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Elsevier Editorial System(tm) for Surface and Coatings Technology Manuscript Draft Manuscript Number: SURFCOAT-D-20-02420R2 Title: Graphene-coated Ti-Nb-Ta-Mn foams: A promising approach towards a suitable biomaterial for bone replacement Article Type: Full Length Article Keywords: Biomaterials; Titanium alloys; Powder Metallurgy; - Nanocoatings; Graphene; Cytotoxicity Corresponding Author: Dr. sheila Katherine Lascano, Dr. Eng. Corresponding Author's Institution: Universidad Técnica Federico Santa María First Author: sheila Katherine Lascano, Dr. Eng. Order of Authors: sheila Katherine Lascano, Dr. Eng.; Ricardo Chávez Vásconez, Eng.; Daniela Muñoz Rojas, Eng.; Juliet Aristizabal, PhD.; Barbara Arce, BS. Phys.; Carolina Parra, PhD.; Cristian Acevedo, Dr.; Nicole Orellana, BS.Biochem; Mauricio Reyes Valenzuela, Eng.; Francisco Gotor, Dr.; Cristina Arévalo, Dr. Eng.; Yadir Torres Hernández, PhD. Abstract: The design of bone implants with proper biological and mechanical properties remains a challenge in medical implantology. The use of bioactive coatings has been shown to improve the biocompatibility of the implant surface. In this study, a new approach including porous scaffolds, β-Ti alloys and nanocoatings to design new bone implants is presented. Porous Ti-Nb-Ta-xMn alloys (x: 2, 4, and 6 wt.%) substrates were obtained by powder metallurgy and the effect of the porosity and Mn content on mechanical properties was studied. CVD single-layer graphene was transferred onto the porous substrates that presented the best mechanical response (x: 4 wt.%) for further evaluation of in vitro cell behavior (biocompatibility and cell adhesion). Cytotoxicity and biocompatibility tests confirmed that cell adhesion and proliferation were successfully achieved on graphene-coated porous substrates, confirming these systems are potential candidates for using in partial bone tissue replacement. This is an Accepted Manuscript of an article published by Elsevier in Surface and Coatings Technology, Vol. 401, on November 2020, available at: https://doi.org/10.1016/j.surfcoat.2020.126250 // Copyright 2020. Elsevier. En idUS Licencia Creative Commons CC BY-NC-ND
1 Graphene-coated Ti-Nb-Ta-Mn foams: A promising approach towards a suitable biomaterial for bone replacement Sheila Lascano1, *, Ricardo Chávez-Vásconez1, Daniela Muñoz-Rojas1, Juliet Aristizabal2, Bárbara Arce2, Carolina Parra2, Cristian Acevedo2, Nicole Orellana3, Mauricio Reyes- Valenzuela1, Francisco José Gotor4, Cristina Arévalo5, Yadir Torres5 1 Departamento de Ingeniería Mecánica, Universidad Técnica Federico Santa María, Avda. Vicuña Mackenna N° 3939- San Joaquín, Santiago, Chile. 2 Departamento de Física, Universidad Técnica Federico Santa María, Av. España 1680, Valparaíso, Chile 3 Centro de Biotecnología “Dr. Daniel Alkalay Lowitt”. CB-DAL, Universidad Técnica Federico Santa María, Av. España 1680, Valparaíso, Chile. 4 Instituto de Ciencia de Materiales de Sevilla (CSIC-US), Américo Vespucio 49. 41092 Sevilla, Spain. 5 Departamento de Ingeniería y Ciencia de los Materiales y del Transporte, Escuela Politécnica Superior, Calle Virgen de África 7, 41011 Seville, Spain. Keywords: biomaterials; titanium alloys; powder metallurgy; nanocoatings; graphene; cell adhesion, cytotoxicity. *Manuscript Click here to view linked References
2 Abstract The design of bone implants with proper biological and mechanical properties remains a challenge in medical implantology. The use of bioactive coatings has been shown to improve the biocompatibility of the implant surface. In this study, a new approach including porous scaffolds, β-Ti alloys and nanocoatings to design new bone implants is presented. Porous Ti-Nb-Ta-xMn alloys (x: 2, 4, and 6 wt.%) substrates were obtained by powder metallurgy and the effect of the porosity and Mn content on mechanical properties was studied. CVD single-layer graphene was transferred onto the porous substrates that presented the best mechanical response (x: 4 wt.%) for further evaluation of in vitro cell behavior (biocompatibility and cell adhesion). Cytotoxicity and biocompatibility tests confirmed that cell adhesion and proliferation were successfully achieved on graphene-coated porous substrates, confirming these systems are potential candidates for using in partial bone tissue replacement.
3 1. Introduction Metallic biomaterials are extensively used for replacing hard tissue and for load-bearing applications. Specifically, titanium and its alloys exhibit the most suitable characteristics for biomedical applications, promoting in vitro and in vivo behavior [1]. However, these materials have shown important drawbacks that compromise the reliability of implants: stress-shielding phenomenon, poor or low osseointegration, and fracture of implants due to overload or accumulated damage produced by fatigue. The first drawback, the stress-shielding phenomenon [2], is caused by the mismatch between Young’s modulus of bone tissue and titanium implant (20-25 GPa for cortical bone and 110 GPa for cp- Ti and α+β type Ti) [3], and promotes bone resorption and eventual fracture of the host tissue [4], compromising the clinical success of implants [5]. An approach to solve this issue is the design and manufacture of porous metallic biomaterials that combine the low stiffness of porous structures [6-8] and the high strength of metallic alloys [9]. The control of microstructural parameters of porous materials such as porosity content, pore size distribution, pore morphology, and interconnectivity has become an attractive strategy to reduce stress shielding as well as to promote bone in-growth [10]. Different fabrication methods are currently employed for the manufacture of metallic foams [9, 11-16]. Among these methods, powder metallurgy (PM) is a promising route since offers cost-effective and flexible fabrication of tailored titanium foams for biomedical applications[17] and allows the design and manufacture of new alloys that cannot be produced by casting approaches. The use of the space-holder technique arises as a suitable and economic route for introducing high levels of porosity (35- 80%) and a homogeneous pore distribution throughout the Ti volume [8, 18, 19]. Different materials can be employed as temporary space-holder particles which are later eliminated by two alternative methods: evaporation at low temperatures, in the case of ammonium bicarbonate [20-
4 22], carbamide [15, 17, 23], K2CO3 [24], polymethyl methacrylate (PMMA) [25, 26] and polyvinyl alcohol (PVA) [27], or dissolution in water, in the case of sodium chloride [6, 21, 28, 29]. It is also important to highlight that, the higher the porosity, the lower the mechanical strength and wear resistance of the porous structure. One approach to address this specific issue in titanium alloys is to reduce the stiffness by designing alloys with low Young’s modulus. Two generations of Ti alloys have been developed for biomedical applications [30, 31]. The first generation of titanium alloys, which exhibit both α and (α+β) phases, was developed between 1950 and 1990 and extensively used for implants. However, these alloys showed some drawbacks, specifically poor wear resistance, low hardness, and high Young’s modulus (~110 GPa) [32, 33]. In addition, depending on the elements present in these alloys, a cytotoxic effect has to be taken into account [34-36]. Ti, Zr, Ta and Pd are low cytotoxicity elements [32], whereas other elements such as Al, V, Ni, and Co have been reported as cytotoxic [34, 37, 38]. Aluminum, for instance, has been found to increase scar tissue and is involved in severe neurological and metabolic-bone diseases, such as Alzheimer's and osteomalacia [39]. Vanadium produces a severe tissue reaction that is characterized by a sterile abscess [32] whereas nickel exhibits one of the highest sensitivities in metallic allergen tests [40], producing contact allergenic reactions and carcinogen effects [41]. In response to these drawbacks, a second generation of Ti alloys, the β-phase Ti-based alloys, have been developed and used since the 1990s. These alloys have been preferred for bio-implant applications rather than α or (α+β) Ti alloys, mainly due to their lower elastic modulus [42]. In these β-type Ti alloys, the presence of β-phase is promoted by incorporating β-stabilizing elements, such as Pd, Ni, Mo, Ta, V, Mn, and Nb [43]. Biesiekierski, et al. [34] have identified the biological impact of some of those elements on human health, assessing their biocompatibility and other potential risks such as corrosion, degradation, and their carcinogenic,
5 genotoxic, mutagenic, cytotoxic and allergenic properties. According to literature, Ti, Nb, Ta, Mn, Zr, and Ru, have been found to exhibit the best biofunctional behavior [42]. Among those elements, Ta, Nb, and Zr have been reported to impact the mechanical properties of β titanium alloys, by decreasing their elastic modulus while increasing their strength [44, 45]. Some reports illustrating this behavior of Ti-30Nb-13Ta, Ti-13Nb-13Zr, and Ti-35Nb-7Zr-5Ta can be found in Ref [46-49]. These alloys have been developed with the aim to match Young’s moduli of different types of human bone (cortical: 3–30 GPa; cancellous: 0.02–0.5 GPa). One route to decrease Young’s modulus of a Ti-based alloy is by increasing its bond order (Bo) and energy level (Md) [34,50]. For bone replacement applications, the target bond order value is 2.92 eV, and whereas the target energy level is 2.38 eV. The Bo and Md values can be obtained using the equations (1) and (2) [50], where Xi is the atomic fraction of each alloying element: () o i o i i B X B (1) () d i d i i M X M (2) Efforts are now focused on finding new alloying elements to improve the mechanical and corrosion properties of metallic biomaterials. In particular, Mn is an interesting alternative due to its role in cartilage and collagen formation, bone mineralization [51], and cell adhesion [52]. However, only a few studies have reported the effect of Mn on Ti alloys properties, especially in the second-generation alloys [53]. Good corrosion behavior of Mn-containing alloys in simulated body fluid has been recently reported [54]. In author’s previous work, Ti-34Nb-29Ta-xMn (x: 2, 4, and 6 wt.%) alloy foams fabricated by mechanical alloying were studied, showing elastic moduli ranging between 27 and 30 GPa [55]. These results, in the range of cortical bone, suggested that this specific Ti alloy is not expected to exhibit a strong stress-shielding effect. Although these results are promising, the overall cost of material fabrication, related to long processing time (~60 hours), is a relevant aspect that still needs to be addressed.
6 Another important disadvantage of Ti-based materials is their poor or low rate of osseointegration caused by the formation of fibrous tissue at the bone-implant interface, which promotes micro-movements of the implant and eventual loosening, whether this is of aseptic nature or caused by the presence of bacterial biofilms. The use of thermochemical treatments and/or bioactive coatings has been proposed to modify the surface texture to improve the bioactivity of Ti implants. Some techniques to enhance the cell adhesion to implant surface include anodic reaction, hydrogen peroxide, sol-gel, thermochemical surface modification, and chemical vapor deposition. [56]. Although rough and porous surfaces have proven to increase fixation of Ti implants [57, 58], to obtain reliable implants it is essential to generate bioactive surfaces that promote cell adhesion and ingrowth, preventing bacteria proliferation. In this sense, bioactive coatings, such as hydroxyapatite and bioactive glass, have shown positive results in terms of osseointegration. In this context, surface modification at the nanometric scale represents a unique framework to improve the biofunctionality of porous materials [59]. Nanostructured coatings have been designed and applied to non-porous titanium surfaces to control cell behavior and to obtain bioactive surfaces, promoting cell adhesion and proliferation [60, 61]. Graphene-family nanomaterials have been widely used in the biomedical field because of their various unique properties. Graphene supports the absorption and binding of antibodies, adapters, drugs, genes, enzymes, and other molecules [62], has been explored for cancer treatments [63], has been used for biological imaging [64], as drug carrier [65], biosensor [66], and biological scaffold in tissue engineering [67]. Previous studies have revealed that scaffolds based on graphene and its derivatives, such as graphene oxide, can enhance cell differentiation [68-70]. It has been also proven that single-layer graphene (SLG) promotes the osteogenic differentiation into osteogenic lineages when used as a coating onto titanium samples. This nanomaterial, that can be grown as large as 50cm x 5cm [71], improves the initial fixation strength and long-term osseointegration of
7 the implant/bone interface required for further promotion of bone defect healing in Ti6Al4V [72]. However, Al and V are considered as hazardous elements that could compromise long term implantation in the human body [32, 73], as was mentioned before. The aim of this work is to propose a novel approach based on the use of graphene-coated porous Ti-Nb-Ta-Mn alloys produced by space-holder technique, aim to present low Young’s modulus for stress-shielding reduction and to increase osseointegration and cell viability and proliferation. For the selection of the optimal chemical composition of Ti alloys, theoretical calculus was used to estimate the atomic fraction of each element as well as the data obtained in previous works, where an α + β Ti phase was processed via mechanical alloying and conventional sintering [54, 55]. Using this background, which will be discussed in detail in the following sections, a specific Ti alloy foams composition was selected, Ti-35Nb-29Ta-xMn (x: 2, 4, 6 wt.%), for implant applications. In this work the effect of physical and processing parameters of Ti alloys, such as Mn content, sintering temperature, and porosity, on its microstructural characteristics and mechanical properties, was investigated and compared with the reported values for porous commercially pure titanium (c.p. Ti) grade 4 samples [21]. This porous material, fabricated by space-holder technique, was coated with high-quality single-layer graphene to promote a bioactive surface and increase the material’s biofunctionality and further osseointegration. Biocompatibility and biological behavior of coated and uncoated substrates were evaluated by in vitro cytotoxicity tests using Mouse Embryonic Fibroblasts (MEF). 2. Materials and methods The percentage of each alloying element in Ti-35Nb-29Ta-xMn (x: 2, 4, 6 wt.%) alloys was selected following two main criteria: (i) to look for an adequate concentration of β stabilizing elements required to retain the β phase at room temperature, and (ii) to tune the bond order and
8 energy level needed to achieve a Young’s modulus close to the modulus of the bone (~ 30 GPa) to minimize the stress shielding. Regarding the first criterium, the equation (3), (based on Ref [74]) allows obtaining the equivalent Nb fraction (Nbeq), as a function of Mn and Ta content, to achieve the stabilized β phase in the alloy. (3) Using the reported atomic percent (at. %) values to obtain a stable β phase (21 at. % for Ta, 5.3 at. % for Mn and 23 at. % for Nb) [74], the calculated Nbeq for the Ti-35Nb-29Ta-xMn alloy was 54.5 at. % (for 2 wt.% Mn), 67.7 at. % (for 4 wt.% Mn) and 80.4 at. % (for 6 wt.% Mn). Concerning the second criterium, the Bo and Md values for the Ti-35Nb-29Ta-xMn alloy can be obtained using the equations (1) and (2) [50]. The optimum Bo and Md calculated values are 2.925 eV and 2.376 eV, respectively. These values place the selected alloy in the region where Young’s modulus will be theoretically between 50-60 GPa. 2.1. Fabrication and characterization of the porous substrates Ti-35Nb-29Ta-xMn (x: 2, 4 and 6 wt.%) and c.p. Ti grade 4 (reference material) porous samples were fabricated using space-holder technique. For sample processing, metallic powders and NH4HCO3 (50 vol.%) particles were blended for 40 min in a vacuum chamber (Plas-Lab) to reach good homogenization. Morphological characterization and information of commercial powders prior to this blending procedure are shown in Figure S1 and Table S1. The particle size distribution for spacer material was determined by sieve analysis. Then, uniaxial cold compaction of powders was performed using a universal testing machine Zwick Roell at 400 MPa (according to compressibility curves of mixed powders). A preload of 20 MPa was applied at a rate of 8
15 interconnected porosity of samples obtained by the Archimedes’ method are, on average, 70% and 57%, respectively. The porosity measured by image analysis (P(IA)) is slightly lower than P(Arch) since only the results of surface porosity are considered. It is also observed that the porosity is greater than the space holder percentage. In the case of samples with 4 wt.% Mn, the porosity estimated by image analysis is about 50%. This aspect is important since the elements of the alloy are influencing the porosity in a significant way. Previous author´s work showed that, when using the space holder technique, porosities close to wt.% of the added spacer can be achieved [16, 22, 95]. Table I. Morphological parameters of pores. Mn [wt.%] Sintering Temperature [°C] Total Porosity P(Arch) [%] Interconnected Porosity Pint [%] Porosity by Image Analysis (IA) [%] Equivalent Diameter Deq (*) [µm] Shape factor Ff Pore distance λ [µm] 2 1200 70.2±0.0 54.2±0.2 63.0±4.9 181.3±13.7 0.68±0.29 7.3 1300 69.2±0.1 50.8±0.4 62.4±5.6 201.7±15.7 0.80±0.24 9.6 4 1200 68.5±0.2 59.5±0.2 52.1±5.1 161.5±7.4 0.76±0.27 12.3 1300 68.7±0.0 59.4±0.1 57.6±5.5 194.9±13.1 0.77±0.25 10.9 6 1200 71.2±0.2 57.3±0.0 66.2±3.4 183.3±11.4 0.81±0.24 6.4 1300 70.8±0.3 62.0±0.4 67.2±3.9 192.3±20.2 0.76±0.26 7.3 The equivalent pore diameter (Deq) obtained by image analysis was between 162 and 202 µm, approximately. No significant effects of Mn content or sintering temperature on the pore diameter were found. Pore diameters obtained by different sintering temperatures and Mn contents are not statistically different (p >0.05). The observed pore size distribution shows that 50-80% of the pores are between 100 and 200 µm size, 10-15% are around 400 µm size, whereas only 5% of the
16 pores are around 800 µm size. Interestingly, the formation of pores larger than 1200 µm for the 2 wt.% Mn and 6 wt.% Mn samples was observed. These larger isolated pores could be attributed to the initial size and possible interconnectivity between the particles. However, in specimens with 4 wt.% Mn, a maximum value of 800 µm pore size was obtained. This size is similar to the values obtained in commercial foams and trabecular bones [96]. The calculated pore shape factor (Ff) was 0.76 (Ff equal to 1 suggests a rounded pore). The statistical analysis (Tukey test) indicates that the influence of sintering temperature on Ff is statistically significant for samples with 2 wt.% Mn, with p-value < 0.05, whereas for 4 wt.% Mn and 6 wt.% Mn, the sintering temperature has little or no effect. Besides, there is a substantial difference between the shape factor values for the 2 wt.% Mn and 6 wt.% Mn samples sintered both at 1200°C and at 1300°C. However, when samples of 2 wt.% Mn and 4 wt.% are compared, this large difference can be only found in samples sintered at 1300°C. The pore distance, λ, is used to determine the mean distance between pores. In this case, the calculated λ is between 7.3 and 12 µm, with values slightly higher for the 4 wt.% Mn sample. These λ values indicate that the pores are separated by distances that are on average less than their pore size (Figure 2 (d) and (e)). In this sense, the best result is the one obtained for 4 wt.% Mn specimens, while c.p. Ti sample showed an average value of 85 µm. This confirms what was observed in optical microscopy (Figure 2), where a difference in the porosity distribution and the mean free path between the pores was noticed. From this image analysis it can be inferred that 4 wt.% Mn samples present better results in terms of porosity control, pore morphology, and pore interconnectivity. Ti alloy samples sintered at 1200 and 1300 °C were analyzed by X-ray diffraction (Figure 4) to identify Ti phases. Biesiekierski, et al. [34] have shown that Nb and Ta, which possess the same crystalline structure than Ti and show complete miscibility, are β-isomorphous elements. Although, Mn is a β-eutectoid element, i.e. it is not perfectly soluble in the Ti bulk, its eutectoid
17 effect could be reduced using a low percentage of Mn and the addition of isomorphous stabilizers [97]. XRD pattern analysis confirmed the presence of β-Ti phase (cubic structure) at room temperature, together with a small amount of α phase (hexagonal structure) for all Mn content and both sintering temperatures. Peaks corresponding to the β phase are large for samples sintered at 1200 ºC and, in some cases, they split as a consequence of an incomplete alloying process; thus, the more Mn content, the more evident this effect is. According to these results, the presence of β-isomorphous Nb and Ta promotes the stabilization of β-phase of Ti alloys samples at room temperature, despite the β-eutectoid nature of Mn. These results are confirmed by TEM measurements (Figure 5). A TEM image of 4 wt.% Mn porous sample sintered at 1200 °C and the corresponding polycrystalline electron diffraction pattern are presented in Figure 5 (a). The multiple rings, most of which can be attributed to the β phase of titanium, revealed the polycrystalline nature of the sample. In Figure 5 (b), a high-resolution TEM (HR-TEM) micrograph of the same sample is shown. In the inset, the Fast Fourier Transform corresponding to the two different grains marked with a dashed square is displayed. Both can be unambiguously assigned to the BCC phase of titanium along the [001] and [011] zone axis. XRD patterns and transmission electron microscopy confirm the presence of a β-phase matrix in Ti-35Nb-29Ta-xMn (x: 2, 4, and 6 wt.%) alloys. Despite the complexity of obtaining β-phase, it is possible to stabilize this phase at room temperature. In a similar way, the β phase of the Ti-based alloy appears to be well formed at 1300 °C. According to the results obtained for both sintering temperatures, a solid solution is formed between Ti, Nb, Ta and Mn, during the sintering process. A brief inspection of phase diagrams shows that the binaries systems Ti-Nb [98] and Ti-Ta [98] present complete mutual solubility in the temperature range mentioned. Furthermore, for the Ti-Mn system [98], it is feasible to form a Ti-β solid solution with an amount of Mn between 18 to 30 wt.%. There are not reports in the
18 literature about the phase diagram of Ti-Nb-Ta-Mn and few reports regarding the phase diagram of Ti-Nb-Ta [99, 100]. The mechanical response of porous samples was analyzed by uniaxial compression tests, performed on Ti-35Nb-29Ta-xMn (2, 4, and 6 wt.% Mn) specimens sintered at 1200 °C and 1300 °C, and the results were compared with previous author’s works [21, 55, 95]. The results of the compression tests and stress–strain curves, are presented in Figure 6. In general, the curves indicate an elastic linear behavior followed by a flatter plateau-like region starting around 50 MPa. The Ti-35Nb-29Ta-4Mn samples sintered at 1200 °C exhibited the best mechanical performance under compression stress. This aspect could be related to the results observed in microstructural characterization and image analysis, where the porosity distribution and morphology present the best results. The observed mechanical properties of Ti-based β alloys for all Mn contents are summarized in Table II. The compression test results of the foams showed Young´s modulus (Ec) in the range of 9-12 GPa. Also, Young’s moduli estimated by the Nielsen equation (ENielsen) [80] showed values very similar to those achieved by the compression test. The values are in the admissible range for bone tissue replacement (3-30 GPa). There are no significant differences between the Ec or ENielsen for c.p Ti and Ti-Nb-Ta-Mn samples. Furthermore, yield strength (σy) was calculated according to the criterion proposed by R. M. Christensen [79], obtaining values between 30 MPa and 67 MPa. According to the results, the sample with 4 wt.% Mn sintered at 1200 °C exhibits the highest σy value and compression stress (69 MPa and 98 MPa, respectively). This sample showed a superior capacity of energy absorption in the compression test (area under the curve), which provides a better toughness (Figure 6). In the 4 wt.% Mn samples, pores are smaller than 800µm (Figure 3), the lowest value for the studied samples. Besides, λ is higher than those achieved for samples with other wt% Mn contents. These aspects are particularly relevant in mechanical performance, because of the effect of the pore-size distribution on sample strength.
19 An increase of λ enhances the fraction of the effective strength area and, consequently, the mechanical strength is improved. The plastic behavior of these materials was controlled by the collapse of pores walls and not by the strain hardening. In any case, obtained specimens showed better mechanical strength and ductility than c.p. Ti grade 4 foams with similar porosity, as observed in Table II [95]. Therefore, even if both materials (Ti and Ti alloy) were completely dense, Ti-35Nb-29Ta-xMn samples should have better mechanical response than c.p Ti samples in terms of mechanical strength and ductility, and less stress shielding because of the lower discrepancy with the cortical or cancellous bone tissue (3-30 GPa). Table II. Mechanical properties for porous Ti c.p. and Ti-Nb-Ta-Mn alloys. Note: *Ref [88] and ** Christensen’s [72]. Sintering Temperature [°C] Total Porosity [%] Young’s Modulus [GPa] σy estimated** [MPa] Maximum Compression Strain [mm/mm] Ec ENielsen c.p.Ti* 1250 66 2.6 10.9 29.0 0.04 Mn [wt.%] 2 1200 70.2 9.8 10.5 41.6 16.9 1300 69.2 10.1 12.6 52.7 24.9 4 1200 68.5 9.2 12.9 67.5 21.3 1300 68.7 9.3 12.7 42.3 12.4 6 1200 71.2 11.8 11.1 30.4 14.6 1300 70.8 9.8 11.0 43.3 16.2 Regardless of the type of titanium alloy used, the space holder technique is effective to reach porous structures with pore size and interconnectivity degree needed to benefit the physiological fluid entrance and the subsequent growth of bone tissue inside the implant. Porosity reduces
20 Young's modulus, but also, high porosity levels compromise the tribomechanical and corrosion behavior of the materials. In the case of β alloys, the values required for cortical bone tissue could be achieved by lowering the porosity that translates into less mechanical performance loss. For the obtained β Ti alloys, Young’s modulus was reduced, the ductility was improved, and the yield strength was found close to trabecular bones [96], as shown in Figure 5. Hence, the synthesized Ti alloy foams present a promising mechanical behavior for bone replacement applications, in contrast to the results obtained in previous studies [55]. The observed Young’s modulus value of porous Ti-35Nb-29Ta-4Mn samples, with values ranging between 8.0 and 9.3 GPa, and pore size values between 100 and 800 µm, are closer to those of the trabecular bone [23, 30] and similar to the ones found in previous studies on other Ti alloys (Table III). Table III summarizes the physical and mechanical properties of porous metals, some commercially available alloys [101-103], and trabecular bone [104]. Besides the abovementioned potential of Ti-35Nb-29Ta-4Mn alloy for bone replacement, it is expected that the reduction in processing time achieved in this work will impact on the overall costs of the manufacturing route, making more likely the adoption, commercialization and wide-scale application of this technology. Table III. Physical and mechanical properties comparison of commercial porous metals and trabecular bone with porous Ti alloys obtained in this work and other authors´ studies [8, 55, 96, 101-103, 105-107]. *Measured by Ultrasound technique, **processed by mechanical alloying and sintering. Composition Total Porosity [%] Pore Size [µm] Yield Strength [MPa] Young’s Modulus [GPa] BiofoamTM 50% Polysaccharides and 50% high 60-70 478- 55-70 2.5-3.0
21 molecular weight proteins 578 RegenerexT M Matrix enhanced with thymosin β4 (Tβ4) 67 100- 600 - 1.6 Trabecular MetalTM Carbon foam infiltrated with tantalum 75-85 550 35-51 2.5-3.9 Cachinho et al c.p Ti 75 100- 600 - 0.3 Jia et al c.p Ti 79 370- 600 21 0.9 Torres et al + c.p Ti 65-68 50-300 2-31 9.2-11.2* Aguilar et al** Ti–34Nb–29Ta–xMn 50 100- 600 22-55 27.0-33.0 This study 4 wt.% Mn 69-72 100- 800* 25-68 8.0-9.3 Trabecular bone Matrix 30% (ossein (collagen fibers)) Bound minerals 70% (Calcium hydroxyapatite) 70-80 400- 700 2-12 0.1-0.5 Although from the mechanical and structural point of view the Ti-35Nb-29Ta-4Mn alloy confirmed to be suitable for bone-replacement applications when it comes to corrosion resistance, potential for osseointegration and protection against biofilm formation, additional strategies need to be explored. In this context, nanoscale surface modification has emerged as a powerful tool to control cellular behavior and to develop biomimetic surfaces, since it has been confirmed that materialhost tissue interactions are principally governed by nanometric phenomena [108, 109]. To improve the biological response of obtained surfaces, the use of single-layer graphene has been explored, a nanostructured coating that has been reported to be cytocompatible [81, 110], to suppress biofilm formation [82] and to protect metals from electrochemical corrosion [111] and
22 microbial-induced corrosion [83, 84]. Besides, this one-atom-thick material presents a good adhesion to metallic surfaces [112], which can be relevant, considering several reports on the detachment of hydroxyapatite from the Ti surface [113]. 3.2. Characterization of graphene coatings Before transfer SLG onto the Ti substrate, the graphitic quality and atomic resolved imaging of CVD graphene grown on Cu was characterized by Raman spectroscopy and STM (Figure 7). Large-scale STM tomography (Figure 7 (a)) and characteristic fingerprint of single-layer graphene (honeycomb pattern) were observed through atomic-resolved topographies. A hexagonal structure with around 2.4 Å lattice distance was found (Figure 7 (b)), in agreement with expected values for this graphitic material [84, 114]. CVD graphene transferred onto SiO2 displays sharp G (1584 cm-1) and 2D (2680–2693 cm-1) bands. The G band indicates the order and purity structure of graphite sheets. The 2D band is the characteristic peak of the graphene structure. It is known that the ratio I2D/IG of the intensities of the bands 2D and G are dependent on the number of graphene layers [83, 105, 115]. The ratio I2D/IG~ 2-3 is for single-layer graphene, I2D/IG > 1 for bilayer graphene, and I2D/IG < 1 for multilayer one (graphite). The graphene sample transferred on SiO2 exhibits a ratio I2D/IG > 2, Figure 7 (c), which is consistent with single-layer graphene [84, 114]. Raman spectroscopy was performed to confirm the presence of the SLG coating onto the Ti-Nb-Ta-Mn porous substrate and to evaluate the quality of the transfer process. Figure 7 (d) shows Raman spectra of the CVD single-layer graphene supported on the substrates, suspended over a pore, and on a flat area between pores. The micrographs of the analyzed zones are shown in Figure 7 (e) and (f). The intensity ratio I2D/IG associated with suspended graphene is ~2.5, significantly higher than that for the graphene on the solid surface of the porous substrate, I2D/IG ≈ 1.5. This change of the intensity ratio I2D/IG is due to the Etalon effect [116] of the pore surface under graphene: both surfaces are reflective and the
23 signal obtained for the Raman analysis from the graphene interferes with the one reached from the pore surface. In addition, this constructive interference between the suspended graphene and the inner surface of the pore also produces a strong background signal (See Figure 7d and Figure S3) which has been reported for suspended graphene on TEM grids [116]. The phenomenon is not observed for the smooth surface due to the proximity between layers. The observed shifting in the position of 2D and G bands is probably related to the strain induced on the graphene [117] due to the roughness of the surface and the porosity. Also, a defect band is observed on the spectra obtained on the coating supported on the foam, caused by the wrinkles on the coating, which can be seen in Figure 7 (e) and Figure 8 (c). The morphology of graphene coating transferred onto Ti alloy substrates was studied through OM and SEM (Figure 8). It has been reported that bioactive coatings such as graphene, enhance the formation of calcium phosphates (bone) [62, 72] and improve the cellular adhesion due to the biofunctionalization of the surface. According to these images, coating presents a good graphene coverage of the porous Ti substrate, both flat areas and pores (Figure 8 (a) and (c)). Graphene coating is entirely suspended over the pores (areas marked with the arrows) when pores are smaller than ~400 µm (Figure 8 (d)). However, for larger pores the coating integrity is affected, leading to the presence of holes that leave these large pores exposed (Figure 8 (b) and (d)). This damage is presumably connected with some intrinsic aspects of the transfer process such as (a) the pressure resulting from the vaporization inside the pore of the remnant fluid used during transfer procedure or (b) the stress introduced in the coating when the coated sample is baked to improve coating adhesion. The presence of PMMA residues from other transference process is observed as stains using bright field in Figure 8 (a) and dark field in Figure 8 (b) [116, 117]. It is a consequence of the low-cost method used here for graphene transfer. In any case, PMMA is used on biomedical applications because of its good biocompatibility [83, 115] and despite some concerns such as its cytotoxicity [118], the quantity of PMMA found here is very
24 low and is expected to not interfere in graphene performance. Finally, the SEM image of coated substrates is presented in Figure 8 (c) confirming the presence of graphene wrinkles at the SLG coating surface, produced during the transfer process [119]. 3.3. Cytotoxicity and biocompatibility test Results of cell growth for the 72 hours’ biocompatibility tests (uncoated and coated samples) are depicted in Figure 9. MEF cells cultured on the graphene-coated samples, showed an exponential growth phase similar to that obtained in fresh medium, indicating that SLG is an optimal material for MEF cell growth. However, cells directly seeded onto the uncoated substrate did not grow, suggesting that they cannot adhere to the metallic material without surface treatment. According to these results, since the Ti alloy does not exhibit cytotoxicity but shows poor cell adhesion, it can be treated by using a SLG coating to promotes cell growth. At 72h, the results show a reduced cell proliferation on graphene-coated materials compared to the fresh medium. This behavior is similar to the one observed when cells begin the osteoblastic differentiation process which decreases proliferation rate. Another aspect to be considered is the intrinsic physical damage of SLG coating when it is transferred using PMMA-assisted method. This might lead to a partially covered substrate that may influence the cell growth rate. However, as previously mentioned, the cell proliferation values are reasonable from a biological point of view, suggesting that SLG improves the cell growth and adhesion of cells on the porous Ti- 35Nb-29Ta-4Mn substrate. The morphology of the cells at 24, 48, and 72 hours is shown in Figure S4. The cells grown on the graphene-coated samples presented a spherical morphology at 24 hours, and some of them already begin to show a typical fibroblastic cell morphology when cells are adhering to the surface. At 72 hours, the cell’s elongated shape, standard in fibroblasts, was observed and a larger
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39 Figure 1. Diagram representing the PMMA-assisted transfer method used to obtain graphenecoated Ti-35Nb-29Ta-4Mn foam samples. Figure 2. Optical micrographs of foams obtained by space-holder technique: (a) c.p. Ti–Tsint: 1250 °C; (b) 4 wt.% Mn– Tsint: 1200 °C; (c) 4 wt.% Mn – Tsint: 1300 °C. SEM micrographs showing wall thickness (d) 1200 ºC and (e) 1300 °C and inner porous roughness (f) 1200 °C and (g) 1300 ºC. Figure 3. Pore size distribution: (a) 1200 °C and b) 1300 °C. Figure 4. XRD patterns of samples Ti-35Nb-29Ta-xMn sintered at: (a) 1200 °C and (b) 1300 °C. The Ti-β phase, Nb and Ta have the same crystalline structure and space group (Im-3m), with XRD peaks very close in 2θ values. Indexing was performed using the following reference diffraction patterns from the PDF-4+ database of the International Centre for Diffraction Data (ICDD): Ti-β (44-1288), Ti-α (44-1294), Nb (34-0370), Ta (04-0788) and Mn (32-0637). Figure 5. TEM characterization of foams with 4 wt.% Mn at 1200 ºC: (a) TEM image and polycrystalline electron diffraction pattern; (b) HR-TEM image and specific areas Fast Fourier Transformation. Figure 6. Mechanical behavior of Ti-35Nb-29Ta-xMn (x: 2, 4, 6 wt.%) foams: (a) 1200 °C; (b) 1300 °C. Effect of temperature and wt.% Mn on ductility and strength in porous structures of titanium alloys produced via space-holder. Figure 7. (a) Large-scale STM topography (120 × 120 nm2) of single-layer graphene grown on Cu; (b) High-magnification STM image (1.3 × 1.3 nm2) showing the hexagonal lattice atomic structure of single-layer graphene on Cu with lattice constant 2.4 Å, according to Fourier transform analysis (inset). Tunnel current and bias voltages were between 0.1 and 0.9 nA and
40 0.05–1 V; (c) Raman spectra of transferred graphene over SiO2; (d) Raman spectra of monolayer graphene on substrates: on a solid surface of the foam (blue), and suspended on a pore (red). MO images of areas where Raman spectra of (e) graphene on porous substrate and (f) graphene suspended on pore were obtained. Figure 8. Optical micrograph of 4 wt.% Mn: (a) substrates coated with a SLG; (b) Detail of PMMA residues on SLG coatings at high magnification (dark field); SEM micrographs of substrates coated with SLG on solid surface, showing (c) wrinkles on SLG coating, and (d) graphene suspended on pores and roughness inside of pores. Figure 9. Growth of MEF cells with liquid extract and direct contact onto graphene-coated material.
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Supplementary Material Click here to download Supplementary Material: Supporting Information (reviewed).docx
CRediT author statement The manuscript was written with the contributions of all authors. All authors have given approval to the final version of the manuscript. Sheila Lascano: Investigation, Writing- Review & Editing, Funding acquisition, Ricardo Chávez-Vásconez: Investigation, Formal analysis, Writing, Daniela Muñoz-Rojas: Investigation, Formal analysis, Juliet Aristizabal: Investigation, Writing- Original Draft, Bárbara Arce: Investigation, Carolina Parra: Investigation, Resources, Writing- Review & Editing, Cristian Acevedo: Investigation, Resources and Writing, Nicole Orellana: Investigation, Formal Analysis, Mauricio Reyes-Valenzuela: Investigation, Formal Analysis, Francisco José Gotor: Formal Analysis, Review & Editing, Cristina Arévalo: Investigation, Resources, Writing- Review & Editing, Yadir Torres: Investigation, Review & Funding acquisition *Credit Author Statement