Acta Physica Sinica, Volume. 68, Issue 9, 096201-1(2019)

Theoretical calculations of stabilities and properties of transition metal borocarbides TM3B3C and TM4B3C2 compound

Qian-Ku Hu1,2、*, Yi-Ming Hou1, Qing-Hua Wu1, Shuang-Hong Qin1, Li-Bo Wang1, and Ai-Guo Zhou1
Author Affiliations
  • 1School of Materials Science and Engineering, Henan Key Laboratory of Materials on Deep-Earth Science and Technology, Henan Polytechnic University, Jiaozuo 454000, China
  • 2State Key Laboratory of Metastable Materials Science and Technology, Yanshan University, Qinhuangdao 066004, China
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    Figures & Tables(7)
    Crystal structures of the (a), (b) Nb3B3C and (c), (d) Nb4B3C2. The light brown, blue and pink spheres represent Nb, B and C atoms, respectively. The Nb6B trigonal prisms and Nb6C octahedrons are painted green and dark brown.(a), (b) Nb3B3C和(c), (d) Nb4B3C2的晶体结构(棕球, Nb原子; 蓝球, B原子; 粉球, C原子; Nb6B三棱柱和Nb6C八面体分别用绿色和褐色表示)
    Energy differences of Ta3B3C and Ta4B3C2 phases with respect to their most competing phases as a function of temperature.不同温度下Ta3B3C, Ta4B3C2相分别和其相应最稳定竞争组合相的自由能之差
    Phonon dispersion curves of (a) Ta3B3C and (b) Ta4B3C2 structures.(a) Ta3B3C和(b) Ta4B3C2结构的声子色散曲线
    Band structures and density of states of (a), (c) Ta3B3C and (b), (d) Ta4B3C2 structures.(a), (c) Ta3B3C和(b), (d) Ta4B3C2结构的能带结构和态密度图
    • Table 1.

      Structural parameters of the Nb3B3C, Nb4B3C2, Ta3B3C and Ta4B3C2 configurations.

      Nb3B3C, Nb4B3C2, Ta3B3C和Ta4B3C2晶体的结构参数

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      Table 1.

      Structural parameters of the Nb3B3C, Nb4B3C2, Ta3B3C and Ta4B3C2 configurations.

      Nb3B3C, Nb4B3C2, Ta3B3C和Ta4B3C2晶体的结构参数

      模型晶系和空间群晶格参数(Å, degree)原子坐标
      注: a文献[17]中的实验值.
      Nb3B3C Orthorhombic Cmcma = 3.284, 3.265a, b = 28.877, 28.710a, c = 3.144, 3.129a, α = β = γ = 90 Nb1 (4c) (0, 0.2128, 0.25), Nb2 (4c) (0, 0.3620, 0.25), Nb3 (4c) (0, 0.4532, 0.25), B1 (4c) (0, 0.1120, 0.25), B2 (4c) (0, 0.0155, 0.25), B3 (4c) (0, 0.0790, 0.25), C (4c) (0, 0.2878, 0.25)
      Nb4B3C2Orthorhombic Cmcma = 3.257, 3.229a, b = 37.874, 37.544a, c = 3.153, 3.133a, α = β = γ = 90 Nb1 (4c) (0, 0.1621, 0.75), Nb2 (4c) (0, 0.2805, 0.75), Nb3 (4c) (0, 0.3946, 0.75), Nb4 (4c) (0, 0.4642, 0.25), B1 (4c) (0, 0.0854, 0.75), B2 (4c) (0, 0.0118, 0.25), B3 (4c) (0, 0.0602, 0.25), C1 (4c) (0, 0.2202, 0.75), C2 (4c) (0, 0.3383, 0.75)
      Ta3B3C Orthorhombic Cmcma = 3.267, b = 28.688, c = 3.133, α = β = γ = 90 Ta1 (4c) (0, 0.2121, 0.25), Ta2 (4c) (0, 0.3619, 0.25), Ta3 (4c) (0, 0.4531, 0.25), B1 (4c) (0, 0.1130, 0.25), B2 (4c) (0, 0.0155, 0.25), B3 (4c) (0, 0.0791, 0.25), C (4c) (0, 0.2874, 0.25)
      Ta4B3C2Orthorhombic Cmcma = 3.243, b = 37.609, c = 3.141, α = β = γ = 90 Ta1 (4c) (0, 0.1615, 0.75), Nb2 (4c) (0, 0.2806, 0.75), Nb3 (4c) (0, 0.3945, 0.75), Nb4 (4c) (0, 0.4641, 0.25), B1 (4c) (0, 0.0861, 0.75), B2 (4c) (0, 0.0118, 0.25), B3 (4c) (0, 0.0602, 0.25), C1 (4c) (0, 0.2202, 0.75), C2 (4c) (0, 0.3380, 0.75)
    • Table 2.

      Calculated formation enthalpies of different TM3B3C and TM4B3C2 phases (eV/atom).

      不同成分TM3B3C和TM4B3C2的形成焓(eV/atom)

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      Table 2.

      Calculated formation enthalpies of different TM3B3C and TM4B3C2 phases (eV/atom).

      不同成分TM3B3C和TM4B3C2的形成焓(eV/atom)

      TMTM3B3C TM4B3C2
      $\Delta {H_{{\rm{elements}}}}$$\Delta {H_{{\rm{comp}}}}$最稳定竞争组合$\Delta {H_{{\rm{elements}}}}$$\Delta {H_{{\rm{comp}}}}$最稳定竞争组合
      Sc–0.6370.0716ScB2 + Sc4C3 + Sc2C = 4Sc3B3C –0.5200.14410ScB2 + 4Sc4C3 + Sc2BC2 = 7Sc4B3C2
      Ti–0.8960.0199TiB2 + TiC + Ti8C5 = 6Ti3B3C –0.8630.0189TiB2 + 7TiC + Ti8C5 = 6Ti4B3C2
      V–0.6870.1013VB + C = V3B3C –0.6280.09218VB + 7C + V6C5 = 6V4B3C2
      Cr–0.2940.1593CrB + C = Cr3B3C –0.1940.1789CrB + 4C + Cr3C2 = 3Cr4B3C2
      Mn–0.1000.1953MnB + C = Mn3B3C 0.024
      Fe0.0020.139
      Co0.0940.255
      Ni0.2960.456
      Cu0.7380.959
      Zn0.7130.929
      Y–0.3850.0899YB2 + 5Y2C + Y2B3C2 = 7Y3B3C –0.2830.1606YB2 + 8Y2C + 3Y2B3C2 = 7Y4B3C2
      Zr–0.8510.0193ZrB2 + 2ZrC + Zr = 2Zr3B3C –0.8380.0203ZrB2 + 4ZrC + Zr = 2Zr4B3C2
      Nb–0.698–0.0233NbB + C = Nb3B3C –0.661–0.002C + 6Nb3B3C + Nb6C5 = 6Nb4B3C2
      Mo–0.2570.1753MoB + C = Mo3B3C –0.1550.2023MoB + C + MoC = Mo4B3C2
      Tc–0.0050.32612TcB2 + 11C + 3Tc7B3 = 11Tc3B3C 0.138
      Ru0.211–0.369
      Rh0.230–0.406
      Pd0.5520.744
      Ag1.0271.295
      Cd0.8461.112
      Hf–0.9200.0163HfB2 + 2HfC + Hf = 2Hf3B3C –0.9220.0183HfB2 + 4HfC + Hf = 2Hf4B3C2
      Ta–0.7040.0033Ta3B4 + C + 3TaC = 4Ta3B3C –0.691–0.0103Ta3B4 + C + 7TaC = 4Ta4B3C2
      W–0.0940.2273WB + C = W3B3C –0.0070.2733WB + C + WC = W4B3C2
      Re0.2810.425
      Os0.5900.755
      Ir0.6040.758
      Pt0.7080.855
      Au1.0961.310
      Hg1.1861.333
    • Table 3.

      Calculated elastic constants Cij, bulk modulus B, shear modulus G, Vickers hardness HV of Ta3B3C and Ta4B3C2 configurations (GPa).

      Ta3B3C, Ta4B3C2结构的弹性常数、体弹模量、剪切模量和维氏硬度 (GPa)

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      Table 3.

      Calculated elastic constants Cij, bulk modulus B, shear modulus G, Vickers hardness HV of Ta3B3C and Ta4B3C2 configurations (GPa).

      Ta3B3C, Ta4B3C2结构的弹性常数、体弹模量、剪切模量和维氏硬度 (GPa)

      结构弹性常数力学性能a硬度
      C11C22C33C44C55C66C12C13C23BGB/GHChenHTian
      注: a二元相力学性能数据来自Materials Project网站.
      Ta3B3C 569.6514.4563.5194.1180.0261.8187.1147.3173.9295.9200.81.4725.325.3
      Ta4B3C2581.1535.3602.1197.3185.1275.8200.3146.0170.2305.7209.01.4626.226.2
      Nb3B3C 544.3479.8522.8181.5171.9245.3170.9132.9162.2275.3189.71.4524.824.7
      Nb4B3C2551.5499.2548.5184.0175.1257.1183.2132.7157.8282.9195.81.4425.525.4
      TaB23022001.5124.424.5
      NbB22871951.4724.824.8
      TaC3242151.5125.625.9
      NbC2391611.4821.621.4
      SiC2131871.1433.632.2
      Al2O32321471.5818.718.7
      TiN2591801.4424.324.0
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    Qian-Ku Hu, Yi-Ming Hou, Qing-Hua Wu, Shuang-Hong Qin, Li-Bo Wang, Ai-Guo Zhou. Theoretical calculations of stabilities and properties of transition metal borocarbides TM3B3C and TM4B3C2 compound [J]. Acta Physica Sinica, 2019, 68(9): 096201-1

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    Paper Information

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    Received: Jan. 27, 2019

    Accepted: --

    Published Online: Oct. 29, 2019

    The Author Email:

    DOI:10.7498/aps.68.20190158

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