Abstract
The piezoelectric effect of biological piezoelectric materials promotes bone growth. However, the material should be subjected to stress before it can produce an electric charge that promotes bone repair and reconstruction conducive to fracture healing. A novel method for in vitro experimentation of biological piezoelectric materials with physiological load is presented. A dynamic loading device that can simulate the force of human motion and provide periodic load to piezoelectric materials when co-cultured with cells was designed to obtain a realistic expression of piezoelectric effect on bone repair. Hydroxyapatite (HA)/barium titanate (BaTiO3) composite materials were fabricated by slip casting, and their piezoelectric properties were obtained by polarization. The d33 of HA/BaTiO3 piezoelectric ceramics after polarization was 1.3 pC/N to 6.8 pC/N with BaTiO3 content ranging from 80% to 100%. The in vitro biological properties of piezoelectric bioceramics with and without cycle loading were investigated. When HA/BaTiO3 piezoelectric bioceramics were affected by cycle loading, the piezoelectric effect of BaTiO3 promoted the growth of osteoblasts and interaction with HA, which was better than the effect of HA alone. The best biocompatibility and bone-inducing activity were demonstrated by the 10%HA/90%BaTiO3 piezoelectric ceramics.
Hydroxyapatite (HA) is widely used in the fabrication of bone repair materials because of its similarity to the inorganic components of human bone and its biological activity1,2. HA has been used in numerous studies to prepare porous scaffolds for bone substitute materials3,4. The nano-HA coating on the surface of metal (such as Ti alloy) was also prepared based on the bionic human bone composition5. The surface and volume effects of the nanomaterials are easy to produce and stabilize using other atoms to promote bone cell growth. Performance improvement of HA by inducing the collagen, growth factor, and other bio-inspired organic compounds has also been studied6,7. Existing studies have continuously optimized the composition and structure of HA bioactive materials, but the biological properties of these materials are based on the osteoacusis of HA8,9. Numerous clinical trials have shown that the bone induction of HA was low. The growth cycle of new bones induced with HA usually takes half a year to one year, which is not conducive to the early activities of patients after surgery especially those in the middle- and old-age groups10,11,12.
The human bone tissue is also a type of piezoelectric material, that is, the composition of the human body can produce biological electricity owing to the electron displacement of the local electric field produced by deformation force13,14,15. This electrical activity will affect many biochemical reactions in the body, and energy conversion can be achieved in the process during these biochemical reactions. The effect of external force on the human body is transmitted by biological electricity. Biological electricity also affects the growth factor and extracellular matrix, which in turn can affect bone reconstruction and repair16. On the basis of the piezoelectric properties of biological tissues, some works used piezoresponse force microscopy (PFM) to investigate localized piezoelectric behavior17,18. In addition, in the aspect of piezoelectric effect, the use of BaTiO3 as a hard tissue replacement material has been reported19, and in vivo animal experiments have shown its good biocompatibility. BaTiO3 after polarization can lead to calcium phosphate deposit20. The surface cell adhesion and proliferation of polarizing HA were also investigated. Findings indicate that the surface of polarized HA can bond inorganic ions and organic cell adhesive proteins, thereby resulting in accelerated mineralization and cell adhesion and proliferation on the polarized HAp surface21,22. BaTiO3, CaTiO3, and HA composites can also be used as bone repair materials, and an in vitro cell experiment found that the introduction of piezoelectric phase could promote the adhesion and proliferation of mouse fibroblast L929 and human osteoblast SaOS223. HA/BaTiO3 composites can also be made into porous structures24, and the piezoelectric effect increases with the increase of BaTiO3 content. Moreover, in vitro experiments showed that composites had no cytotoxicity and had good biological activity. All these studies and findings show that the introduction of piezoelectric materials can induce bone growth25,26,27. During in situ loading on the animal bone, the mineralization behavior in simulated body fluid was observed, thereby indicating that the piezoelectric effect of bone promotes mineralization28,29. However, biological experiments have not considered how the growth of bone cell is promoted by the effect of piezoelectric material with physiological loading (cycle loading). In particular, the piezoelectric properties of the samples are actually in the residual polarization rather than the piezoelectric effect of the piezoelectric material.
A novel method for in vitro experiment of biological piezoelectric material with physiological loading is presented in this paper. A dynamic loading device for piezoelectric bioceramics based on the human activity cycle was designed; this device can mimic human motion to a given physiological loading to materials periodically when co-cultured with cells and can express the influence of the piezoelectric effect for bone repair accurately. Composite materials with different piezoelectric properties were obtained by adjusting the ratio of HA and BaTiO3. During simulated body fluid (SBF) immersion and co-culture with cells, physiological loading was applied on the surface of HA/BaTiO3 composites quantitatively and periodically. The deposition of HA and the adhesion of osteoblasts on the surface of composites with and without cycle loading were observed, and the proliferation and activity of osteoblasts were characterized.
Results and Discussion
Morphologies and phase composition of HA/BaTiO3 composite materials
Figure 1 shows the morphologies of HA/BaTiO3 composite materials with various compositions. After sintering, the grain growth of each composite group was uniform, and a gap was present between the grains. Morphologies of 100% BaTiO3 and 100% HA showed similar grain size without excessive growth, which had a positive effect on the performance of biological materials to ensure stability. The BaTiO3 particles accounted for the majority in 90% BaTiO3/10% HA and 80% BaTiO3/20% HA composites. BaTiO3 particles in the composite were connected to form the network, which was conducive for obtaining the overall piezoelectric effect30.
Figure 2 shows the X-ray diffraction (XRD) patterns of HA/BaTiO3 composite materials with various compositions sintered at 1250 °C. Diffraction peaks of 100% BaTiO3 after sintering were in agreement with the standard JCPDS card no. 5–626, and the diffraction peak of 100% HA were in agreement with JCPDS 9–432, thereby indicating that the phase composition of BaTiO3 and HA did not change during sintering. Compared with the 100% BaTiO3 group, some diffraction peaks of BaTiO3/HA composite materials appeared weak, thereby indicating the presence of HA. The diffraction peak of HA increased with HA content.
Piezoelectric and mechanical properties of HA/BaTiO3 composite materials
Figure 3(a) shows the effects of polarization time on the piezoelectric coefficient (d33) of 90%BaTiO3/10%HA piezoelectric bioceramics. The d33 of BaTiO3/HA piezoelectric ceramics initially increased with the increasing polarization time and then remained constant. The polarization of piezoelectric ceramics is the process in which the spontaneous polarization direction of the electric domain turns to the direction of the external electric field. The steering and orientation of the electric domain were gradually completed31,32. With the increase of the polarization time, the electric domain gradually overcame resistance to orientation, and the d33 increased. However, when the polarization time is more than 30 min, the d33 remained constant because the interfacial polarization, ion displacement polarization, inversion of the 180° domain, and shift of the 90° domain were completed. Figure 3(b) shows the influence of polarization temperature on the piezoelectric constant of 90%BaTiO3/10%HA composites. The d33 significantly increased with the increasing polarization temperature but remained constant after the temperature reached 130 °C33. The formation of electric domains has a tendency to follow the preferential orientation of the external electric field. In the phase transition, the newly formed electric domain orientation along the direction of the external electric field is more likely to be easier than that of the electric domain that has been formed. Obtaining a high piezoelectric constant is easier at a high temperature than at room temperature (25 °C). However, 130 °C is the Curie point temperature of BaTiO3, and the d33 did not increase at higher polarization temperatures. Figure 3(c) shows the optimization of polarized electric field intensity of 90%BaTiO3/10%HA composites. The d33 increased with increasing polarized electric field intensity. The d33 maintained a constant maximum value of 2.7 pC·N−1 when the polarization field strength exceeded 1.2 kV·mm−1. The polarization and ferroelectric to paraelectric phase transition occurred at the same time. The electric domain is the preferred orientation in the formation process, and it arranged along the direction of the external electric field. However, the preferred orientation of the electric domains was disturbed and changed because the grains were active at high temperature34. The high electric field intensity could decrease the direction changes of the electric domain; hence, a lower limit of the electric field intensity exists. Through the optimization of different polarization conditions, the optimal polarization process was obtained for the polarization time of 30 min, polarized electric field intensity of 1.2 kV·mm−1, and polarization temperature of 130 °C. Other composite materials (BaTiO3 content is 80% or 100%) showed the same variation. To ensure comparability between the four groups, the optimized polarization process was used for the polarization of all samples; the results are shown in Fig. 3(d). With the reduction of the BaTiO3 content, the d33 decreased from 6.8 to 1.3 pC·N−1, and that of the 100% HA group was 0. The piezoelectric coefficient d33 of 90% BaTiO3/10%HA composites is close to that of the human bone range from 0.7–2.3 pC/N35.
Table 1 shows the compressive strength of HA/BaTiO3 with different BaTiO3 contents. Note that 100% BaTiO3 and 100% HA groups have high compressive strengths, namely, 28.4 and 21.8 MPa, respectively. The compressive strengths of HA/BaTiO3 composites are lower than those of pure BaTiO3 or HA because HA dispersed in the BaTiO3 phase and chemical reaction did not occur in the sintering process but in the formation of a physical combination. Moreover, HA hindered the sintering densification process of BaTiO3.
Table 1. Compressive strengthens of HA/BaTiO3 composites with different BaTiO3 contents.
Composition/wt% | Compressive strength/MPa |
---|---|
100% BaTiO3 | 28.4 ± 3.21 |
90% BaTiO3/10% HA | 21.8 ± 2.62 |
80% BaTiO3/20% HA | 16.2 ± 1.99 |
100% HA | 21.8 ± 3.01 |
In vitro characterization of HA/BaTiO3 piezoelectric bioceramics without loading
The formation of bone-like apatite by Ca and P ion deposition in the body fluid is an important advantage of the bioactive materials for use as bone implants36,37. Bone-like apatite plays an important role in the formation of new bone because it serves as the transition and bonding layer between the implant material and new bone. The absorption of ions and proteins in the blood is beneficial to the adhesion of bone cells and provides a suitable surface for the growth of new tissue38. Negative surface morphologies of HA/BaTiO3 piezoelectric bioceramics after 7 days of immersion in SBF are shown in Fig. 4. Some particles were deposited on the surface of the four groups after soaking. The particle size was much smaller than that of the grains shown in scanning electron microscopy (SEM) photos before soaking. The particles can be speculated to be bone-like apatite particles39. However, in the four groups of materials, the deposition amount of HA was more than that in the group that contained BaTiO3. This finding shows that the biocompatibility of HA is higher than that of BaTiO3, and no obvious difference exists between the three groups that contained BaTiO3. HA was degraded slowly after contact with SBF, few calcium and phosphate ions on the HA surface was formed. but calcium and phosphate ions in SBF will be enriched to the surface of HA. When the Ca ion concentration reached the critical value of the bone-like apatite nucleation, the nucleation formed and grew spontaneously40. However, the amount of deposition and its induction ability were not yet determined.
The morphology of osteoblasts on the surface can directly reflect the biological activity of the material41. Figure 5 shows the growth of osteoblasts on the negative surface of HA/BaTiO3 piezoelectric bioceramics without loading after co-culture for 3 days. Osteoblasts are polygonal and distributed on the material surface, and the pseudopodium is connected with piezoelectric bioceramics and neighboring osteoblasts. The cells associated with each sample showed excellent growth, including good cell morphology, extracellular secretions, and intercellular connections. An insignificant difference in the growth of osteoblasts on the surface of HA/BaTiO3 piezoelectric bioceramics with different contents was observed, thereby showing that the BaTiO3 also had biological activity. HA is a widely used bone substitute material, and its biological activity is generally recognized. A comparison of the HA group with the other three groups that contained BaTiO3 demonstrated no obvious differences in osteoblast growth.
Figure 6(a) shows the MTT assay of HA/BaTiO3 piezoelectric bioceramics without loading after co-culture with osteoblast cells. The absorbance values of the four groups increased with the increase of cell culture time. The number of living cells increased as the culture time increased. Insignificant differences in the absorbance values were observed between the 4 groups at 1, 4, and 7 days, thereby showing that the number of living cells at the same time was insignificantly different. When the BaTiO3 content of HA/BaTiO3 composite piezoelectric ceramics was in the range of 80% to 100%, the composite piezoelectric ceramic had the same biocompatibility as the pure HA. In the experiment, although primary osteoblasts were not induced by osteogenic medium, the ALP enzyme on the sample surface could still be differentiated and synthesized. The ALP activity of HA/BaTiO3 piezoelectric bioceramics without loading after co-culture with osteoblasts is shown in Fig. 6(b). The ALP activity of osteoblasts increased as the culture time increased. The ALP activity of osteoblast on HA surface was significantly higher than in the other three groups, and the difference was statistically significant (p < 0.05). When the BaTiO3 content of HA/BaTiO3 composite piezoelectric ceramics ranged from 80% to 100%, the bone induction activity of the composite was worse than that of HA.
In vitro characterization of HA/BaTiO3 piezoelectric bioceramics with cycle loading
To simulate the physiological loading of the human body, cyclic loading was applied to the surface of each group. Figure 7 shows the morphologies of HA/BaTiO3 piezoelectric bioceramics after SBF immersion for 7 days. After soaking, some particles were deposited on the surfaces of the four groups, which was similar to the result without loading. These particles could be the bone-like apatite. In the dynamic loading process, the electric charge bound on the negative surface of composite piezoelectric ceramics (80% to 100% BaTiO3) changed alternately with the piezoelectric properties, and the attraction of the positive ions (Ca2+) can also change during circulation. The electric charge attracted the positive ions attached to their negative surface gradually42,43. The HA in composite piezoelectric ceramics also induced the deposition of bone-like apatite. Thus, the amount of bone-like apatite on the negative surface of composite piezoelectric ceramics was larger than that of the non-loaded bioceramics.
Figure 8 shows the morphologies of HA/BaTiO3 piezoelectric bioceramics with cycle loading after co-culture with osteoblast cells for 3 days. The density of osteoblasts on the surface of piezoelectric bioceramics that contained 80% or 90% BaTiO3 was significantly higher than that of 100% HA and 100% BaTiO3, and the number of pseudopodia was greater. Cells were spread on the surface of the four groups and had pseudopodia (insert images). According to the principle of piezoelectric effect, the piezoelectric material can generate free charge on the surface of the material only under the loading condition. HA/BaTiO3 piezoelectric bioceramics are used for bone defects, thereby generating free charge on the surface under loading action. The electric force effect of the bone acted on the microenvironment, which can increase the bone formation protein, β growth factor, and shima II, and affected the deposition of hydroxyapatite on the surface of the samples44,45,46.
Figure 9(a) shows the MTT assay of HA/BaTiO3 piezoelectric bioceramics with cycle loading after co-culture with osteoblast cells. At different time points, the number of living cells in each group increased as the culture time increased. At the same time point, the number of active cells that contained BaTiO3 was more than that of 100% HA. Moreover, the number of living cells was highest for the 90% BaTiO3/10% HA piezoelectric bioceramics, and the difference was statistically significant (p < 0.05). This finding showed that the biological compatibility of piezoelectric ceramic that contained BaTiO3 was better than that of HA when cycle loading was applied. The electrical stimulation produced by the electric force transformation improved the biocompatibility of BaTiO3 when cycle loading was applied on the surface. The biocompatibility of the piezoelectric ceramics increased initially then decreased with the decreasing BaTiO3 content. This increase may be attributed to the reduction of piezoelectric properties, which leads to the decrease of biological compatibility caused by electrical stimulation. By contrast, the HA content increased with decreasing BaTiO3 content. HA is a material with good biological activity, which will play a positive role in the biocompatibility of the material47,48. These two trends have different effects on each other, and the 90% BaTiO3/10% HA piezoelectric bioceramics have better biocompatibility than the others.
The ALP activity of HA/BaTiO3 piezoelectric bioceramics with cycle loading after co-culture with osteoblasts is shown in Fig. 9(b). According to the different time points of the ALP activity, the ALP activity of the cells increased with the increasing culture time. The ALP activity of the piezoelectric ceramics that contained BaTiO3 was higher than that of HA. Moreover, the ALP activity of piezoelectric ceramics with 90% content was higher than that of piezoelectric ceramics with 80% and pure BaTiO3, and the difference was statistically significant (p < 0.05). This finding showed that the bone induction activity of the piezoelectric ceramic was better than that of HA when cyclic loading was applied. When cyclic loading was applied on HA/BaTiO3 piezoelectric bioceramics, the electrical stimulation promoted osteoblast proliferation and growth, which was similar to the actions of piezoelectric effects on human bone growth, molding, and reconstruction. Negative-bound charge with dynamic changes existed on the negative surface of HA/BaTiO3 piezoelectric bioceramics, which can absorb positively charged ions in the medium to move toward the negative surface. Positively charged layers were formed gradually, and the protein molecules with negative charges on the surface and cells would be attracted by the positively charged layers. The protein layer can induce the formation of bone-like apatite on the surface of biomaterials, regulate the adsorption of platelets on the material surface, and activate the aggregation function and complement49. Furthermore, it can promote the adhesion, proliferation, and differentiation of osteoblasts.
Conclusions
In summary, BaTiO3 with piezoelectric effect was introduced into HA. HA/BaTiO3 composites with different compositions were prepared by using the injection molding process, and the piezoelectric properties were obtained by polarization. An in vitro biological culture device of piezoelectric material, which can simulate the dynamic environment of the human bone, was designed. The effect of the content of piezoelectric phase on the biological properties was studied by means of apatite deposition and osteoblast culture experiments. Compressive strengths of HA/BaTiO3 composites sintered at 1250 °C for 2 h ranged from 16.2 MPa to 28.4 MPa. The d33 of HA/BaTiO3 piezoelectric ceramics after polarization was 1.3 pC/N to 6.8 pC/N. Under static non-loading condition, the change of BaTiO3 content had little effect on the biocompatibility and bone-inducing activity of HA/BaTiO3 composites, but all composite piezoelectric ceramics were lower than that of pure HA. When cyclic loading was applied on the surface of HA/BaTiO3 piezoelectric ceramics, the biocompatibility and bone-inducing activity of HA/BaTiO3 piezoelectric ceramics were higher than that of pure HA. The best biocompatibility and bone-inducing activity were demonstrated by the 10%HA/90%BaTiO3 piezoelectric ceramics. The deficiency of this experiment is that the results of in vitro experiments did not take into account the effects of strength and surface topography on cell adhesion and proliferation in spite of the piezoelectric effect. Further study needs to simulate other movement frequencies and different stresses of the human to examine the role of the piezoelectric effect fully. In addition, the effect of the composite material with a higher piezoelectric coefficient than human bone on cell adhesion and proliferation requires further research.
Materials and Methods
Materials
HA (Sigma-Aldrich Chemical Co. Inc., USA) with a size of 0.5 μm to 1.0 μm was used as a biological phase, and BaTiO3 powder (<3 μm, Aladdin, Shanghai Aladdin Biochemical Polytron Technologies Inc., China) was used as a piezoelectric phase. Carboxymethyl cellulose (CMC, Tianjin Fuchen Chemicals Co. Ltd., China) was used as a binder. A dispersant (polyacrylate sodium; Sinopharm Chemical Reagent Co., Ltd, China) was used to stabilize the slurry, and deionized water was used as a solvent of slurries.
Fabrication of HA/BaTiO3 composite materials
Composite powders (100 wt.% BaTiO3, 90 wt.% BaTiO3/10 wt.% HA, 80 wt.% BaTiO3/20 wt.% HA, and 100 wt.% HA) were mixed with 1 wt.% of dispersant and 0.5 wt.% binder in deionized water and ground with a ball mill for approximately 48 h. The prepared slurries were poured into plaster cylinders (Φ24 mm × 20 mm). The samples were placed in an unlit place, dried slowly at room temperature, and sintered at 1250 °C in air for 2 h. After cooling, the samples were covered with silver on the upper and lower surfaces, and then the samples were polarized. The polarization field intensity was 0.8 kv/mm to 1.4 kv/mm, the polarization time was 10 min to 50 min, and the polarization temperature was 110 °C to 140 °C. The surface of the sample was polished by using No. 400 sandpaper to remove the silver and to ensure consistent surface roughness of all samples.
Characterization of materials science
Morphologies of the HA/BaTiO3 composite materials were characterized by using a SEM (model JSM-4500, JEOL, Japan). XRD (Model 7000, Shimadzu Limited, Japan) was used to identify the phases in the sintered composite samples. The piezoelectric constant d33 of the sample was tested by quasi-static d33 tester (ZJ-3AN, Institute of Acoustics, Chinese Academy of Sciences). The sample size for d33 testing was Φ10 mm × 2 mm. Samples were measured after polarization and stored at room temperature for 24 h. The positive and negative sides of the samples were indicated. The compressive strength were measured on cylindrical samples of Φ10 mm × 10 mm by using a computer server to control the material testing machine (HT-2402-100KN, Hungta, Taiwan) with a pressure speed of 0.5 mm min−1. Five samples were tested to obtain an average value. All samples for experiments are polished to obtain a similar surface roughness.
Design of in vitro dynamic loading device
In the experiment, an in vitro loading device was designed (Fig. 10). The device consists of a circulating force component, culture dish, and indenter. The working principle of the circulating force component is presented. The outer margin of the rotating cam contacts with the connecting rod, which converts the rotary motion into linear reciprocating motion to form the cyclic displacement. The cyclic displacement was converted into a force with sine distribution by a spring. Force was exerted on the lid of the culture dish, and the inner surface of the culture dish lid was connected with a titanium alloy indenter, which contacts with the composite materials in the culture dish (Fig. 10a). This design has the following advantages: the load cycle of the force can be controlled by the speed of the motor; the value of the force can be adjusted by the elastic coefficient of the spring; the loading curve of the force can be controlled by changing the cam profile; and the indirect transfer of the force ensures that the culture dish will not be contaminated by the loading device. The dynamic loading device was used for in vitro biological experiment in the incubator (Fig. 10b) to simulate the physiological loading of bone under different positions of the human body. Loading parameters of 3 Hz and 60 N are selected to simulate the frequency and pressure of the bearing bone when the people walk fast.
SBF immersion
SBF was prepared according to the ion concentration of Kokubo50. The 100 wt.% BaTiO3, 90 wt.% BaTiO3/10 wt% HA, 80 wt.% BaTiO3/20 wt.% HA, and 100 wt.% HA that were static for 24 h after polarization treatment were ultrasonically cleaned in acetone and deionized water. After drying at 70 °C, the samples that were negatively upward were placed in the culture dish, incubated at 37 °C, and soaked for 7 days. The samples were taken out of the SBF and washed with acetone and distilled water. Samples were dried naturally at room temperature. The deposition of HA on the surface of the samples was observed by a SEM (s-4800, Hitachi, Japan). In addition, the samples were loaded using the dynamic loading device for 3 h a day (loading frequency 3 Hz, maximum load 60 N) when soaking in the SBF, and the steps were repeated.
Cell adhesion
The samples were sterilized with Co-60 then placed in 24-well plates. Osteoblasts were digested into monoplast suspension, and approximately 2 × 104 osteoblasts were seeded on each sample in each well and incubated at 37 °C. The culture medium was changed every 2 days. After culturing for 1, 4, and 7 days, the MTT solution was added to each well and incubated at 37 °C for 4 h. Dimethyl sulfoxide was added to each well, and the solution was transferred to 96-well plates51. The absorbance of solutions at 492 nm was measured with an MK-2 microplate reader after culturing for 1, 4, and 7 days. The morphologies of osteoblasts seeded on the samples were observed by SEM. In addition, samples were loaded using the dynamic loading device for 3 h a day (loading frequency 3 Hz, maximum load 60 N) during culture, and the steps were repeated. Experimental results were analyzed using SPSS19.0 software, and p < 0.05 is considered to indicate statistical difference. Five samples of each type were studied. The assays were performed in triplicate.
Alkaline phosphatase (ALP) activity assay
The 2 × 104 osteoblasts were seeded on each sample in each well and incubated at 37 °C. After culturing for 4 and 7 days, the samples were transferred into new 24-well plates and soaked in 0.3% Triton X-100 to lyse cells after four freezing and thawing cycles. The ALP activity test kit was added to the lysate, and corresponding reagents were added according to the manufacturer’s instructions. The lysate was transferred to 96-well plates, and the absorbance of lysates at 520 nm was measured with the MK-2 microplate reader. In addition, samples were loaded using the dynamic loading device for 3 h a day (The loading frequency is 3 Hz, and the maximum load is 60 N.) during culture, and the steps were repeated. Experimental results were analyzed using SPSS19.0 software, and P < 0.05 is considered to indicate statistical difference. Five samples of each type were studied. The assays were performed in triplicate.
Additional Information
How to cite this article: Tang, Y. et al. Fabrication and in vitro biological properties of piezoelectric bioceramics for bone regeneration. Sci. Rep. 7, 43360; doi: 10.1038/srep43360 (2017).
Publisher's note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Acknowledgments
The authors would like to acknowledge the support from the National Natural Science Foundation of China (Nos 51372199 and 51572217).
Footnotes
The authors declare no competing financial interests.
Author Contributions Y.T. and Z.W. conceived the research, Y.T., C.W., L.H. and W.Z. conducted the experiments, Y.T., Z.W. and K.Z. analyzed the results. Y.T. and C.W. wrote the paper, and Z.W. and K.Z. helped with editing. All authors commented on the manuscript.
References
- Shen X. et al. Sequential and sustained release of SDF-1 and BMP-2 from silk fibroin-nanohydroxyapatite scaffold for the enhancement of bone regeneration. Biomaterials 106, 205–216, doi: 10.1016/j.biomaterials.2016.08.023 (2016). [DOI] [PubMed] [Google Scholar]
- Xiong X. B. et al. A Novel Strategy for Preparation of Si-HA Coatings on C/C Composites by Chemical Liquid Vaporization Deposition/Hydrothermal Treatments. Sci. Rep. 6, 31309, doi: 10.1038/srep31309 (2016). [DOI] [PMC free article] [PubMed] [Google Scholar]
- Sun F., Zhou H. & Lee J. Various preparation methods of highly porous hydroxyapatite/polymer nanoscale biocomposites for bone regeneration. Acta Biomater. 7, 3813–3828, doi: 10.1016/j.actbio.2011.07.002 (2011). [DOI] [PubMed] [Google Scholar]
- Feng P., Niu M., Gao C. D., Peng S. P. & Shuai C. J. A novel two-step sintering for nano-hydroxyapatite scaffolds for bone tissue engineering. Sci. Rep. 4, 5599, doi: 10.1038/srep05599 (2014). [DOI] [PMC free article] [PubMed] [Google Scholar]
- Hamidreza F., Jamshid A. M., Davoud H. F. & Fathollah M. Modification of electrophoretically deposited nano-hydroxyapatite coatings by wire brushing on Ti–6Al–4V substrates. Ceram. Int. 38, 4885–4893, doi: 10.1016/j.ceramint.2012.02.079 (2012). [DOI] [Google Scholar]
- Zhu Y. et al. Micropattern of nano-hydroxyapatite/silk fibroin composite onto Ti alloy surface via template-assisted electrostatic spray deposition. Mater. Sci. Eng. C 32, 390–394, doi: 10.1016/j.msec.2011.11.002 (2012). [DOI] [Google Scholar]
- Jeonghwa K. et al. An epidermal growth factor derivative with binding affinity for hydroxyapatite and titanium surfaces. Biomaterials 34, 9747–9753, doi: 10.1016/j.biomaterials.2013.09.004 (2013). [DOI] [PubMed] [Google Scholar]
- Kazutoshi I. et al. Surface functionalization of tissue culture polystyrene plates with hydroxyapatite under body fluid conditions and its effect on differentiation behaviors of mesenchymal stem cells. Colloid. Surface. B 147, 351–359, doi: 10.1016/j.colsurfb.2016.08.020 (2016). [DOI] [PubMed] [Google Scholar]
- Tang Y., Zhao K., Hu L. & Wu Z. Two-step freeze casting fabrication of hydroxyapatite porous scaffolds with bionic bone graded structure. Ceram. Inter. 39, 9703–9707, doi: 10.1016/j.ceramint.2013.04.038 (2013). [DOI] [Google Scholar]
- Movrin I., Vengust R. & Komadina R. Adjacent vertebral fractures after percutaneous vertebral augmentation of osteoporotic vertebral compression fracture: a comparison of balloon kyphoplasty and vertebroplasty. Arch. Orthop. Trauma. Surg. 130, 1157–1166, doi: 10.1007/s00402-010-1106-3 (2010). [DOI] [PubMed] [Google Scholar]
- Agata P. & Grazyna G. In vitro evaluation of the risk of inflammatory response after chitosan/HA and chitosan/β-1,3-glucan/HA bone scaffold implantation. Mater. Sci. Eng. C 61, 355–361, doi: 10.1016/j.msec.2015.12.066 (2016). [DOI] [PubMed] [Google Scholar]
- Subramaniam S., Fang Y.-H., Sivasubramanian S., Lin F.-H. & Lin C.-P. Hydroxyapatite- calcium sulfate-hyaluronic acid composite encapsulated with collagenase as bone substitute for alveolar bone regeneration. Biomaterials 74, 99–108, doi: 10.1016/j.biomaterials.2015.09.044 (2016). [DOI] [PubMed] [Google Scholar]
- Fukada E. & Yasuda I. Piezoelectric effects in collagen. Jpn. J. Appl. Phys. 3, 502B (1964). [Google Scholar]
- Fukada E. & Yasuda I. On the piezoelectric effect of bone. J. Phys. Soc. Jap. 12, 1158–1162 (1957). [Google Scholar]
- Braden M., Bairstow A. G., Beider I. & Ritter B. G. Electrical and piezo-electrical properties of dental hard tissues. Nature 212, 1565–1566 (1966). [DOI] [PubMed] [Google Scholar]
- Sarah, S., Li C., Choi Y. J., Michael, L.& David, L. K. Bioelectric modulation of wound healing in a 3D in vitro model of tissue-engineered bone. Biomaterials 34, 6695–6705, doi: 10.1038/2121565a0 (2013). [DOI] [PMC free article] [PubMed] [Google Scholar]
- Shin J., Rodriguez B. J., Baddorf A. P. & Thundat T. Simultaneous elastic and electromechanical imaging by scanning probe microscopy: Theory and applications to ferroelectric and biological materials. J. Vac. Scie. Technol. B 23, 2102–2108, doi: 10.1116/1.2052714 (2005). [DOI] [Google Scholar]
- Liu Y., Zhang Y., Chow M. J., Chen Q. N. & Li J. Biological ferroelectricity uncovered in aortic walls by piezoresponse force microscopy. Phys. Rev. Lett. 108, 123–133, 10.1103/PhysRevLett.108.078103 (2011). [DOI] [PMC free article] [PubMed] [Google Scholar]
- Park J. B., Kenner G. H., Brown S. D. & Scott J. K. Mechanical property changes of barium titanate (ceramic) after in vivo and in vitro aging. Biomater. Med. Devices. Artif. Organs. 5, 267–276 (1977). [DOI] [PubMed] [Google Scholar]
- Park Y.-J., Hwang K.-S., Song J.-E., Ong J. L. & Rawls H. R. Growth of calcium phosphate on poling treated ferroelectric BaTiO3 ceramics. Biomaterials 23, 3859–3864, doi: 10.1016/S0142-9612(02)00123-0 (2002). [DOI] [PubMed] [Google Scholar]
- Kumar D. et al. Polarization of hydroxyapatite: Influence on osteoblast cell proliferation. Acta Biomater 6, 1549–1554, doi: 10.1016/j.actbio.2009.11.008 (2010). [DOI] [PubMed] [Google Scholar]
- Bodhak S., Bose S. & Bandyopadhyay, A. Role of surface charge and wettability on early stage mineralization and bone cell–materials interactions of polarized hydroxyapatite. Acta Biomater 5, 2178–2188, doi: 10.1016/j.actbio.2009.02.023 (2009). [DOI] [PubMed] [Google Scholar]
- Dubey A. K., Basu B., Balani K., Guo R. & Bhalla A. S. Multifunctionality of perovskites BaTiO3 and CaTiO3 in a composite with hydroxyapatite as orthopedic implant materials. Integr. Ferroelectr 131, 119–126, doi: 10.1080/10584587.2011.616425 (2011). [DOI] [Google Scholar]
- Zhang Y., Chen L., Zeng J., Zhou K. & Zhang D. Aligned porous barium titanate/hydroxyapatite composites with high piezoelectric coefficients for bone tissue engineering. Mater. Sci. Eng. C 39, 143–149, doi: 10.1016/j.msec.2014.02.022 (2014). [DOI] [PubMed] [Google Scholar]
- Nakamura S., Kobayashi T., Nakamura M. & Yamashita K. Enhanced in vivo responses of osteoblasts in electrostatically activated zones by hydroxyapatite electrets. J. Mater. Sci.-Mater. M. 20, 99–103, doi: 10.1007/s10856-008-3546-7 (2009). [DOI] [PubMed] [Google Scholar]
- Feng J., Yuan H. P. & Zhang X. D. Promotion of osteogenesis by a piezoelectric biological ceramic. Biomaterials 18, 1531–1534, doi: 10.1016/S0142-9612(97)80004-X (1997). [DOI] [PubMed] [Google Scholar]
- Liu B. et al. Improved osteoblasts growth on osteomimetic hydroxyapatite/BaTiO3 composites with aligned lamellar porous structure. Mater. Sci. Eng. C 61, 8–14, doi: 10.1016/j.msec.2015.12.009 (2016). [DOI] [PubMed] [Google Scholar]
- Noris-Suárez K. et al. In Vitro Deposition of Hydroxyapatite on Cortical Bone Collagen Stimulated by Deformation-Induced Piezoelectricity. Biomacromolecules 8, 941–948, doi: 10.1021/bm060828z (2007). [DOI] [PubMed] [Google Scholar]
- Jing D. et al. In situ intracellular calcium oscillations in osteocytes in intact mouse long bones under dynamic mechanical loading. FASEB J 28, 1582–1592, doi: 10.1096/fj.13-237578 (2014). [DOI] [PMC free article] [PubMed] [Google Scholar]
- Zhang S. & Yu F. Piezoelectric materials for high temperature sensors. J. Am. Ceram. Soc. 94, 3153–3170, doi: 10.1111/j.1551-2916.2011.04792.x (2011). [DOI] [Google Scholar]
- Gittings J. P., Bowen C. R., Turner I. G., Baxter F. & Chaudhuri J. Characterisation of ferroelectric-calcium phosphate composites and ceramics. J. Eur. Ceram. Soc. 27, 4187–4190, doi: 10.1016/j.jeurceramsoc.2007.02.120 (2007). [DOI] [Google Scholar]
- Xu T. & Wang C.-A. Effect of two-step sintering on micro-honeycomb BaTiO3 ceramics prepared by freeze-casting process. J. Eur. Ceram. Soc. 36, 2647–2652, 10.1016/j.jeurceramsoc.2016.03.032 (2016). [DOI] [Google Scholar]
- Zhang W., Cheng H., Yang Q., Hu F. & Ouyang J. Crystallographic orientation dependent dielectric properties of epitaxial BaTiO3 thin films. Ceram. Int. 42, 4400–4405, doi: 10.1016/j.ceramint.2015.11.122 (2016). [DOI] [Google Scholar]
- Song H.-J. & Park Y.-J. Fabrication of BaTiO3 films on titanium by microarc oxidation method and improvement of bioactivity by electric poling treatment. Mater. Lett. 61, 3473–3476, doi: 10.1016/j.matlet.2006.11.100 (2007). [DOI] [Google Scholar]
- Park J. B. & Lake R. S. Biomaterials: An Introduction (2nd edition). Plenum Press, New York (1992). [Google Scholar]
- McNamara I. et al. Mechanical properties of morcellised bone graft with the addition of hydroxyapatite. J. Mater. Sci.-Mater. M. 25, 321–327, doi: 10.1007/s10856-013-5085-0 (2014). [DOI] [PubMed] [Google Scholar]
- Subhadip B., Susmita B. & Amit B. Role of surface charge and wettability on early stage mineralization and bone cell–materials interactions of polarized hydroxyapatite. Acta Biomater. 5, 2178–2188, doi: 10.1016/j.actbio.2009.02.023 (2009). [DOI] [PubMed] [Google Scholar]
- Giovanni B. et al. Suspension thermal spraying of hydroxyapatite: Microstructure and in vitro behaviour. Mater. Sci. Eng. C 34, 287–230, doi: 10.1016/j.msec.2013.09.017 (2014). [DOI] [PubMed] [Google Scholar]
- Kim H.-M., Himeno T., Kokubo T. & Nakamura T. Process and kinetics of bonelike apatite formation on sintered hydroxyapatite in a simulated body fluid. Biomaterials 26, 4366–4373, doi: 10.1016/j.biomaterials.2004.11.022 (2005). [DOI] [PubMed] [Google Scholar]
- Kokubo T., Kushitani H., Ohtsuki C., Sakka S. & Yamamuro T. Chemical reaction of bioactive glass and glass-ceramics with a simulated body fluid. J. Mater. Sci.-Mater. M. 3, 79–83, doi: 10.1007/BF00705272 (1992). [DOI] [Google Scholar]
- Zhao M. Z. et al. Response of Human Osteoblast to n-HA/PEEK-Quantitative Proteomic Study of Bio-effects of Nano-Hydroxyapatite Composite. Sci. Rep. 6, 22832, doi: 10.1038/srep22832 (2016). [DOI] [PMC free article] [PubMed] [Google Scholar]
- Itoha S., Nakamurab S. & Nakamurab M. Enhanced bone ingrowth into hydroxyapatite with interconnected pores by Electrical Polarization. Biomaterials 27, 5572- 5579, doi: 10.1016/j.biomaterials.2006.07.007 (2006). [DOI] [PubMed] [Google Scholar]
- Ohgaki M., Kizuki T., Katsura M. & Yamashita K. Manipulation of selective cell adhesion and growth by surface charges of electrically polarized hydroxyapatite. J. Biomed. Mater. Res. A 57, 366–373, doi: (2001). [DOI] [PubMed] [Google Scholar]
- Clark J. et al. Physiological effects of lower extremity functional electrical stimulation in early spinal cord injury: lack of efficacy to prevent bone loss. Spinal Cord 45, 78–85, doi: 10.1038/sj.sc.3101929 (2007). [DOI] [PubMed] [Google Scholar]
- Cornaglia A. I. et al. Stimulation of osteoblast growth by an electromagnetic field in a model of bone-like construct. Eur. J. Histochem 50, 199–204, doi: 10.4081/993 (2006). [DOI] [PubMed] [Google Scholar]
- Chen S.-C. et al. Increases in bone mineral density after functional electrical stimulation cycling exercises in spinal cord injured patients. Disabil. Rehabil. 27, 1337–1341, doi: 10.1080/09638280500164032 (2005). [DOI] [PubMed] [Google Scholar]
- Gittings J., Bowen C., Turner I., Baxter F. & Chaudhuri J. Characterisation of ferroelectric-calcium phosphate composites and ceramics. J. Eur. Ceram. Soc. 27, 4187–4190, doi: 10.1016/j.jeurceramsoc.2007.02.120 (2007). [DOI] [Google Scholar]
- Wang H. et al. Biocompatibility and osteogenesis of biomimetic nano-hydroxyapatite/polyamide composite scaffolds for bone tissue engineering. Biomaterials 28, 3338–3348, 10.1016/j.biomaterials.2007.04.014 (2007). [DOI] [PubMed] [Google Scholar]
- Zanello L. P. & Norman A. W. Electrical responses to 1α, 25 (OH)2-Vitamin D3 and their physiological significance in osteoblasts. Steroids 69, 561–565, doi: 10.1016/j.steroids.2004. 05.003 (2004). [DOI] [PubMed] [Google Scholar]
- Kokubo T. & Takadama H. How useful is SBF in predicting in vivo bone bioactivity? Biomaterials 27, 2907–2915, doi: 10.1016/j.biomaterials.2006.01.017 (2006). [DOI] [PubMed] [Google Scholar]
- Guo Q. et al. Preparation and characterization of poly(pluronic-co-l-lactide) nanofibers for tissue engineering. Int. J. Biol. Macromol. 58, 79–86, doi: 10.1016/j.ijbiomac.2013.03.061 (2013). [DOI] [PubMed] [Google Scholar]