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  1. NTU Theses and Dissertations Repository
  2. 工學院
  3. 工程科學及海洋工程學系
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/79329
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor趙修武zh_TW
dc.contributor.advisorShiu-Wu Chauen
dc.contributor.author邱勝瑄zh_TW
dc.contributor.authorSheng-Hsuan Chiuen
dc.date.accessioned2022-11-23T08:58:14Z-
dc.date.available2024-05-30-
dc.date.copyright2021-11-04-
dc.date.issued2021-
dc.date.submitted2002-01-01-
dc.identifier.citation[1] B. Selvan, K. Ramachandran, K. Sreekumar, T. Thiyagarajan, and P. Ananthapadmanabhan, "Numerical and experimental studies on DC plasma spray torch," Vacuum, vol. 84, no. 4, pp. 444-452, 2009.
[2] 徐少駒,在不同背壓條件下非傳輸型井式陰極直流空氣電漿火炬內部流場模擬,國立臺灣科技大學機械工程系碩士論文,2013。
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[13] R. Huang, H. Fukanuma, Y. Uesugi, and Y. Tanaka, "An improved local thermal equilibrium model of DC arc plasma torch," IEEE Transactions on Plasma Science, vol. 39, no. 10, pp. 1974-1982, 2011.

[14] J. Trelles, J. Heberlein, and E. Pfender, "Non-equilibrium modelling of arc plasma torches," Journal of Physics D: Applied Physics, vol. 40, no. 19, p. 5937, 2007.
[15] J. M. Park, K. S. Kim, T. H. Hwang, and S. H. Hong, "Three-dimensional modeling of arc root rotation by external magnetic field in nontransferred thermal plasma torches," IEEE Transactions on Plasma Science, vol. 32, no. 2, pp. 479-487, 2004.
[16] J. L. Dorier, M. Gindrat, C. Hollenstein, A. Salito, M. Loch, and G. Barbezat, "Time-resolved imaging of anodic arc root behavior during fluctuations of a DC plasma spraying torch," IEEE Transactions on Plasma Science, vol. 29, no. 3, pp. 494-501, 2001.
[17] Z. Duan and J. Heberlein, "Arc instabilities in a plasma spray torch," Journal of Thermal Spray Technology, vol. 11, no. 1, pp. 44-51, 2002.
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[21] M. J. Ni, R. Munipalli, N. B. Morley, P. Huang, and M. A. Abdou, "Validation case results for 2D and 3D MHD simulations," Fusion Science and Technology, vol. 52, no. 3, pp. 587-594, 2007.
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[38] D. L. Lin, S. H. Chen, and C. C. Tzeng, "Characteristics of a Non-Transferred Plasma Torch Operated in a Positive Pressure Environment", INER-8651R, 2011. (in Chinese)
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dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/79329-
dc.description.abstract本研究使用有限體積法離散基於連續方程式、動量方程式、能量方程式、電磁場方程式及SST k-ω紊流模型的磁流體動力方程組,建立非傳輸型井式直流電漿火炬的三維暫態數學模型,並開發流場分析程式碼。本研究的火炬長690 mm,火炬半徑11 mm,模擬分析工作壓力為1大氣壓條件下,流量範圍為100 SLM至200 SLM間以及工作電流為100 A至200 A 間的空氣電漿火炬特性,並假定陰極弧根以1000 Hz頻率環繞火炬內壁移動。本研究利用迴歸分析計算結果顯示電弧長度正比於工作電流的-1.008次方以及入流流量的0.295次方;出口平均軸向速度正比於工作電流的-0.754次方以及入流流量的1.691次方;出口平均旋向速度正比於工作電流的-2.061次方以及入流流量的3.491次方;出口平均溫度正比於工作電流的-0.415次方以及入流流量的0.427次方。zh_TW
dc.description.abstractThis study develops a numerical framework where a finite volume method is used to discretize the MHD equations consisting of the continuity, momentum, energy, Maxwell's equations and the SST k-ω turbulence model. A three-dimensional unsteady model is established to simulate a non-transferred direct-current plasma torch equipped with well-type cathode. The investigated torch has a length of 690 mm and a radius of 11 mm. The plasma torch flow is calculated at an inlet flow rate ranging from 100 SLM to 200 SLM and a working current ranging from 100 A to 200 A. The working pressure is 1 atm where the cathode spot is assumed to have a circulation frequency of 1000 Hz. With the help of a regression analysis, the arc length is predicted to grow with I^(-1.008) and Q^0.295; the mean axial velocity at the outlet is predicted to grow with I^(-0.754) and Q^1.691; the mean tangential velocity at the outlet is predicted to grow with I^(-2.061) and Q^3.491; the mean temperature at the outlet is predicted to grow with I^(-0.415) and Q^0.427.en
dc.description.provenanceMade available in DSpace on 2022-11-23T08:58:14Z (GMT). No. of bitstreams: 1
U0001-2710202110133000.pdf: 8638523 bytes, checksum: 7c3247665ff7f6cfc3b97a82367da8cd (MD5)
Previous issue date: 2021
en
dc.description.tableofcontentsContents
Nomenclature v
Acronyms v
Latin Symbols vi
Greek Symbols xi
List of Figures xiii
List of Tables xvii
Chapter 1 Introduction 1
Chapter 2 Method 7
2-1 Governing Equations 7
2-1-1 Magnetohydrodynamic Equations 7
2-1-2 Boundary Conditions 11
(a) Inlet 11
(b) Outlet 11
(c) Wall 12
(d) Symmetry Plane 13
(e) Cathode 13
(f) Anode 14
2-2 Numerical Method 16
2-2-1 Finite Volume Method 16
(a) Transient Term 18
(b) Convection Term 18
(c) Diffusion Term 19
2-2-2 Pressure-correction Equation 21
2-2-3 Wall Distance Calculation 24
2-2-4 Solution Procedure 25
Chapter 3 Study Case 29
3-1 Description of Experiment 29
3-2 Case Description 30
3-3 Computational Domain and Boundary Conditions 31
(a) Cathode 34
(b) Anode 35
3-4 Plasma Properties 38
3-5 Mesh 41
3-6 Grid Dependency 44
Chapter 4 Result and Discussion 48
4-1 Validation 48
4-2 Working Current 52
4-2-1 Time-Averaged Analysis 52
4-2-2 Time History Analysis 62
4-3 Inlet Flow Rate 71
4-3-1 Time-Averaged Analysis 71
4-3-2 Time History Analysis 80
4-4 Discussion 86
Chapter 5 Conclusions and Future Works 95
Appendix 97
References 99
-
dc.language.isozh_TW-
dc.subject直流電漿火炬zh_TW
dc.subject暫態zh_TW
dc.subject三維zh_TW
dc.subject磁流體模型zh_TW
dc.subject空氣電漿zh_TW
dc.subject井式陰極zh_TW
dc.subjectWTCen
dc.subjectDC Plasma Torchen
dc.subjectAir Plasmaen
dc.subjectMagnetohydrodynamic Modelen
dc.subjectThree-dimensionalen
dc.subjectUnsteadyen
dc.title三維暫態直流電漿火炬模擬zh_TW
dc.titleThree-Dimensional Unsteady Simulation of Direct Current Plasma Torchen
dc.typeThesis-
dc.date.schoolyear109-2-
dc.description.degree碩士-
dc.contributor.oralexamcommittee吳宗信;陳孝輝;魏大欽;林洸銓;戴璽恆zh_TW
dc.contributor.oralexamcommitteeZhong-Xing Wu;Xiao-Hui Chen;Ta-Chin Wei;Kuang C. Lin;Hsi-Heng Daien
dc.subject.keyword直流電漿火炬,井式陰極,空氣電漿,磁流體模型,三維,暫態,zh_TW
dc.subject.keywordDC Plasma Torch,WTC,Air Plasma,Magnetohydrodynamic Model,Three-dimensional,Unsteady,en
dc.relation.page104-
dc.identifier.doi10.6342/NTU202104312-
dc.rights.note同意授權(全球公開)-
dc.date.accepted2021-10-31-
dc.contributor.author-college工學院-
dc.contributor.author-dept工程科學及海洋工程學系-
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