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The primary electro-mechanical model is developed for the acceleration kinetics of electromagnetic railguns. Pulsed plasma thrusters (PPTs), whose operation principle is similar to that of electromagnetic railguns, generate thrust via electromagnetic acceleration of plasma. Therefore, the electro-mechanical model serves as a valuable analytical tool to explore the mechanisms of energy conversion and thrust generation of PPTs. In fact, a PPT initiates discharge at its propellant surface and then ejects the discharged channel away to form accelerated plume. During the acceleration, the plasma channel assumes a curved shape, which is different from the flat sheet shape. The curved geometric shape of PPT discharge channel makes the flat current sheet model currently used in the electro-mechanical models inherently flawed. In this paper, a two-dimensional (2D) curved current sheet model is proposed to improve the PPT electro-mechanical model, by referring to the curved morphology of PPT discharge plasma channels. No matter what is the real geometry of the 2D current sheet, the Ampere force on discharge plasma channels and corresponding kinetics can be derived to obtain final kinetic energy of discharge plasma channels. As a result, the relation between the kinetic energy and the inductance of PPT discharge circuit is obtained and expressed as $ {E}_{{\mathrm{k}}}=\displaystyle\int _{0}^{{t}_{{\mathrm{e}}{\mathrm{n}}{\mathrm{d}}}}{i\left(t\right)}^{2}\frac{{\mathrm{d}}{L}_{{\mathrm{e}}{\mathrm{q}}}\left(t\right)}{{\mathrm{d}}t}{\mathrm{d}}t $. To determine the inductance as a temporal function, an algorithm for the inductance is proposed in which time-segment fitting of PPT discharge waveforms is adopted. Moreover, based on the temporal function of the inductance, PPT discharge waveforms can be simulated by using the ODE45 solver of MATLAB with high fitting goodness. So far, a calculation scheme for the kinetic energy of PPT plumes and simulation code for PPT discharge waveforms have set up based on the improved electro-mechanical model. To verify the improved model and the corresponding calculation scheme, the PPT prototype is used to evaluate its energy conversion efficiency. The results show that the model enables elucidating the low PPT electro-mechanical efficiency, which is attributed to the partition limitation of PPT energy to electromagnetic acceleration process. Accordingly, a possible exploration routine for elevating PPT electro-mechanical efficiency is suggested.
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Keywords:
- pulsed plasma thruster /
- improved electro-mechanical model /
- electro-mechanical efficiency /
- plume kinetic energy
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[7] Koizumi H, Noji R, Komurasaki K, Arakawa Y 2007 Phys. Plasmas 14 033506
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[9] Antropov N, Diakonov G, Orlov M, Popov G, Yakovlev V 2003 28th International Electric Propulsion Conference Paper Toulouse, March 17–21 2003 p3
[10] Schönherr T, Nawaz A, Herdrich G, Röser H P, Auweter-Kurtz M 2009 J. Propul. Power 25 380
Google Scholar
[11] Palumbo D J, Guman W J 1976 J. Spacecraft Rockets 13 163
Google Scholar
[12] Ling W Y L, Zhang S, Fu H, Huang M C, Quansah J, Liu X Y, Wang N F 2020 Chin. J. Aeronaut. 33 2999
Google Scholar
[13] Ou Y, Wu J J, Du X R, Zhang H, He Z F 2019 Vacuum 165 163
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[14] Spanjers G G, Lotspeich J S, McFall K A, Spores R A 1998 J. Propul. Power 14 554
Google Scholar
[15] Schönherr T, Komurasaki K, Herdrich G 2013 J. Propul. Power 29 1478
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Google Scholar
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Google Scholar
[19] Jahn R G 1968 Physics of Electric Propulsion (New York: McGraw-Hill) p263
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Google Scholar
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Google Scholar
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[34] Yang L, Liu X Y, Wu Z W, Wang N F 2011 47th AIAA/ASME/SAE/ASEE Joint Propulsion Conference & Exhibit California, USA, July 31–August 3, 2011 p6077
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Google Scholar
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图 1 基本PPT机-电模型等效电路示意图
Figure 1. Equivalent circuit schematic of primary PPT electromechanical model.
图 2 二维薄电流片及机-电模型电路示意图
Figure 2. Circuit schematic of the improved electromechanical model with 2D thin current sheet.
图 3 PPT实验装置示意图
Figure 3. Schematic of PPT experimental setup.
图 4 典型PPT放电电流波形及其数值滤波、对比拟合效果 (a) 原始电流波形及滤波效果; (b) 电流波形的不同拟合效果对比
Figure 4. A typical current waveform and its numerical filtering and fitting: (a) Measured and filtered waveforms; (b) current waveform fittings with different scheme.
图 5 PPT波形的分段拟合区间划分及仿真效果 (a) 分段拟合区间的划分示意图; (b) 波形的分段拟合效果; (c) 波形的仿真效果
Figure 5. Segmentation and the simulation outcome of PPT waveform: (a) Fitting segments; (b) segmental fitted waveform; (c) simulated waveform.
图 6 PPT放电回路的时变特性 (a) 6次PPT回路电感数据; (b) 6次PPT回路电阻数据; (c) 电感二次式拟合效果; (d) 电阻二次式拟合效果
Figure 6. Temporal variance of PPT circuit inductance during discharge: (a) Inductive data for 6 PPT discharges; (b) resistance data for 6 PPT discharges; (c) inductive fitting with a quadratic function; (d) resistance fitting with a quadratic function.
图 7 基于改进PPT机-电模型计算的电磁加速动能
Figure 7. Electromagnetic kinetic energy calculated with the improved PPT electromechanical model.
图 8 PPT机-电效率随工况参数的变化
Figure 8. Electromechanical efficiency with operation conditions of PPT.
图 9 PPT放电电压、电流、瞬时功率和能量沉积的典型波形($ {E}_{{\mathrm{q}}} $, 快沉积能量; $ {E}_{{\mathrm{s}}} $, 慢沉积能量)
Figure 9. Typical waveforms of PPT discharge voltage, current, power and energy deposition ($ {E}_{{\mathrm{q}}} $, quick deposition energy; $ {E}_{{\mathrm{s}}} $, slow deposition energy).
图 10 不同工况PPT放电的能量注入分配 (a)快沉积能量与慢沉积能量; (b)慢沉积能量占比
Figure 10. Energy deposition for PPT discharges with different operation conditions: (a) Quick ($ {E}_{{\mathrm{q}}}) $ and slow ($ {E}_{{\mathrm{s}}}) $deposition energy; (b) ratio of slow deposition energy.
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[1] Wu Z W, Huang T K, Liu X Y, Ling W Y L, Wang N F, Ji L C 2020 Plasma Sci. Technol. 22 094014
Google Scholar
[2] Northway P 2020 Ph. D. Dissertation (Washington: University of Washington
[3] Lev D, Myers R M, Lemmer K M, Kolbeck J, Koizumi H, Polzin K 2019 Acta Astronaut. 159 213
Google Scholar
[4] 吴建军, 胡泽君, 张宇, 何志成, 欧阳, 郑鹏, 赵元政, 李宇奇 2023 推进技术 44 11
Google Scholar
Wu J J, Hu Z J, Zhang Y, He Z C, Ou Y, Zheng P, Zhao Y Z, Li Y Q 2023 J. Propul. Technol. 44 11
Google Scholar
[5] Molina-Cabrera P, Herdrich G, Lau M, Fausolas S, Schönherr T, Komurasaki K 2011 the 32nd International Electric Propulsion Conference Wiesbaden, September 11–15, 2011 p1
[6] Spanjers G, McFall K, Gulczinski F, Spores R 1996 32nd AIAA/ASME/SAE/ASEE Joint Propulsion Conference and Exhibit Lake Buena Vista, July 1–3, 1996 p2723
[7] Koizumi H, Noji R, Komurasaki K, Arakawa Y 2007 Phys. Plasmas 14 033506
Google Scholar
[8] Gomez E W, Saravia M M, Castelló W B, Elaskar S 2022 8th International Conference on Space Propulsion ESTORIL, May 9–13, 2022 p00203
[9] Antropov N, Diakonov G, Orlov M, Popov G, Yakovlev V 2003 28th International Electric Propulsion Conference Paper Toulouse, March 17–21 2003 p3
[10] Schönherr T, Nawaz A, Herdrich G, Röser H P, Auweter-Kurtz M 2009 J. Propul. Power 25 380
Google Scholar
[11] Palumbo D J, Guman W J 1976 J. Spacecraft Rockets 13 163
Google Scholar
[12] Ling W Y L, Zhang S, Fu H, Huang M C, Quansah J, Liu X Y, Wang N F 2020 Chin. J. Aeronaut. 33 2999
Google Scholar
[13] Ou Y, Wu J J, Du X R, Zhang H, He Z F 2019 Vacuum 165 163
Google Scholar
[14] Spanjers G G, Lotspeich J S, McFall K A, Spores R A 1998 J. Propul. Power 14 554
Google Scholar
[15] Schönherr T, Komurasaki K, Herdrich G 2013 J. Propul. Power 29 1478
Google Scholar
[16] Zeng L H, Wu Z W, Sun G R, Huang T K, Xie K, Wang N F 2019 Acta Astronaut. 160 317
Google Scholar
[17] Nawaz A, Albertoni R, Auweter-Kurtz M 2010 Acta Astronaut. 67 440
Google Scholar
[18] Wu Z W, Sun G R, Huang T K, Liu X, Xie K, Wang N F 2018 AIAA J. 56 3024
Google Scholar
[19] Jahn R G 1968 Physics of Electric Propulsion (New York: McGraw-Hill) p263
[20] Turchi P, Mikellides P 1995 31st AIAA/ASME/SAE/ASEE Joint Propulsion Conference and Exhibit San Diego, July 10–12, 1995 p1
[21] Gatsonis N A, Hastings D E 1992 J. Geophys. Res.-Space 97 14989
Google Scholar
[22] Vondra R J, Thomassen K, Solbes A 1970 J. Spacecraft Rockets 7 1402
Google Scholar
[23] 魏荣华 1982 空间科学学报 2 319
Google Scholar
Wei R H 1982 Chin. J. Space Sci. 2 319
Google Scholar
[24] Laperriere D, Gatsonis N, Demetriou M 2005 41st AIAA/ASME/SAE/ASEE Joint Propulsion Conference and Exhibit Tucson, July 10–13, 2005 p4077
[25] Gatsonis N, Demetriou M 2004 40st AIAA/ASME/SAE/ASEE Joint Propulsion Conference and Exhibit Florida, July 11–14, 2004 p3464
[26] Laperriere D D 2005 M. S. Thesis (Massachusetts: Worcester Polytechnic Institute
[27] Ou Y, Wu J J, Zhang Y, Li J, Tan S 2018 Energies 11 1146
Google Scholar
[28] 张华, 吴建军, 张代贤, 张锐, 何振 2013 物理学报 62 210202
Google Scholar
Zhang H, Wu J J, Zhang D X, Zhang R, He Z 2013 Acta Phys. Sin. 62 210202
Google Scholar
[29] Mikellides Y G 1999 Theoretical Modeling and Optimization of Ablation-fed Pulsed Plasma Thrusters (The Ohio State University
[30] Mikellides P G, Henrikson E M, Rajagopalan S S 2019 J. Propul. Power 35 811
Google Scholar
[31] Keidar M, Boyd I D, Beilis I I 2003 J. Propul. Power 19 424
Google Scholar
[32] Keidar M, Boyd I 2002 38st AIAA/ASME/SAE/ASEE Joint Propulsion Conference and Exhibit Indianapolis, July 7–10, 2002 p4275
[33] Yang L, Huang Y, Tang H, Liu X 2015 34th International Electric Propulsion Conference and 6th Nano-satellite Symposium Hyogo-Kobe, July 4–10, 2015 p1
[34] Yang L, Liu X Y, Wu Z W, Wang N F 2011 47th AIAA/ASME/SAE/ASEE Joint Propulsion Conference & Exhibit California, USA, July 31–August 3, 2011 p6077
[35] Riazantsev A, Jakubczak M, Kurzyna J 2024 38th International Electric Propulsion Conference Toulouse, June 23–28, 2024 p1
[36] Schönherr T, Nawaz A, Lau M, Petkow D, Herdrich G 2010 Trans. JSASS Aerospace Tech. Japan 8 Tb_11
Google Scholar
[37] 王亚楠, 任林渊, 丁卫东, 孙安邦, 耿金越 2021 物理学报 70 235204
Google Scholar
Wang Y N, Ren L Y, Ding W D, Sun A B, Geng J Y 2021 Acta Phys. Sin. 70 235204
Google Scholar
[38] 王尚民, 田立成, 张家良, 张天平, 冯玮玮, 陈新伟, 高军 2017 中国空间科学技术 37 24
Google Scholar
Wang S M, Tian L C, Zhang J L, Zhang T P, Feng W W, Chen W X, Gao J 2017 Chin. Space Sci. Technol. 37 24
Google Scholar
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