Increased use of titanium and titanium-base alloys in medicine is occurring due to their relatively low elasticity modulus and enhanced corrosion resistance as compared to more convenient alloys intended for implantation into the human body [1]. However, the properties of oxides present in the near-surface region of Tibase materials deserve special attention. The titanium oxides from TiO to Ti3O5 can exist in a stable state at the harsh conditions of the body fluids surrounding the implant. Tribo-chemical reactions during use can modify the oxidized surface of the implant producing wear debris accumulation, which results in an adverse cellular response and implant loosening. To improve bone response and reliability of implanted device, the surface modification by coating of implants with various substances can be used. In particular, titanium carbide on titanium can provide protection against oxidation, excellent corrosion resistance, enhanced hardness, and superior wear resistance of the implant. To cover a substrate with a thin carbide film, different methods are commonly used, e.g., chemical vapor phase deposition, pulsed laser ablation deposition (PLAD), magnetron sputtering [2–4]. The present study is aimed at the study of the hardness of electron beam deposited (EBD) titanium carbide films onto Ti substrates. To prepare the targets for EBD, titanium carbide powder (Aldrich, 98% pure) was pressed into 18 mm diameter pellets. The pellets were placed into a crucible made of titanium diboride/boron nitride composite (Advanced Ceramics Corp. Europe, UK). The crucible was then inserted into a water-cooled electron beam gun (EVI-8, Ferrotec, Germany), which has been positioned into a stainless-steel chamber evacuated by a turbomolecular pump supported by a rotation pump. The electron beam gun was controlled by a joypad that permits a complete control of the accelerating voltage in the range between −3.05 and −10 kV, the shape, pattern and position of the beam. The maximum operation power was 5 kW. The gun has a magnetic lenses system that allows a 270 ◦ deflection of the beam for avoiding contamination of the evaporating material with tungsten of the emitting filament. The substrates were heated under vacuum of 5.10−2 mbar in the chamber with a high-power halogen lamp. The deposition process was performed at the accelerating voltage −3.5 kV and the emission current of 130 to 200 mA. The pattern of electron beam was circular and slow, to ensure uniform consumption of the evaporating material. The deposition was performed at the substrate pre-heating temperature 200 or 800 ◦C for several minutes. After the cooling and venting with N2, the samples were of metallic luster and dark grey colored. The thickness of film was evaluated by scanning electron microscopy observation of the cross-sections of the samples (a LEO 1530 SEM apparatus, Carl Zeiss, Germany). An absolute error of the thickness measurement was ±10 nm. The hardness was measured with the use of a Leica VMHT apparatus (Leica GmbH, Germany) equipped with a standard Vickers pyramidal indenter (square-based diamond pyramid of face angle 136 ◦). On each sample indentations were made with 5 to 7 loads ranging from 0.01 to 5 N. Both diagonals were measured to diminish the effects of asymmetry on the imprint. Standard deviation of the diagonal measurements was about 5 to 9% of the diagonal length. The measured hardness was that of the film-substrate composite system. To separate the hardness of the film-substrate system on its constituents from the film and the substrate, a model based on an area “law-of-mixtures” approach was applied [5], where the composite hardness Hc of the film-substrate system is expressed as
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