analysis (TGA) was carried out using a Mettler Toledo TGA/SDTA851 under N2 atmosphere at a flow rate of 50 mL min−1. The thermograms were obtained from 0 to 700 °C at a heating rate of 10 °C min−1. A sample weight of about 10 mg was used for all the measurements.
X-ray diffraction (XRD) spectra were collected on an X-ray diffraction instrument (Siemens D5000) with a Cu target (k = 0.1540 nm) at room temperature. The system consists of a rotating anode generator, and operated at 35 kV and a current of 20 mA. The samples were scanned from 2 to 40° 2θ at the step scan mode, and the diffraction pattern was recorded using a scintillation counter detector. The basal spacing of the samples was calculated using the Bragg's equation.
The transmission electron microscope (TEM), Zeiss EM10C, with an accelerating voltage of 80 kV was employed to study the morphology of the neat and surface modified HA particles. Samples were prepared by sonication of HAs in ethanol and their deposition on a carbon coated copper grid (mesh 300).
The morphology of electrospun structures was determined by scanning electron microscopy (SEM) (SERON AIS-2100, South Korea) using 15 kV accelerating voltage. The samples were coated with gold using a sputter coater before SEM imaging. The average fiber diameter and corresponding size distribution were analyzed by measuring 200 fibers presented in SEM micrographs using an image analyzer (Image J, developed by the National Institute of Health, USA).
Differential scanning calorimetry (DSC) experiments were conducted with a Flash DSC 1 of Mettler-Toledo, in order to evaluate the thermal properties of the nanocomposites. The experiments were conducted at a constant heating rate of 10 °C min−1 on samples (15–20 mg) packed in aluminum pans under nitrogen flow. The samples were heated in two stages. First, the samples were heated to 120 °C and kept at that temperature for 5 min to erase the thermal history. Afterward they were cooled to −60 °C and then reheated again to 120 °C. The melting temperature (Tm) and the melting enthalpy (ΔH) of these nanocomposites were determined from the heating scans. The crystallinity percentage (% Xc) can be calculated by applying the equation:
Mechanical properties of different scaffolds were performed using an electromechanical tensile tester (Instron 5566, Elancourt, France). Rectangular specimens with a length of 20 mm and a width of 5 mm were manually cut from electrospun samples. All samples were mounted between holders at a distance of 2 cm. The stress strain curves of these materials were constructed from the load-deformation curves recorded at a stretching speed of 5 mm min−1.
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Fig. 1 Reaction routes for surface modification of HA nanoparticle (a) synthesis of F127-COOH, (b) immobilization of F127 on hydroxyapatite surface. |
Fig. 2a shows the FTIR spectra of F127 and F127-COOH. As seen, a sharp peak appears at 1730 cm−1 in F127-COOH spectra which can be attributed to the newly formed carbonyl group in this sample. Therefore, successful transformation of F127 hydroxyl groups to carboxyl groups through interaction with maleic anhydride can be postulated.
FTIR spectra of HA and HA-F127 are presented in Fig. 2b. Considering HA spectrum, the absorption peaks at 562 and 603 cm−1 are assigned to the deformation vibrations of phosphate groups whereas peaks at 1028 and 962 cm−1 are attributed to stretching vibrations of these groups. The band at 3565 cm−1 is related to the stretching vibration of free hydroxyl group. The small adsorption peak around 1600 to 1650 cm−1 and the broad adsorption band at 3412 cm−1 are assigned to the bending vibrations and stretching vibrations of surface absorbed and structural H2O in the HA, respectively.30 From Fig. 2b, a new adsorption peak at 1730 cm−1 appears which can be assigned to the CO stretching vibration of grafted F127-COOH. Moreover, peaks in the range of 3000–2850 cm−1 are corresponded to the C–H stretching vibrations of the CH3 and CH2 groups of grafted polymer chains. Since HA nanoparticles were repeatedly washed with tetrahydrofuran after the modification process, the existence of ungrafted F127-COOH remanence in the HA-F127 sample can be ignored and therefore the newly observed peaks in HA-F127 spectrum can be solely attributed to the surface grafted polymer chains.
TGA analysis was used to study the thermal properties of the HA samples and also the related modifier content. The amount of surface grafted polymer was determined as a weight loss percentage during heating. TGA and dTG results for the pristine F127, neat and modified HA are shown in Fig. 3. According to the results, a small mass loss of HA samples at temperatures less than 100 °C can be attributed to the absorbed water molecules on the surface of nanoparticles. This mass loss is continuous for HA until 520 °C whereas no mass loss can be observed for the modified HA in the range of 100 °C to 220 °C suggesting the omission of hydroxyapatite structural water molecules during modification process. The second stage of neat HA mass loss is observed in the temperature range of 520 to 700 °C, which results from dehydroxylation of surface and structural OH groups. The beginning of this stage shifts to the temperature of 580 °C for the modified HA sample suggesting improved thermal stability of modified HA nanoparticles. The considerable mass loss in the range of 220 to 580 °C for HA-F127 sample is due to the thermal decomposition of the grafted F127. The neat and modified HA sample reaches to 97.51% and 93.84% char value at 700 °C. Thermal decomposition of F127 is observed gradually in the temperatures range 220–580 °C. Also, weight loss at the dehydroxylation step is lower for HA-F127, which results from the covalent reaction of hydroxyl groups with F127. Moreover, pristine F127 completely pyrolyzes before the beginning of surface and structural OH groups of hydroxyapatite dehydroxylation. Compared to pristine F127 degradation temperature, the mass loss of attached F127 chains in HA-F127/PCL/P123 TGA curve obviously shifts to higher temperature and the thermal degradation temperature remarkably increases from 245 to 300 °C. This may be due to the decrease in mobility of F127 chain grafted to hydroxyapatite nanoparticles. The amount of F127 grafted on the HA nanoparticle surfaces was about 4 wt%.
The surface modification of HA nanoparticle should occur only at its surface, in order to keep the state of the bulk properties such as crystallinity and the crystalline phase, intact. If the chemical reaction alters the state of the bulk properties the resulting HA nanoparticle loses its intrinsic properties. Thus, confirmation of the selective reaction on the HA nanoparticle surface and the maintenance of crystalline properties are important. XRD was used to characterize the crystallinity of HA and HA-F127 samples. As shown in Fig. 4, the characteristic diffraction peaks of the (002), (211), (300), (202), (310), (222), (213), and (411) crystal planes of HA nanoparticle is not different from that of HA-F127. This observation demonstrated that grafting reaction did not alter the crystalline structure of HA nanoparticles. However, intensity of the mentioned peaks decreases by a considerable value as a result of polymer grafting. Similar observation has been made in Hemmatpour et al. study.35 They stated that grafting poly (N,N-dimethyl amino ethyl methacrylate) on halloysite nanotube surface diminishes the intensity of the halloysite characteristic peaks. Halloysite, a naturally occurring polymorph of kaolinite, have hydroxyl as its surface functional groups similar to hydroxyapatite.
Transmission electron microscopy (TEM) was employed to study the morphology, size and dispersion of nanoparticles. Fig. 5 demonstrates that HA-F127 have spherical morphology with diameter of about 60 nm. Keen observation on the related TEM images of modified HA nanoparticles reveals once again a spherical morphology plus a 13 nm thick F127-COOH layer with smooth appearances, comprising a well formed core shell structure. This corona is more transparent than the HA nanoparticle, resulted from easier electron transfer, suggesting that shell composition is organic. Therefore successful surface modification of HA nanoparticles with F127-COOH chains can be concluded from TEM images.
The TEM images of HA and HA-F127 nanoparticles dispersed in ethanol with smaller magnification are shown in Fig. 6. The agglomerates of HA nanoparticles are evident from Fig. 6a while finely dispersed HA-F127 nanoparticles constructs the morphology presented in Fig. 6b. This can be attributed to the immobilization of F127 chains on HA surface, which improves their distribution and dispersion in solvent media by reducing the particle/particle interactions.
Investigation on colloidal stability of HA samples is important because HA nanoparticles tend to aggregate due to van der Waals interactions as well as hydrogen bonding of surface hydroxyl groups. These possibilities can result in rapid precipitation of HA nanoparticles after distribution in the solvent media.36 Furthermore, to achieve a homogenous nanocomposite, high colloidal stability is crucial during the electrospinning of HA/polymer suspension. Monitoring of time-dependent colloidal stability of HA and HA-F127 in chloroform is illustrated in Fig. 7. After being stirred for 4 h in chloroform at room temperature, all HA and HA-F127 dispersed and suspended in the solvent. However, the aggregation and precipitation of HA nanoparticles started immediately after the stirring process halted. In the case of HA-F127 nanoparticles, the suspension remained fairly stable up to several hours, due to the non-polar interactions between the stretched F127 brushes and chloroform molecules. It is noteworthy to mention that F127 solubilizes in chloroform rather than forming stable micelles. In fact, the amphiphilic characteristic of the HA-F127 shell, inherited from F127, can cause colloidal stability in both aqueous and non-aqueous media. The existence of a polymer layer on the surface of modified HA nanoparticles overwhelms the overall HA density and inter-particle interactions, which favors the stability of nanoparticles in the solvent media. This argument is in good agreement with the dispersion state of nanoparticles in the TEM images.
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Fig. 7 Monitoring of time-dependent colloidal stability of HA and HA-F127: (a) 5, (b) 30, (c) 60 minutes, and (d) 12 hours. |
The differential scanning calorimeter (DSC) test was performed to determine the thermal properties of electrospun nanocomposites. DSC experiments included a heating scan that gives information about the crystalline structure with electrospinning process history. This scan was performed between −60 °C and 120 °C. This was followed by a cooling procedure before the finale second heating scan which was recorded to characterize the structure of the polymer crystallized from the melt without the electrospinning process history. The thermal behavior of nanocomposites was characterized and the data were summarized in Table 1.
Samples | First heat scan | Second heat scan | δ | ||||
---|---|---|---|---|---|---|---|
ΔH′ (J g−1) | % Xc | Tm (°C) | ΔH′′ (J g−1) | % Xc | Tm (°C) | ||
PCL/P123 | 53 | 42.37 | 58.13 | 40 | 31.98 | 53.92 | 13 |
HA/PCL/P123 | 60 | 47.97 | 58.14 | 42 | 33.58 | 54.00 | 18 |
HA-F127/PCL/P123 | 77 | 61.55 | 59.63 | 55 | 43.97 | 55.01 | 22 |
During the first heating scan the crystallinity of PCL is affected by three parameters including the electrospinning process, imparting induced crystallization to PCL chains placed on the surface of developing jet, existence of HA nanoparticles in the vicinity of evolving PCL crystals and finally the HA surface modification. The latter has a drastic effect on the PCL nucleation and confined crystallization. The area under the DSC thermograms related to the PCL melting transition for different electrospun samples has been calculated. The difference between the mentioned area during first and second heat scans was obtained by the following equation described elsewhere:28
δ = ΔH′ − ΔH′′ |
Parameter δ considerably increases for samples containing HA nanoparticles. This parameter signifies the electrospinning process effect on the formation of PCL crystals. The mentioned increment of parameter δ for HA/PCL/P123 and HA-F127/PCL/P123 samples in comparison with the PCL/P123 sample should be investigated through the effect of the presence of HA nanoparticles on the electrospinning solution properties. Inertness of HA nanoparticles dismisses the idea of these particles can be affected in the electrical field during electrospinning process, forming an aligned arrangement and consequently changing the amount of PCL crystallinity. However, incorporation of nanoparticle into electrospinning solution has a drastic effect on the overall viscosity.39 Simultaneously, due to the direct relationship between solution viscosity and shear rate, it can be postulated that presence of nanoparticles in the electrospinning solution enhances polymer chain alignment and induced crystallization. This can be the reason behind the observed increase in parameter δ by introducing HA nanoparticles into solution. Moreover, increased solution viscosity is expected when using modified nanoparticles which can establish strong polymer/particle and solvent/particle interfacial interaction. Therefore, by the same logic, incorporation of HA-F127 should have a more pronounced effect on solution viscosity, the resulted shear rate and finally induced crystallization of PCL chains in comparison with neat HA; justifying the observed 4 unit increase of parameter δ (see Table 1).
TGA and dTG curves of PCL/P123, HA/PCL/P123 and HA-F127/PCL/P123 were obtained (ESI Fig. 1†). The related weight loss of P123 which normally occurs in the range of 300 to 350 °C is merged with that of PCL which happens in the range of 350 to 450 °C. This may be due to the excellent compatibility and miscibility of these two polymers which approximate their thermal stability. In addition, synergistic interactions between PCL and P123 chains at 90/10 blend ratio have been reported previously and can also explain the mass loss behavior of PCL/P123.28 Blend of PCL and P123 fully pyrolyzes at the final temperature (700 °C). As a result, the final residual weight of nanocomposites corresponds to the neat and modified hydroxyapatite weight in their related TGA curves. The percentage weight of hydroxyapatite nanoparticles embedded in the HA-F127/PCL/P123 differs slightly from that of HA/PCL/P123 (0.5 wt%). Considering the results from colloidal stability experiment, this observation was anticipated as neat hydroxyapatite nanoparticles tend to precipitate in the polymer solution during the electrospinning process. Therefore, the initial concentration of neat hydroxyapatite nanoparticles used to fabricate the HA/PCL/P123 changes in the final scaffold. Surprisingly, the percentage weight of modified hydroxyapatite nanoparticles implanted in HA-F127/PCL/P123 suggests that most of the initially added HA-F127 nanoparticles enter the PCL/P123 fibers.
Scaffold manageable handling and load endurance are crucial during cell culture and therefore mechanical properties of the nanofibrous membrane play an important role on its successful application in tissue engineering. In most bone tissue engineering approaches, improving mechanical properties by incorporation of nanoscale reinforcements into substrates has been proven to be most effective. At high filler contents agglomeration of nanoparticle is inevitable due to the strong interactions between the nanoparticles themselves and therefore low filler content must be beneficial to the satisfactory dispersion of the nanoparticles for both untreated and grafted HA. The mechanical properties of nanocomposites mostly depend on the characteristics of components, composition, structure and interfacial interactions between the constituents.
Based on the typical stress–strain curves of the electrospun fibrous scaffolds (Fig. 9), tensile strength, elongation at break, and Young's modulus could be calculated (Table 2). Electrospun fibrous scaffolds containing nanoparticles show higher Young's modulus whereas their elongation at break is less than that of PCL/P123 sample. It is noteworthy to mention that adding HA nanoparticles to PCL/P123 results in decrease in tensile strength, implying that HA/PCL/P123 is more brittle than PCL/P123. This can be explained by heterogeneous distribution of HA nanoparticles, agglomerates and weak particle/matrix interfacial adhesion. On the contrary, for the samples containing the same amount of reinforcing phase, HA-F127/PCL/P123 shows higher tensile strength and Young's modulus which confirms the remarkable role of grafted F127 chains in enhancing mechanical properties of nanocomposite by reducing the particle–particle interactions and increasing particle–matrix interactions. This leads to uniform dispersion of nanoparticles, enhanced interfacial crystallization and consequently improved interfacial adhesion. Interfacial interactions can be described in a more quantitative way using the experimentally determined tensile properties. The theoretical model proposed by Pukánszky40,41 gave a quantitative relation between tensile strength and interfacial interaction as
Samples | Tensile strength (MPa) | Young's modulus (MPa) | Elongation at break (%) | Bσy |
---|---|---|---|---|
PCL/P123 | 3.6 ± 0.2 | 4.6 ± 0.4 | 163.4 ± 6.7 | — |
HA/PCL/P123 | 3.0 ± 0.2 | 6.6 ± 0.1 | 88.1 ± 5.3 | −1.15 ± 0.15 |
HA-F127/PCL/P123 | 5.0 ± 0.3 | 10.2 ± 0.2 | 103.8 ± 4.4 | 11.61 ± 0.11 |
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Fig. 10 Cell adhesion and proliferation on various classes of substrates: asterisk shows significant difference with p < 0.05. |
Einteraction = Enanocomposite − Ematrix − Enanoparticle |
The interaction energy of the nanoparticle with the polymer chains in each system was calculated, and results were displayed in Table 3. Interactions of PCL/P123 chains with HA-F127 are about 1.5 times larger than that of the pure HA (absolute value). By comparing these values and since more negative interaction energy indicates larger attraction, it can be concluded that the interaction between HA-F127 and PCL/P123 chain is stronger than that of pristine HA. Elevated interaction energy of HA and polymer substrate after the modification process promises better distribution and dispersion of nanoparticles in fibrous scaffold. This speculation was confirmed by the results from the colloidal stability of the modified HA nanoparticles and the interfacial interaction parameter calculated from Pukanszky model and are in line with the MD simulations data.
System | Enanocomposite | Ematrix | Enanoparticle | Einteraction |
---|---|---|---|---|
HA/PCL/P123 | 1![]() ![]() |
7755.181379 | 1![]() ![]() |
−37![]() |
HA-F127/PCL/P123 | 1![]() ![]() |
13![]() |
1![]() ![]() |
−56![]() |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c6ra19499k |
This journal is © The Royal Society of Chemistry 2016 |