簡易檢索 / 詳目顯示

研究生: 黃怡龍
Huang, Yi-Lung
論文名稱: 六硼化鑭無加熱器中空陰極放電電壓特性研究
Investigation of Discharge Voltage Characteristics in Lanthanum Hexaboride Heaterless Hollow Cathode
指導教授: 李約亨
Li, Yueh-Heng
學位類別: 碩士
Master
系所名稱: 工學院 - 航空太空工程學系
Department of Aeronautics & Astronautics
論文出版年: 2023
畢業學年度: 112
語文別: 英文
論文頁數: 117
中文關鍵詞: 電能推進霍爾推進器中空陰極模式轉換
外文關鍵詞: Electric propulsion, Hall effect thruster, Hollow cathode, mode transition
相關次數: 點閱:55下載:0
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
  • 霍爾推進器做為電能推進器的一種,具有非常高的推力功率比,被世界各國廣泛的應用於衛星的軌道變換、高度維持和深空探索,如BUSEK公司的BHT系列、ESA的PPS-1350和俄羅斯的SPT系列。霍爾推進器的運作需要一穩定電子源提供足夠的電子來離子化燃料氣體和中和被加速的離子束,這使得中空陰極作為一電子源被應用於霍爾推進器上。傳統的中空陰極由陰極管、發射體、保持器和加熱器組成。加熱器被用於加熱發射體以達到陰極的工作溫度,讓發射體發射出電子。但多次的溫度變化過程會造成加熱器材料的熱疲乏,導致加熱器的損壞和短路。這個問題嚴重的影響了陰極的壽命,往往發射體還未蒸發殆盡,加熱器就已經損壞。無加熱器中空陰極的概念因此被提出,透過大流量和高電壓誘發的電弧放電來加熱發射體不僅避免了加熱器損壞的問題也帶來許多好處,包括重量減輕達到更緊湊的設計、減少能量需求和降低電源單元複雜度。
    陰極的運作情況在文獻中被分為點模式和羽流模式。點模式為穩定運作的情況,外觀上為一明亮電漿球出現於保持器出口處。羽流模式為陰極不穩定運作的情況,外觀為大範圍電漿充滿陰極和陽極之間。羽流模式下放電電壓上升,電壓和電流大幅度振盪並產生高能粒子。高能粒子的產生對保持器和陰極的孔徑侵蝕增強,造成陰極的性能和壽命降低。針對陰極的模式轉換,多種以放電電流和電壓振盪幅度為測量值的半經驗公式被提出用以評估陰極的模式轉換。
    本研究利用陽極放電壓和保持器浮動電壓的峰對峰值大於5伏特作為陰極發生模式轉換進入羽流模式的標準,對我們設計的陰極進行性能評估。在流量低於5 sccm時,放電電壓出現大幅振盪,說明陰極進入羽流模式。放電電流範圍4安培到7安培在流量 7 sccm下被測試,但低於振盪標準的峰對峰值說明運作仍然維持在點模式。陰極在兩個不同的背景壓力條件(8.1×10^(-4),3×10^(-4) torr)被測試以評估背景壓力對陰極性能的影響。結果顯示過高的背景壓力造成模式轉消失而無法利用電壓振盪標準來找出陰極的最佳工作流量和放電電流。軸向磁場的施加造成陽極放電電壓下降,推測原因為磁場降低電子的跨場傳輸能力,使得陽極接收電流的有效表面積增加。

    Hall-effect thrusters, as a type of electric propulsion system, offer an exceptionally high thrust-to-power ratio, making them widely utilized in various space applications by countries around the world. They are commonly employed for satellite orbit changes, altitude maintenance, and deep space exploration. Examples include BUSEK's BHT series, ESA's PPS-1350, and Russia's SPT series. The operation of Hall-effect thrusters relies on a stable electron source to ionize propellant gas and neutralize accelerated ion beams. This has led to the utilization of hollow cathodes as electron sources in Hall-effect thrusters. Traditional hollow cathodes consist of a cathode tube, an emitter, a keeper, and a heater. The heater is used to raise the emitter's temperature to the working level, promoting electron emission. However, frequent temperature fluctuations can cause thermal fatigue in the heater material, resulting in damage and short circuits. This issue significantly impacts the cathode's lifespan, often leading to heater failure before the emitter is fully evaporated. The concept of a heaterless hollow cathode has thus been proposed. This approach involves inducing arc discharge through high flow rates and high voltages to heat the emitter. This approach not only avoids the issues related to heater damage but also brings forth several advantages. These include reduced weight, enabling a more compact design, decreased energy requirements, and lowered complexity of the power supply unit.
    The operation of the cathode is categorized in the literature as either the "spot mode" or the "plume mode." In the spot mode, stable operation is observed, characterized by the appearance of a bright plasma ball at the cathode exit plane. In the plume mode, the cathode operates unstably, resulting in a wide-range plasma filling the region between the cathode and anode. In the plume mode, the discharge voltage increases, and both voltage and current exhibit significant oscillations, accompanied by the generation of high-energy particles. The production of high-energy particles enhances the erosion of the apertures in the keeper and cathode, leading to a degradation in cathode performance and lifespan. For the cathode mode transition, several semi-empirical formulas based on measurements of discharge current and voltage oscillations have been proposed to assess the cathode mode transition. In this study, we utilized a criterion of the peak-to-peak values of the anode discharge voltage and the keeper floating voltage exceeding 5 volts to indicate the cathode mode transition into the plume mode. This criterion was employed to evaluate the performance of the cathode design. When the flow rate was below 5 sccm, significant voltage oscillations were observed in the discharge voltage, indicating the transition of the cathode into the plume mode. Discharge currents ranging from 4 amperes to 7 amperes were tested at a flow rate of 7 sccm. However, the peak-to-peak voltage oscillations remained below the defined threshold, indicating that the operation was still maintained in the spot mode. The cathode was tested under two different background pressure conditions ("8.1×" 〖"10" 〗^"-4" and "3×" 〖"10" 〗^"-4" torr) to assess the impact of background pressure on cathode performance. The results indicated that excessively high background pressure led to the disappearance of the mode transition, making it impossible to utilize the voltage oscillation criterion to determine the optimal operating flow rate and discharge current for the cathode. The application of axial magnetic field resulted in a decrease in anode discharge voltage. The speculate is that the magnetic field diminish the electron mobility to traverse fields, thereby increasing the effective surface area of anode.

    摘要 i ABSTRACT iii 誌謝 v CONTENTS vi LIST OF TABLES ix LIST OF FIGURES x NOMENCLATURE xiv CHAPTER1 Introduction 1 1.1 Electric propulsion 1 1.1.1 Electrothermal Thruster 2 1.1.2 Electromagnetic Thruster 5 1.1.3 Electrostatic Thruster 7 1.2 Propulsion Principle 11 1.2.1 Thrust 11 1.2.2 Specific Impulse 12 1.2.3 Thruster Efficiency 13 1.2.4 Thruster Performance Metrics 13 1.3 Hall Effect Thruster 15 1.3.1 Hall Effect Thruster Operation Principle 16 1.3.2 Type of Hall Effect Thruster 20 1.3.3 Cathode Coupling 23 1.4 Motivation and Objective 26 CHAPTER2 Literature Review 28 2.1 Hollow Cathode 28 2.1.1 Operation principle 28 2.1.2 Thermionic electron emitter 31 2.1.3 Low Current Hollow Cathode 34 2.1.4 High Current Hollow Cathode 36 2.2 Heaterless Hollow Cathode 37 2.2.1 Operation Principle 37 2.2.2 Breakdown Phase 38 2.2.3 Emitter Heating Stage 41 2.3 Cathode Stability 42 2.3.1 Plasma Oscillation in Hollow Cathode 42 2.3.2 Spot and Plume Mode 43 CHAPTER3 Experimental Setup and Cathode Design 48 3.1 Experimental Setup 48 3.1.1 Vacuum Chamber 48 3.1.2 Propellant Feeding System 51 3.1.3 Discharge Circuit 52 3.1.4 External Magnetic Field Generator 54 3.1.5 Measurement device 55 3.2 Cathode Design 55 3.2.1 Cathode Material 56 3.2.2 Cathode Geometry 58 3.2.3 Operation Pressure in the Cathode 59 CHAPTER4 Result and Discussion 61 4.1 Cathode Performance Test 61 4.1.1 Ignition Test 61 4.1.2 Test of flow rate variation 64 4.1.3 Test of Discharge Current Variation 69 4.2 Influence of Background Pressure 71 4.3 Influence of Magnetic Field 76 CHAPTER5 Conclusion and Future Work 84 5.1 Conclusion 84 5.2 Future Work 86 APPENDIX 87 REFERENCE 94

    [1] D. M. Goebel and I. Katz, Fundamentals of Electric Propulsion: Ion and Hall Thrusters (JPL Space Science and Technology Series).U.S.A, 2008.
    [2] D. O’Reilly, G. Herdrich, and D. F. Kavanagh, "Electric Propulsion Methods for Small Satellites: A Review," Aerospace, vol. 8, no. 1, 2021, doi: 10.3390/aerospace8010022.
    [3] A. R. Tummala and A. Dutta, "An Overview of Cube-Satellite Propulsion Technologies and Trends," Aerospace, vol. 4, no. 4, 2017, doi: 10.3390/aerospace4040058.
    [4] P. b. Inc. "<pale-blue_co.pdf>." (accessed.
    [5] H.-Y. Lee, "Indigenous Technology Development of a Prototype Arcjet System," Master, Department of Aeronautics and Astronautics, National Cheng Kung University, Taiwan, 2010.
    [6] J. Kolbeck, M. Keidar, and A. Anders, "Micropropulsion Based on Vacuum Arc Physics and Technology: A Review," presented at the 52nd AIAA/SAE/ASEE Joint Propulsion Conference, 2016.
    [7] Y.-H. Li, J.-Y. Pan, and G. Herdrich, "Design and demonstration of micro-scale vacuum cathode arc thruster with inductive energy storage circuit," Acta Astronautica, vol. 172, pp.33-46, 2020, doi:10.1016/j.actaastro.2020.03.012.
    [8] S.-W. LIU, "The Development of Vacuum Arc Cathode Induced Pulsed Plasma Thruster," International Master Degree Program on Energy Engineering, National Cheng Kung University, Taiwan, 2021.
    [9] M. Tsay, J. Frongillo, and J. Zwahlen, "Maturation of Iodine Fueled BIT-3 RF Ion Thruster and RF Neutralizer," presented at the 52nd AIAA/SAE/ASEE Joint Propulsion Conference, 2016.
    [10] M. Martinez-Sanchez and P. Lozano, "Session 10-11: Electrostatic Thrusters (Kaufman Ion Engines)," U.S.A, 2015.
    [11] D. Krejci and P. Lozano, "Space Propulsion Technology for Small Spacecraft," Proceedings of the IEEE, vol. 106, no. 3, pp. 362-378, 2018, doi:10.1109/jproc.2017.2778747.
    [12] S. Weston, "State-of-the-Art Small Spacecraft Technology," Small Spacecraft Systems Virtual Institute, U.S.A, NASA/TP—2022–0018058, 2022.
    [13] P. Lozano and M. Martinez-Sanchez, "Session 16: Hall Thrusters," U.S.A, 2015.
    [14] F. F. Chen, Introduction to Plasma Physics and Controlled Fusion. Los Angeles, CA, USA, 2015.
    [15] E. Y. Choueiri, "Fundamental Difference between the Two Variants of Hall Thrusters: SPT and TAL," presented at the AIAA, 2001, AIAA-2001-3504.
    [16] Y. Raitses, A. Smirnov, and N. Fisch, "Cylindrical Hall Thrusters," presented at the 37th AIAA Plasmadynamics and Lasers Conference, 2006.
    [17] R. R. Hofer, D. M. Goebel, I. G. Mikellides, and I. Katz, "Magnetic shielding of a laboratory Hall thruster. II. Experiments," Journal of Applied Physics, vol. 115, no. 4, 2014, doi: 10.1063/1.4862314.
    [18] I. G. Mikellides, I. Katz, R. R. Hofer, and D. M. Goebel, "Magnetic shielding of a laboratory Hall thruster. I. Theory and validation," Journal of Applied Physics, vol. 115, no. 4, 2014, doi: 10.1063/1.4862313.
    [19] R. R. Hofer, S. E. Cusson, R. B. Lobbia, and A. D. Gallimore, "The H9 Magnetically Shielded Hall Thruster," presented at the IEPC, 2017, IEPC-2017-232.
    [20] N. Z. Warner, "Theoretical and Experimental Investigation of Hall Thruster Miniaturization," DEGREE OF DOCTOR OF PHILOSOPHY, THE DEPARTMENT OF AERONAUTICS AND ASTRONAUTICS, Massachusetts Institute of Technology, U.S.A, 2007.
    [21] K. K. Jameson, D. M. Goebel, and R. R. Hofer, "Cathode Coupling in Hall Thrusters," presented at the IEPC, 2007, IEPC-2007-278.
    [22] M. S. McDonald and A. D. Gallimore, "Cathode Position and Orientation Effects on Cathode Coupling in a 6-kW Hall Thruster," presented at the IEPC, 2009, IEPC-2009-113.
    [23] J. D. Sommerville and L. B. King, "Effect of Cathode Position on Hall-Effect Thruster Performance and Cathode Coupling Voltage," presented at the AIAA/ASME/SAE/ASEE Joint Propulsion Conference, 2007, AIAA 2007-5174.
    [24] N. Turan, U. Kokal, and M. Celik, "EXPERIMENTAL INVESTIGATION OF THE EFFECTS OF CATHODE CURRENT ON HK40 HALL THRUSTER OPERATION," presented at the SPACE PROPULSION 2016, 2016, SP2016_ 3125333.
    [25] D. M. Goebel, G. Becatti, I. G. Mikellides, and A. Lopez Ortega, "Plasma hollow cathodes," Journal of Applied Physics, vol. 130, no. 5, 2021, doi: 10.1063/5.0051228.
    [26] D. M. Goebel and R. M. Watkins, "Compact lanthanum hexaboride hollow cathode," Rev Sci Instrum, vol. 81, no. 8, p. 083504, Aug 2010, doi: 10.1063/1.3474921.
    [27] J. Polk, D. Goebel, R. Watkins, K. Jameson, and L. Yoneshige, "Characterization of Hollow Cathode Performance and Thermal Behavior," 96 presented at the 42nd AIAA/ASME/SAE/ASEE Joint Propulsion Conference &amp; Exhibit, 2006.
    [28] D. R. Lev, I. G. Mikellides, D. Pedrini, D. M. Goebel, B. A. Jorns, and M. S. McDonald, "Recent progress in research and development of hollow cathodes for electric propulsion," Reviews of Modern Plasma Physics, vol. 3, no. 1, 2019, doi: 10.1007/s41614-019-0026-0.
    [29] D. M. Goebel and E. Chu, "High Current Lanthanum Hexaboride Hollow Cathodes for High Power Hall Thrusters," presented at the IEPC, 2011, IEPC2011 053.
    [30] G. Becatti, R. W. Conversano, and D. M. Goebel, "Demonstration of 25,000 ignitions on a proto-flight compact heaterless lanthanum hexaboride hollow cathode," Acta Astronautica, vol. 178, pp. 181-191, 2021, doi: 10.1016/j.actaastro.2020.09.013.
    [31] R. K. Ham, "AN EXPERIMENTAL INVESTIGATION OF HEATERLESS HOLLOW CATHODE IGNITION," Master of Science, Department of Mechanical Engineering, Colorado State University, 2020.
    [32] H. Eichhorn, K. H. Schoenbach, and T. Tessnow, "Paschen’s law for a hollow cathode discharge," Applied Physics Letters, vol. 63, no. 18, pp. 2481-2483, 1993, doi: 10.1063/1.110455.
    [33] A. Daykin-Iliopoulos, S. Gabriel, and I. Golosnoy, "Investigation of Heaterless Hollow Cathode Breakdown," presented at the IEPC, 2015, IEPC-2015-193.
    [34] Z.-X. Ning et al., "10000-Ignition-Cycle Investigation of a LaB6 Hollow Cathode for 3–5-Kilowatt Hall Thruster," Journal of Propulsion and Power, vol. 35, no. 1, pp. 87-93, 2019, doi: 10.2514/1.B37192.
    [35] A. Daykin-Iliopoulos, I. Golosnoy, and S. Gabriel, "Thermal Profile of a Lanthanum Hexaboride Heaterless Hollow Cathode," presented at the IEPC, 2017, IEPC-2017-291.
    [36] D. G. Fearn and S. Patterson, "The Hollow Cathode - A Versatile Component of Electric Thrusters," 3rd International Conference on Spacecraft Propulsion p. 587, 2000.
    [37] M. P. Georgin, "Ionization Instability of the Hollow Cathode Plume," degree of Doctor of Philosophy (Applied Physics), University of Michigan, 2020.
    [38] D. M. Goebel, K. K. Jameson, and I. Katz, "Potential fluctuations and energetic ion production in hollow cathode discharges," Phys. Plasmas, vol. 14, 2007, doi: 10.1063/1.2784460 兴.
    [39] I. G. Mikellides, A. Lopez Ortega, D. M. Goebel, and G. Becatti, "Dynamics of a hollow cathode discharge in the frequency range of 1–500 kHz," Plasma Sources Science and Technology, vol. 29, no. 3, 2020, doi: 10.1088/1361-976595/ab69e4.
    [40] G. C. Potrivitu, L. Xu, S. Huang, M. W. A. B. Rohaizat, and S. Xu, "Discharge mode transition in a Krypton-fed 1 A-class LaB6 cathode for low-power Hall thrusters for small satellites," Journal of Applied Physics, vol. 127, no. 6, 2020, doi: 10.1063/1.5142019.
    [41] G.-C. Potrivitu, R. Joussot, and S. Mazouffre, "Anode position influence on discharge modes of a LaB6 cathode in diode configuration," Vacuum, vol. 151, pp. 122-132, 2018, doi: 10.1016/j.vacuum.2018.02.010.
    [42] S. J. Hall and T. G. Gray, "The Effect of Anode Position on Operation of a 25-A class Hollow Cathode," presented at the IEPC, 2019, IEPC-2019-299.
    [43] U. Kokal, N. Turan, and M. Celik, "Thermal analysis and testing of different designs of lanthanum hexaboride hollow cathodes," presented at the 2017 8th International Conference on Recent Advances in Space Technologies (RAST), 2017.
    [44] M. N. Macrossan and C. R. Lilley, "Viscosity of argon at temperatures Ì2000 K from measured shock thickness," PHYSICS OF FLUIDS, vol. 15, 2003, doi: 10.1063/1.1616556 兴.
    [45] D. Lev and L. Appel, "Heaterless Hollow Cathode Technology - A Critical Review," presented at the SPACE PROPULSION 2016, MARRIOTT PARK HOTEL, ROME, ITALY, 2016, SP2016_3125366.
    [46] D. J. Asselin, "CHARACTERIZATION OF THE NEAR-PLUME REGIONOF A LOW-CURRENT HOLLOW CATHODE," Degree of Master of Science, Mechanical Engineering, WORCESTER POLYTECHNIC INSTITUTE, 2011.
    [47] S. J. Hall, T. G. Gray, and J. T. Yim, "The Effect of a Hall Thruster-like Magnetic Field on Operation of a 25-A class Hollow Cathode," presented at the 36th International Electric Propulsion Conference, University of Vienna • Vienna, Austria, 2019, IEPC-2019-300.
    [48] D. Imaguchi, H. Watanabe, and S. Imai, "Characterization of a Hollow Cathode Plasma with Magnetic Fields," presented at the AIAA Propulsion and Energy 2021 Forum, 2021.
    [49] G.-C. Potrivitu and S. Xu, "Ionization instability and turbulence in the plume of sub-ampere hollow cathodes depending on an applied magnetic field," CEAS Space Journal, 2022, doi: 10.1007/s12567-022-00478-5.
    [50] B. A. Jorns and R. R. Hofer, "Plasma oscillations in a 6-kW magnetically shielded Hall thruster," Physics of Plasmas, vol. 21, no. 5, 2014, doi: 10.1063/1.4879819

    無法下載圖示 校內:2027-12-31公開
    校外:2027-12-31公開
    電子論文尚未授權公開,紙本請查館藏目錄
    QR CODE