| 研究生: |
許富傑 Hsu, Fu-Chieh |
|---|---|
| 論文名稱: |
以分子動力學分析在受壓縮負荷的Nix-Al100-x金屬玻璃奈米線之機械性質 A Study on Mechanical Behaviors of Nix-Al100-x Metallic Glasses Nanowires under Compressive Test by Molecular Dynamics Simulation |
| 指導教授: |
陳鐵城
Chen, Tei-Chen |
| 學位類別: |
碩士 Master |
| 系所名稱: |
工學院 - 機械工程學系 Department of Mechanical Engineering |
| 論文出版年: | 2017 |
| 畢業學年度: | 105 |
| 語文別: | 中文 |
| 論文頁數: | 93 |
| 中文關鍵詞: | 鎳-鋁金屬玻璃 、奈米線 、分子動力學 、壓縮 、挫曲 |
| 外文關鍵詞: | NixAly metallic glasses, Nanowires (NWs), Molecular dynamics, Slenderness ratio, Buckling |
| 相關次數: | 點閱:172 下載:12 |
| 分享至: |
| 查詢本校圖書館目錄 查詢臺灣博碩士論文知識加值系統 勘誤回報 |
金屬玻璃由於其獨特的機械和物理性能而引起廣泛的關注,而奈米結構中又以奈米線特別受到注意,由於其優越的機械、光學和電學性質。本研究重點在於探討鎳-鋁金屬玻璃奈米線在奈米尺度下的機械以及材料性質。在模擬理論方法上,使用分子動力學法與EAM勢能函數作為理論基礎,並配合開放式軟體LAMMPS做為工具,分析在不同細長比、淬火速率、合金比例、壓縮速率、溫度、缺陷等條件下之鎳-鋁金屬玻璃奈米線受單軸壓縮情形,並且分析材料的應力分佈、晶相變化、剪應變、滑移系統以及金屬玻璃奈米線在壓縮下的挫曲情形。其結果顯示當淬火速率越低,極限應力和楊氏模數越高,而當在相同的淬火速率之下進行軸向壓縮,極限應力隨細長比的下降而上升。在合金比例的影響下,相具有最高的極限應力和楊氏模數。而當淬火速率在5K/ps和50K/ps時,奈米線對於溫度的影響無明顯的改變,不過當淬火速率下降到0.5K/ps時,奈米線的極限應力隨著溫度的上升而下降。當在較低的壓縮速率下,最大剪應變會發生在彎曲處,而當壓縮速率提升到0.5%/ps時,最大剪應變則會發生在固定端側,且有原子堆積的現象。而在金屬玻璃奈米線缺陷的影響中,淬火速率在0.5K/ps時,奈米線非晶比例受缺陷的影響最大,導致應力值下降的最多。
This study investigated the mechanical properties and deformation mechanism of Nix-Al100-x metallic glasses nanowires (NWs) at nanoscale. Molecular dynamics simulation was carried out using the program package LAMMPS with Embedded-Atom potential. Simulation was performed and focused on the effects of different slenderness ratio, quenching rate, alloy ratio, compression rate, temperature, defects and fracture process of Nix-Aly metallic glasses nanowires under uniaxial compression. Simulation results show that when the quenching rate is lower, the ultimate stress and the Young's modulus become higher. Moreover, under the same quenching rate, the ultimate stress increases with the decrease of the slenderness ratio. For different alloy ratio, it is found that phase has the highest ultimate stress and Young's modulus. When the quenching rate is within the range from 5 to 50 K/ps, the effect of temperature is insignificant. However, when the quenching rate decreases to 0.5 K/ps, the ultimate stresses of nanowires decrease with the increase of temperature. Finally, the deformation mechanism and fracture phenomena are evaluated and discussed.
[1] 李思毅, 李佳穎, and 曾俊元, "奈米材料的製程及其潛在的應用," 物理雙月刊, vol. 26, pp. 473-482, 2004.
[2] J. Irving and J. G. Kirkwood, "The statistical mechanical theory of transport processes. IV. The equations of hydrodynamics," The Journal of chemical physics, vol. 18, pp. 817-829, 1950.
[3] B. J. Alder and T. E. Wainwright, "Studies in molecular dynamics. I. General method," The Journal of Chemical Physics, vol. 31, pp. 459-466, 1959.
[4] L. Verlet, "Computer" experiments" on classical fluids. I. Thermodynamical properties of Lennard-Jones molecules," Physical review, vol. 159, p. 98, 1967.
[5] B. Quentrec and C. Brot, "New method for searching for neighbors in molecular dynamics computations," Journal of Computational Physics, vol. 13, pp. 430-432, 1973.
[6] D. Rapaport, "Molecular-dynamics study of Rayleigh-Bénard convection," Physical review letters, vol. 60, p. 2480, 1988.
[7] G. S. Grest, B. Dünweg, and K. Kremer, "Vectorized link cell Fortran code for molecular dynamics simulations for a large number of particles," Computer Physics Communications, vol. 55, pp. 269-285, 1989.
[8] W. Klement, R. Willens, and P. Duwez, "Non-crystalline structure in solidified gold–silicon alloys," Nature, vol. 187, pp. 869-870, 1960.
[9] H. Chen and D. Turnbull, "Formation, stability and structure of palladium-silicon based alloy glasses," Acta metallurgica, vol. 17, pp. 1021-1031, 1969.
[10] A. Inoue, T. Zhang, and T. Masumoto, "Al--La--Ni amorphous alloys with a wide supercooled liquid region," Materials transactions, JIM, vol. 30, pp. 965-972, 1989.
[11] A. Inoue, A. Kato, T. Zhang, S. Kim, and T. Masumoto, "Mg--Cu--Y Amorphous Alloys With High Mechanical Strengths Produced by a Metallic Mold Casting Method," Materials Transactions, JIM, vol. 32, pp. 609-616, 1991.
[12] A. Peker and W. L. Johnson, "A highly processable metallic glass: Zr41. 2Ti13. 8Cu12. 5Ni10. 0Be22. 5," Applied Physics Letters, vol. 63, pp. 2342-2344, 1993.
[13] J. Y. Lee, K. H. Han, J. M. Park, K. Chattopadhyay, W. T. Kim, and D. H. Kim, "Deformation and evolution of shear bands under compressive loading in bulk metallic glasses," Acta Materialia, vol. 54, pp. 5271-5279, 2006.
[14] A. Alavi, K. Mirabbaszadeh, P. Nayebi, and E. Zaminpayma, "Molecular dynamics simulation of mechanical properties of Ni–Al nanowires," Computational Materials Science, vol. 50, pp. 10-14, 2010.
[15] J. Wang, P. D. Hodgson, J. Zhang, W. Yan, and C. Yang, "Effects of pores on shear bands in metallic glasses: A molecular dynamics study," Computational Materials Science, vol. 50, pp. 211-217, 2010.
[16] J. G. Wang, K. C. Chan, J. C. Fan, L. Xia, G. Wang, and W. H. Wang, "Buckling of metallic glass bars," Journal of Non-Crystalline Solids, vol. 387, pp. 1-5, 2014.
[17] J. Wachter, G. Gutiérrez, A. Zúñiga, and R. Palma, "Buckling of Cu–Zr-based metallic glasses nanowires: molecular dynamics study of surface effects," Journal of Materials Science, vol. 49, pp. 8051-8056, 2014.
[18] P.-H. Sung and T.-C. Chen, "Effects of quenching rate on crack propagation in NiAl alloy using molecular dynamics," Computational Materials Science, vol. 114, pp. 13-17, 2016.
[19] L. A. Girifalco and V. G. Weizer, "Application of the Morse potential function to cubic metals," Physical Review, vol. 114, p. 687, 1959.
[20] J. E. Jones, "On the determinations of molecular fields - 1 From the variation of the viscosity of a gas with temperature," Proceedings of the Royal Society of London Series a-Containing Papers of a Mathematical and Physical Character, vol. 106, pp. 441-462, 1924.
[21] J. E. Jones, "On the determination of molecular fields - II From the equation of state of a gas," Proceedings of the Royal Society of London Series a-Containing Papers of a Mathematical and Physical Character, vol. 106, pp. 463-477, 1924.
[22] J. E. Jones, "On the determination of molecular fields III - From crystal measurements and kinetic theory data," Proceedings of the Royal Society of London Series a-Containing Papers of a Mathematical and Physical Character, vol. 106, pp. 709-718, 1924.
[23] M. S. Daw, S. M. Foiles, and M. I. Baskes, "The embedded-atom method: a review of theory and applications," Materials Science Reports, vol. 9, pp. 251-310, 1993.
[24] F. Cleri and V. Rosato, "Tight-binding potentials for transition metals and alloys," Physical Review B, vol. 48, p. 22, 1993.
[25] W. Cheong and L. Zhang, "Monocrystalline silicon subjected to multi-asperity sliding: nano-wear mechanisms, subsurface damage and effect of asperity interaction," International Journal of Materials and Product Technology, vol. 18, pp. 398-407, 2003.
[26] J. Tersoff, "New empirical approach for the structure and energy of covalent systems," Physical Review B, vol. 37, p. 6991, 1988.
[27] J. Tersoff, "Empirical interatomic potential for silicon with improved elastic properties," Physical Review B, vol. 38, p. 9902, 1988.
[28] J. Tersoff, "Modeling solid-state chemistry: Interatomic potentials for multicomponent systems," Physical Review B, vol. 39, p. 5566, 1989.
[29] T. Iwaki, "Molecular dynamics study on stress-strain in very thin film: Size and location of region for defining stress and strain," JSME international journal. Ser. A, Mechanics and material engineering, vol. 39, pp. 346-353, 1996.
[30] A. Inoue, "Bulk amorphous and nanocrystalline alloys with high functional properties," Materials Science and Engineering: A, vol. 304, pp. 1-10, 2001.
[31] A. Inoue, "Bulk amorphous alloys with soft and hard magnetic properties," Materials Science and Engineering: A, vol. 226, pp. 357-363, 1997.
[32] A. Inoue, T. Zhang, and A. Takeuchi, "Ferrous and nonferrous bulk amorphous alloys," in Materials Science Forum, vol. 269, p. 855, 1998.
[33] A. Inoue, A. Takeuchi, and T. Zhang, "Ferromagnetic bulk amorphous alloys," Metallurgical and Materials Transactions A, vol. 29, pp. 1779-1793, 1998.
[34] R. E. Reed-Hill and R. Abbaschian, "Physical metallurgy principles, PWS Publ," Comp., Boston, vol. 853, p. 841, 1994.
[35] D. Turnbull, "Under what conditions can a glass be formed?," Contemporary physics, vol. 10, pp. 473-488, 1969.
[36] D. R. Uhlmann, "A kinetic treatment of glass formation," Journal of Non-Crystalline Solids, vol. 7, pp. 337-348, 1972.
[37] Z. Lu, Y. Li, and S. Ng, "Reduced glass transition temperature and glass forming ability of bulk glass forming alloys," Journal of non-crystalline solids, vol. 270, pp. 103-114, 2000.
[38] Z. Lu and C. Liu, "A new glass-forming ability criterion for bulk metallic glasses," Acta materialia, vol. 50, pp. 3501-3512, 2002.
[39] G.-F. Wang and X.-Q. Feng, "Surface effects on buckling of nanowires under uniaxial compression," Applied physics letters, vol. 94, p. 141913, 2009.