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  1. NTU Theses and Dissertations Repository
  2. 工學院
  3. 應用力學研究所
Please use this identifier to cite or link to this item: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/30062
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???org.dspace.app.webui.jsptag.ItemTag.dcfield???ValueLanguage
dc.contributor.advisor舒貽忠
dc.contributor.authorChi-Pin Chaoen
dc.contributor.author趙起平zh_TW
dc.date.accessioned2021-06-13T01:33:45Z-
dc.date.available2013-08-08
dc.date.copyright2011-08-08
dc.date.issued2011
dc.date.submitted2011-08-02
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[9] T. Kakeshita, K. Shimizu, S. Funada and M. Date, 'Magnetic Field-Induced Martensitic Transformations In Disordered and Ordered Fe-Pt Alloys' Transactions of Japan Insitute of Metals, vol. 25, pp. 837-844. (1984)
[10] K. Oikawa, T. Ohta, F. Gejima, T. Ohmori, R. Kainuma and K. Ishida, 'Phase Equilibria and Phase Transformations in New B2-type Ferromagnetic Shape Memory Alloys of Co-Ni-Ga and Co-Ni-Al Systems,' Materials Transactions, vol.42,pp. 2472-2475, (2001)
[11] K. Oikawa, L. Wulff, T. Iijima, G. Gejima, T. Ohmori, A. Fujita, K. Fukamichi, R. Kainuma and K. Ishida 'Promissing Ferromagnetic Ni-Co-Al Shape Memory Alloy System' Applied Physics Letters, vol.81, pp. 3290-3292.(2001)
[12] M. Wuttig, J. Li and C. Craciunescu, 'A New Ferromaggnetic Shape Memory Alloy System,' Scripta Materialia, vol. 44, pp.2393-2397. (2001)
[13] J. Tellinen, I. Suorsa, A. Jaaskelainen, I. Aaltio and K. Ullakko, 'Basic Properties Of Magnetic Shape Memory Actuators,'8th international conference ACTUATOR ,Bremen, Germany, 10-12 June (2002)
[14] Sozinov A, Likhachev AA, Lanska N, Ullakko K. 'Giant magnetic-field-induced strain in NiMnGa seven-layered martensitic phase,' Applied Physics Letters, vol.80, pp.1746. (2002)
[15] R. Tickle and R. D. James, 'Magnetic and magnetomechanical properties of Ni2MnGa,' Journal of Magnetism and Magnetic Materials, vol.195, pp. 627-638. (1999)
[16] O. Heczko, 'Magnetic shape memory effect and magnetization reversal,' Journal of Magnetism and Magnetic Materials, vol. 290, pp. 787-794. (2005)
[17] A. Sozinov, A. A. Likhachev, N. Lanska, and K. Ullakko, 'Giant magnetic-field-induced strain in NiMnGa seven-layered martensitic phase,' Applied Physics Letters, vol.80, pp.1746. (2002)
[18] Y. F. Ma and J. Y. Li, 'Magnetization rotation and rearrangement of martensite variants in ferromagnetic shape memory alloys,' Applied Physics Letters, vol.90, 172504. (2007)
[19] Y. C. Shu 'Shape-Memory Micropumps. Materials Transactions,' Materials Transactions, vol. 43, pp. 1037-1044. (2002)
[20] L. Q. Chen 'Phase-Field Models for Microstructure Evolution,' Annual Review of Materials Research, vol.32, pp. 113-140. (2002)
[21] J. X. Zhang and L. Q. Chen 'Phase-Field Model for Ferromagnetic Shape Memory Alloys,' Philosophical Magazine Letters, vol. 85, pp.533-541. (2005)
[22] J. X. Zhang and L. Q. Chen 'Phase-Field Microelasticity Theory and Micromagnetic Simulations of Domain Structures in Giant Magnetostrictive Materials,' Acta Materialia, vol.53, pp. 2845-2855, (2005)
[23] Y. C. Shu and J. H. Yen. 'Pattern Formation in Martensitic Thin Films,' Applied Physics Letters, vol. 91, (2007)
[24] Y. C. Shu and J. H. Yen. 'Multivariant Model of Martensitic Microstructure in Thin Films,' Acta Materialia, vol. 56, pp. 3969-3981, (2008).
[25] L. Yang and K. Dayal. 'Formulation of phase-field energies for microstructure in complex crystal structures,' Applied Physics Letters, vol.96, (2010)
[26] L. J. Li, J. Y. Li, Y. C. Shu, H. Z. Chen, and J. H. Yen. 'Magnetoelastic domains and magnetic field-induced strains in ferromagnetic shape memory alloys by phase-field simulation,' Applied Physics Letters, vol. 92, (2008)
[27] L.J. Li, C.H. Lei, Y.C. Shu and J.Y. Li 'Phase-field simulation of magnetoelastic couplings in ferromagnetic shape memory alloys,' Acta Materialia,vol.59 pp.2648-2655. (2011)
[28] X. P. Wang, C. J. Garc’ıa-Cervera, and Weinan E. 'A Gauss–Seidel Projection Method for Micromagnetics Simulations,' Journal of Computational Physics vol.171, pp.357-372, (2001)
[29] L. D. Landau and E. M. Lifshitz, 'On the theory of the dispersion of magnetic permeability in ferromagnetic bodies,' Phys. Z. Sowjet, vol. 8, (1935)
[30] W. F. Brown, 'Micromagntics,' John Wiley & Sons, NY (1963)
[31] G. J. Fix 'Free Boundary Problems: Theory and Applications ed A Fasano and M Primicerio,' Boston:Pitman (1983)
[32] J.S. Langer, 'Models of pattern formation in first-order phase transitions. In Directions in Condensed Matter Physics,' World Scientific.(1986)
[33] J. N. Armstrong, M. R. Sullivan, M. L. Romancer, V. A. Chernenko, and H. Deep Chopra, 'Role of magnetostatic interactions in micromagnetic structure of multiferroics,' Journal of Applied Physics, vol. 103. (2008)
[34] P. P. Wu, X. Q. Ma, J. X. Zhang, and L. Q. Chen 'Phase-field simulations of stress-strain behavior in ferromagnetic shape memory alloy Ni2MnGa.' Journal of Applied Physics, vol. 104, (2008)
[35] Hubert A, Schafer R. 'Magnetic domains: the analysis of magnetic microstructure,' Berlin: Springer (1998)
[36] 顏睿亨(2003), Micromagnetic Simulation of Ferromagnetic Films. 台灣大學應用力學研究所碩士論文
[37] 陳宏志(2007), The Application of Parallel Computation and Fast Algorithm to The Study of Martensitic.台灣大學應用力學所碩士論文
[38] 顏睿亨(2008), Application of Multirank Lamination Theory to the Modeling of Ferroelectric and Martensitic Materials.台灣大學應用力學所博士班論文
[39] 林昇旺(2009), Microstructure simulation of Martensitic thin film/substrate accounting for the out-of-plane inhomogeneity.台灣大學應用力學所碩士論文.
[40] 徐建輝(2007), A novel phase field simulation of Martensitic microstructures. 台灣大學應用力學所碩士論文.
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/30062-
dc.description.abstract鐵磁形狀記憶合金是一個同時具有鐵磁性以及鐵彈性的材料,由於內部微結構排列與演化使其具有多功能的特性,近年來廣泛的被研究。為了正確的使用這些材料,分析與模擬材料內部微結構是極重要的課題,因此從相場法著手進行分析。
本文(1)使用「新式相場法」以及「改良新式相場法」兩種數值模擬方法進行比較,其中發現「改良新式相場法」可以提高模擬效率以及使結果更穩定;(2)以本研究團隊所發展的理論為基礎,將「改良新式相場法」應用在鐵磁形狀記憶合金磁彈耦合中磁域微結構的演化,微觀磁學的部分使用著名的Landau Lifshitz Gilbert方程式來描述磁化向量的演化。最後在這些方程式的描述下,藉由能量最小原理搭配變分法來推導各種能量所造成的驅動力,並利用FFT(Fast Fourier Transform)的技術來計算消磁能以及應力場。4.2.1節中模擬結果與實驗[33]得到圖案相符,4.2.3節中展示材料受壓力後其兄弟晶翻轉的情形,4.2.4節驗證材料受磁場產生極大的應變;但是相對大的應力(blocking stress)會阻止此應變的產生,最後在4.2.5節中模擬了4.2.4節中的應變在適當磁場下的恢復性,證明材料在不同磁場下具有準塑性(quasi-plastic)或偽彈性(pseudo-elastic)的特性。
zh_TW
dc.description.abstractFerromagnetic shape memory alloys (FSMA) are those possessing both ferromagnetic and ferroelastic orderings. Their unique properties are due to the formation of very fine scale magnetic and elastic domains. As a result, these materials have been extensively studied by understanding how and why these domains are formed and arranged. One of the power tools for investigating them is to use the phase-field simulations.
Different from the “novel phase-field method” developed by the research group of Professor Shu, this thesis proposes a modification based on the new choice of phase-field variable [25]. It is shown that the modified method is more efficient and stable than the original approach. Second, we use this modified model, together with Landau-Lifshitz-Gilbert equation, to simulate the magnetoelastic couplings in FSMAs. First, the evolution equations are obtained by the vraiational argument and are solved numerically by Fast Fourier Transform (FFT). In Section 4.2.1, the simulated domain pattern is illustrated to agree well with the observed microstructure. Second in Section 4.2.3, it is shown that applied compressive stress can induce favorable magnetic domains. In addition, Section 4.2.4 demonstrates the effect of force and magnetic fields on the formation of magnetoelastic domains. It is found that magnetic-field-induced strain in FSMAs results from the process of variant rearrangement. Yet such rearrangement can be blocked by a relatively large compressive stress. Finally, it is demonstrated that FSMAs exhibit quasi-plastic or pseudo-elastic behavior depending on the strength of applied magnetic field.
en
dc.description.provenanceMade available in DSpace on 2021-06-13T01:33:45Z (GMT). No. of bitstreams: 1
ntu-100-R98543051-1.pdf: 4182890 bytes, checksum: a12785be2bbd72e07f0b76c3aa0c6983 (MD5)
Previous issue date: 2011
en
dc.description.tableofcontents口試委員會審定書 #
誌謝 1
中文摘要 2
ABSTRACT 3
目錄 4
圖目錄 6
表目錄 8
第1章 導論 9
1.1 研究動機 9
1.2 文獻回顧 10
1.3 致動器(actuator)特性 11
1.4 本文架構 12
第2章 數學模型 13
2.1 鐵磁形狀記憶合金 13
2.1.1 材料特性 13
2.1.2 數學模型 14
2.1.3 能量及小原理 18
2.1.4 演化方程式 21
2.2 新式相場法之比較 23
第3章 數值方法 25
3.1 數值方法求解演化方程式 26
3.2 利用快速傅立葉轉換求解應力 29
3.3 利用快速傅立葉轉換求得雜散場(stray field) 31
第4章 數值模擬結果 32
4.1 比較改良新式相場法與新式相場法 32
4.2 模擬鐵磁形狀記憶合金 37
4.2.1 平均應變為零 38
4.2.2 施加磁場且平均應變為零 41
4.2.3 施加應力場之模擬 43
4.2.4 施加應力場及磁場之模擬 45
4.2.5 擬塑性(quasi-plastic)以及偽彈性(pseudo-elastic)的特性 50
第5章 結論及未來展望 60
5.1 結論 60
5.2 未來展望 61
REFERENCE 62
dc.language.isozh-TW
dc.subject改良新式相場法zh_TW
dc.subject鐵磁形狀記憶合金zh_TW
dc.subject微結構zh_TW
dc.subjectMicrostructureen
dc.subjectModified Novel Phase-Field Methoden
dc.subjectFerromagnetic Shape Memory Alloysen
dc.title改良相場法模擬鐵磁形狀記憶合金磁彈耦合微結構之研究zh_TW
dc.titleModified Phase-Field simulation of magnetoelastic domain in ferromagnetic shape memory alloysen
dc.typeThesis
dc.date.schoolyear99-2
dc.description.degree碩士
dc.contributor.oralexamcommittee陳國慶,劉進賢
dc.subject.keyword鐵磁形狀記憶合金,改良新式相場法,微結構,zh_TW
dc.subject.keywordFerromagnetic Shape Memory Alloys,Modified Novel Phase-Field Method,Microstructure,en
dc.relation.page65
dc.rights.note有償授權
dc.date.accepted2011-08-02
dc.contributor.author-college工學院zh_TW
dc.contributor.author-dept應用力學研究所zh_TW
Appears in Collections:應用力學研究所

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