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采用第一性原理方法, 对孕镶金刚石基底表层Co原子金刚石涂层膜基界面结合作用进行仿真计算分析, 以探究基底中黏结相Co的嵌入深度对金刚石涂层膜基界面结合强度的影响. 计算结果表明, 膜基界面结合能随基底中Co嵌入深度的增大呈先降低后升高的趋势. 当Co原子排列位于第3层时, 涂层生长易出现明显的石墨结构, Co促金刚石石墨化作用最为显著, 膜基界面结合强度达到最小值. 分析结构及电荷发现, 此时在表面效应及Co—C键键长的共同作用下基底第2层C移至表层, 并由sp3杂化转变为sp2杂化, 且C的移动导致Co与周围C原子的作用空间增大、作用数量增多, 加之Co价层未配对电子较多, 易与周围多个碳原子发生电子轨道的混合与重排, 最终使得基底表面呈现为石墨结构. Co位于第5层时不再影响基底表面的稳定构型及膜基界面结合强度.Diamond coating has many excellent properties such as extreme hardness, high elastic modulus, high thermal conductivity, low friction coefficient, low thermal expansion coefficient, and good corrosion resistance. Those properties are close to natural diamond’s, thereby making the diamond coating an ideal new type of wear-resistant tool coating material. However, a large number of experiments have proved that during the deposition of diamond coating, the bonding phase cobalt on the surface of impregnated diamond substrate will generate a layer of graphite at the interface, which seriously weakens the adhesive strength between the substrate and the coating. To thoroughly solve this problem, it is necessary to investigate the microscopic process of graphitization caused by the Co element embedded on the substrate surface. Therefore, the first principle theory is adopted to simulate and analyze the interfacial adhesive strength of diamond coating when Co atom is embedded at different depths on the surface of impregnated diamond substrate, thereby exploring the mechanism of the influence of bonding phase Co element in the substrate on the diamond coating and the mechanism of Co promoting diamond graphitization. The calculation results show that the interfacial binding energy first decreases and then increases with the increase of Co embedding depth in the substrate. When Co atom is embedded in the third layer, obvious graphite structures are prone to appear at the interface, and Co promotes diamond graphitization most significantly, resulting in the minimum bonding strength between the film and substrate interface. The results of structure and charge indicate that under the influence of surface effect and Co—C bond length, the C atoms in the second layer of the substrate move to the first layer and the hybridization mode changes from sp3 to sp2. Meanwhile, this movement leads to an increase in the interaction space and quantity between Co atoms and the surrounding C atoms. In addition, there are many unpaired electrons in the Co valence layer, which can easily mix and rearrange electron orbitals with the surrounding C atoms, ultimately resulting in a graphite structure on the substrate surface. When Co atoms are embedded in the fifth layer, the stable configuration of the substrate surface and the interfacial adhesive strength are no longer affected.
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Keywords:
- diamond coating /
- Co element /
- adhesive strength /
- graphitization
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原子层数/N 层间距变化/% ${\varDelta _{12}}$ ${\varDelta _{23}}$ ${\varDelta _{34}}$ ${\varDelta _{45}}$ ${\varDelta _{56}}$ ${\varDelta _{67}}$ 3 –10.852 5 –11.142 4.606 7 –10.716 4.643 –0.429 9 –10.708 4.643 –0.701 0.933 11 –10.701 4.688 –0.702 0.825 0.472 13 –10.718 4.688 –0.704 0.862 0.330 –0.613 
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基底中
Co位置Eslab1
/eVEslab2
/eVEinterface
/eVA/Å2 Wad/
(J·m–2)表面第1层 –10822.680 –9874.157 –20740.528 56.903 12.302 表面第2层 –10824.324 –20739.004 11.410 表面第3层 –10820.914 –20725.527 8.575 表面第4层 –10816.048 –20735.417 12.730 表面第5层 –10816.702 –20738.245 13.342 不含Co –9879.266 –19801.206 13.454
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Atom Mulliken atomic populations Total electron/e Transfer charge/e s p d Co 0.05 –0.77 7.79 7.06 1.94 C(1) 1.32 2.82 0.00 4.14 –0.14 C(2) 1.19 2.91 0.00 4.10 –0.10 C(3) 1.22 2.94 0.00 4.15 –0.15 C(4) 1.18 3.00 0.00 4.17 –0.17 C(5) 1.22 2.94 0.00 4.15 –0.15 C(6) 1.18 2.91 0.00 4.10 –0.10 C(7) 1.22 2.90 0.00 4.12 –0.12 C(8) 1.17 3.04 0.00 4.20 –0.20 C(9) 1.17 3.04 0.00 4.20 –0.20
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Bond Population Length/Å Co—C(1) –0.22 1.94970 Co—C(2) –0.22 2.02913 Co—C(3) –0.31 1.93623 Co—C(4) –0.19 1.98079 Co—C(5) –0.13 1.93626 Co—C(6) –0.22 2.02911 Co—C(7) 0.41 2.07074 Co—C(8) 0.34 1.88913 Co—C(9) 0.34 1.88915
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