Kaili Lin*a,
Chucheng Linb and
Yi Zengb
aSchool & Hospital of Stomatology, Tongji University, Shanghai Engineering Research Center of Tooth Restoration and Regeneration, 399 Middle Yanchang Road, Shanghai, 200072, China. E-mail: lklecnu@aliyun.com; Fax: +86-21-66524025; Tel: +86-21-56722215
bAnalysis and Testing Center for Inorganic Materials, Shanghai Institute of Ceramics, Chinese Academy of Sciences, 1295 Dingxi Road, Shanghai 200050, China
First published on 27th January 2016
The biodegradable wollastonite (CaSiO3, CS) bioceramics can stimulate the growth and osteogenic differentiation of osteoblasts and bone marrow mesenchymal stem cells (BMSCs), and possess excellent bone regeneration ability in vivo. However, their mechanical properties are apparently lower than that of the cortical bone which has hindered their wider clinic applications. In the present study, CS bioceramics with high bending strength were fabricated by pressureless sintering using wollastonite nanofibers as raw materials. The bending strength of the samples sintered at 1100 °C for 3 h reached 145.70 ± 2.74 MPa, i.e., the upper limit value of human cortical bone. This results from the good sinterability of nanofibers and the fiber self-reinforcement in the sintered matrices. The in vitro simulated body fluid soaking result showed that the fabricated CS bioceramics could induce a fast formation of bone-like apatite layers. Our results suggest that CS bioceramics sintered from nanofibers might be used as bioactive materials under load-bearing applications in the clinical field.
To date, most bioceramics and their composites have typically been implanted in the form of granules, scaffolds or bulk materials. However, the mechanical properties of pure CS bioceramics are lower than those of cortical bone, which has hindered the wide use of CS bioceramics for clinical applications.1
Therefore, there is a need to increase the mechanical properties of CS bioceramics. Several methods have been used to overcome this obstacle, such as using two-dimensional graphene nanosheets and Si3N4 particles as reinforcements.22,23 However, graphene and Si3N4 are bioinert and non-biodegradable, which might hinder the bioactivity and biodegradability of final products. Sintering method is another effective approach for improving the mechanical properties of ceramic-based materials.24–26 The spark plasma sintering (SPS) technique has been successfully applied to improve the mechanical properties of CS bioceramics.25,26 During the SPS process, an ultrahigh, pulsed electric current in a high-pressure environment yields high ceramic powder sintering activity, which accelerates the densification process and ultimately produces samples with a smaller grain size and higher density.27 Decreasing grain size and increasing density lead to improved mechanical properties. However, the SPS technique requires special and extremely expensive equipment.
Herein, pure CS bioceramics with a high bending strength of 145.70 ± 2.74 MPa, i.e., the upper limit value of human cortical bone, were fabricated via a simply pressureless sintering using wollastonite nanofibers as raw materials. In addition, the in vitro bioactivity of the fabricated samples was evaluated using the SBF-soaking method.
The sintered CS bioceramics were soaked in SBF for 3 days at 37 °C with a surface area (cm2) to solution volume (cm3) ratio of 0.1. The SBF solution was refreshed every day. After soaking, the CS bioceramics were removed from the SBF solution, gently rinsed with distilled water, and then dried at room temperature prior to further characterization.2 The formation of bone-like apatite layers on the surfaces of the CS bioceramics was demonstrated by FESEM, XRD and Fourier transform infrared spectroscopy (FTIR; Nicolet Co., USA).
The synthetic CS nanofibers were used as raw materials to fabricate the CS bioceramics. Table 1 presents the effect of sintering temperature on the linear shrinkage, porosity and bending strength of the ceramic samples. The linear shrinkage of the samples increased from 10.65% to 14.94% with an increase in sintering temperature from 1050 to 1150 °C; linear shrinkage slightly decreased to 13.07% with a further increase of sintering temperature to 1200 °C. As expected, the porosity of the samples was observed to decrease with the increase of sintering temperature from 1050 to 1100 °C, and porosity decreased slightly with further increase of sintering temperature. While the bending strength of the fabricated CS bioceramics increased with the sintering temperature increase from 1050 to 1100 °C, reaching a maximal value of 145.70 ± 2.74 MPa, it then decreased with a further increase the sintering temperature up to 1200 °C. However, it is hard to understand that the linear shrinkage decreased with the increase of the sintering temperature from 1150 to 1200 °C, which needs to be further investigated in details.
Sintering temperature (°C) | 1050 | 1100 | 1150 | 1200 |
Linear shrinkage (%) | 10.65 ± 0.62 | 11.41 ± 0.80 | 14.94 ± 0.97 | 13.07 ± 1.20 |
Porosity (%) | 22.79 ± 0.33 | 11.39 ± 0.49 | 9.67 ± 0.28 | 9.49 ± 0.53 |
Bending strength (MPa) | 51.12 ± 3.36 | 145.70 ± 2.74 | 93.90 ± 5.15 | 52.93 ± 8.42 |
Fig. 3 shows the fracture surfaces of the ceramic samples sintered at various temperatures ranging from 1050 to 1200 °C for 3 h. The samples sintered at 1050 °C were highly porous with evenly distributed micropores in range of 0.1–0.4 μm in diameter, and the samples were completely constructed of fiber-like crystals with diameters of 30–100 nm and lengths up to several micrometers (Fig. 3A). The number of the micropores decreased remarkably with the increase of sintering temperature to 1100 °C. Moreover, a few fiber-like grains with diameters of 0.4–0.8 μm were still distributed among the sintered matrices. In addition, fiber debonding and pulling-out phenomena could be clearly observed from the fracture surface (Fig. 3B). Increasing the sintering temperature to 1150 °C, the fracture surfaces presented continuous phases accompanied by the formation of spherical pores with diameters of 0.3–1 μm, which demonstrated that a liquid phase had been formed. Meanwhile the amount of the fiber-like crystals decreased remarkably (Fig. 3C). With a further increase of sintering temperature to 1200 °C, the fracture structure with liquid phase phenomenon was maintained. While the sizes of the sphere-like micropores decreased apparently to 0.2–0.4 μm, and the micropores were uniformly distributed within the sintered matrices. Moreover, the fiber-like crystals disappeared completely (Fig. 3D).
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Fig. 3 The fracture images of samples sintered at 1050 °C (A), 1100 °C (B), 1150 °C (C) and 1200 °C (D) for 3 h. The black arrows were the fiber-like grains distributed among the sintered matrices. |
Fig. 4 shows the surface morphologies of the ceramic samples sintered at 1100 °C for 3 h before and after soaking in SBF. It can be clearly observed that large numbers of fiber-like crystals with diameters of 0.2–1 μm and lengths up to 5 μm were uniformly distributed within the sintered samples before soaking (Fig. 4A). After soaking in SBF for 3 days, the samples were completely covered by a dense layer (Fig. 4B). The high magnification image inserted in Fig. 4B illustrates that the newly formed layer consisted of finely structured worm-like particles with a diameter of 50 nm and lengths up to 200 nm.
Fig. 5 presents the XRD spectra of the sintered ceramic samples before and after soaking in SBF for 3 days. The results indicated that the samples sintered at 1100 °C for 3 h were β-wollastonite (β-CaSiO3, β-CS) phase (JCPDS card: no. 84-0655) (Fig. 5A). After soaking the samples in SBF for 3 days, the intensity of the β-CS peaks decreased, while the typical diffraction peaks of hydroxyapatite [Ca10(PO4)6(OH)2, HAp] (JCPDS card: no. 09-0432) appeared, suggesting that the newly formed layers were bone-like apatite.
FTIR was used to further characterize the surface properties of the fabricated β-CS bioceramics before and after soaking in SBF (Fig. 6). Before soaking, the intense peaks between 908 and 1085 cm−1 could be attributed to silicate (Si–O–Si) absorption peaks, and the peaks at 686, 645, 565, and 454 cm−1 were attributable to the bending mode of Si–O–Si.2,9 After soaking in SBF for 3 days, the intensity of the silicate (Si–O–Si) absorption peaks decreased remarkably. The newly appeared peaks at 1113 and 1035 cm−1 could be attributed to the phosphate groups (PO43−) of the deposited apatite layers, the peaks at 1505 and 1420 cm−1 corresponded with the absorption peaks for carbonate group (CO32−), and those at 3403 and 1644 cm−1 resulted from adsorbed water molecules.2,9 The FTIR spectra further demonstrated that the layers deposited on the sintered CS bioceramics after soaking in SBF were bone-like hydroxycarbonate apatite (HCA). The formation of a bone-like HCA layer on the surface of a bioactive material is considered to play an essential role in tight bone bonding between bioactive materials and neighboring tissues.2,9,13 In the present study, the results suggested that the CS bioceramics sintered from nanofibers could induce the rapid formation of bone-like HCA layers, indicating the excellent bioactivity of the fabricated samples.
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Fig. 6 FITR spectra for the samples after soaking CS bioceramics sintered at 1100 °C for 3 h in SBF for 0 (A) and 3 days (B). |
The present study confirmed that the bending strength of pure CS bioceramics fabricated from CS nanofibers reached 145.70 ± 2.74 MPa, i.e., the upper limit value of human cortical bone, which was approximately 2.2 times as high as that of the samples sintered from micro-sized particles by a similar sintering process, and was similar to that of the samples reinforced by the bioinert Si3N4 particles. Recently, Zeng et al.29 reported the improved mechanical properties of CS bioceramics using Si3N4 as reinforcement. In their study, the optimal bending strength reached 157.2 MPa with the addition of 3 wt% Si3N4. However, the inert reinforcement might hinder the bioactivity and biodegradability of final products.
The excellent bending strength observed in the present study resulted from the high sinterability of the nanofibers and from the fiber self-reinforcement in the sintered matrices. It is well known that nano-sized powders possess a much higher driving force for densification due to their enormous surface area compared with micro-sized powders, and this driving force accelerates rates of densification and grain boundary motion.30 Differences in raw powder sintering ability lead to significant differences in the relative densities and microstructures of the resulting sintered matrices; these differences ultimately influence the mechanical properties of the sintered matrices.30
In general, the porosity and grain morphology are the key factors affecting the strength of the ceramics.2 The bending strength of the ceramic materials appeared to increase with decreasing the porosity of the sintered matrices. In the present study, the porosity of the CS bioceramics pressurelessly sintered from nanofibers at 1100 °C for 3 h was 11.39%, which was apparently lower than that of the samples sintered from micro-sized particles due to the better sintering ability of the nanofibers. However, it is still difficult to fabricate the fully dense CS bioceramics, even at higher sintering temperatures, using nanofibers as raw materials due to low sintering ability for CS material.1 The higher sintering temperatures might decrease the porosity of the samples. In contrast, the over-high sintering temperatures resulted in liquid phase formation, which ultimately decreased the bending strength.
The XRF determination result showed that the obtained CS nanofibers contained 0.68 wt% sodium (Na). The residual Na element came from the Na2SiO3 using as raw material in the synthetic process of wollastonite nanofibers. The residual sodium component might play as the driving force for the formation of liquid phase during sintering, which apparently enhanced the densification process and also modified the microstructures of the sintered matrices.31 The sodium element always presents in the final calcium silicate products when the raw materials containing sodium component were used.31–33. However, the previous studies have shown that it is still difficult to obtain fully dense CS bioceramics using this kinds of CS powders containing sodium element or even using Na2O as sintering additive.1,34 In the present study, the CS bioceramics with higher density could be facilely fabricated using nanofibers as raw materials comparing with the micro-sized powders. Therefore, it can be concluded that using the nanofibers as raw materials can accelerate the densification process.
Moreover, the fiber-like grains that remained in the sintered matrices further increased the bending strength of the obtained samples by acting as self-reinforcements. The fiber-like grains serve as reinforcements in the fabricated CS bioceramics by not only hindering crack propagation but also resisting the interfacial shear stress that otherwise results in fiber debonding and pulling-out during bending strength tests.1,30,35–37 It is believed that the fiber-like grains played a dominative role in the mechanical properties among the factors of porosity, grain size, and grain morphologies.9 The present study confirmed that pure CS bioceramics with high mechanical strength could be facilely fabricated by pressureless sintering using CS nanofibers as raw materials. It can be predicted that the mechanical strength of the nanofiber derived CS bioceramics might be further improved via increasing their density. Our present study showed that the CS bioceramics with a relative density of about 95% fabricated using spark plasma sintering (SPS) technique expresses excellent bending strength of about 294 MPa.25
The SBF soaking results demonstrated that the CS bioceramics sintered from nanofibers could induce the rapid formation of bone-like HCA layers, indicating the excellent bioactivity of the fabricated CS bioceramics. The formation of a bone-like HCA layer is considered to play an essential role in tight bone bonding between bioactive materials and neighboring tissues.13,38–40 Our results suggest that CS bioceramics sintered from nanofibers might be used as a bioactive material for clinical load-bearing applications. In addition, it is considered that the major drawback of CS bioceramics is their high dissolution rate. More importantly, the dissolution rate of calcium silicate bioceramics can be modified by incorporation of different elements such as Zn, Mg, Sr, Ti and Zr etc.41,42 Therefore, we can expected that the high mechanical strength calcium silicate bioceramics with regulated degradation rate might be fabricated using the calcium silicate nanofibers containing these kinds of elements. However, the degradation rate of the CS bioceramics fabricated from nanofibers and the effect of the element incorporation on their degradation should be further investigated in details.
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