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Magnetized target fusion (MTF) is an alternative approach to fusion between traditional inertial confinement fusion and magnetic confinement fusion. It involves three processes: the formation of target plasma, the translation of target plasma, and compression process of implosion. In this paper, the translation process is studied with a two-dimensional magneto-hydrodynamic code MPF-2D, and the result shows that it is necessary to add a proper magnetic field in the translation process of field reversed configuration in order to maintain its topological structure. The effects of initial magnetic pressure, translation magnetic field, and the gap between coils are studied in detail.
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Keywords:
- magnetized target fusion /
- field reversed configuration /
- two-dimensional magneto-hydrodynamic
[1] Hurricane O A, Callahan D A, Casey D T, Celliers P M, Cerjan C, Dewald E L, Dittrich T R, Doppner T, Hinkel D E, Berzak Hopkins L F, Kline J L, Pape S L, Ma T, MacPhee A G, Milovich J L, Pak A, Park H S, Patel P K, Remington B A, Salmonson J D, Springer P T, Tommasini R 2014 Nature 506 343
[2] Zaripov M M, Khaybullin I B, Shtyrkov E I 1976 Sov. Phys. Usp. 19 1032
[3] Lindemuth I R, Kirkpatrick R C 1983 Nucl. Fusion 23 263
[4] Taccetti J M, Intrator T P, Wurden G A, Zhang S Y, Aragonez R, Assmus P N, Bass C M, Carey C, deVries S A, Fienup W J, Furno I, Hsu S C, Kozar M P, Langner M C, Liang J, Maqueda R J, Martinez R A, Sanchez P G, Schoenberg K F, Scott K J, Siemon R E, Tejero E M, Trask E H, Tuszewski M, Waganaar W J 2003 Rev. Sci. Instrum. 74 4314
[5] Intrator T P, Siemon R E, Sieck P E 2008 Phys. Plasmas 15 042505
[6] Green T S 1960 Phys. Rev. Lett. 5 297
[7] Wright J K, Phillips N J 1960 J. Nucl. Energy Part C 1 240
[8] Binderbauer M W, Guo H Y, Tuszewski M, et al. 2010 Phys. Rev. Lett. 105 045003
[9] Yamada M, Ono Y, Hayakawa A, Katsurai M 1990 Phys. Rev. Lett. 65 721
[10] Slough J T, Miller K E 2000 Phys. Rev. Lett. 85 1444
[11] Armstrong W T, Linford R K, Lipson J, Platts D A, Sherwood E G 1981 Phys. Fluids 24 2068
[12] Intrator T P, Park J Y, Degnan J H, Furno S I, Grabowski C, Hsu S C, Ruden E L, Sanchez P G, Taccetti J M, Tuszewski M, Waganaar W J, Wurden G A, Zhang S Y, Wang Z 2004 IEEE Trans. Plasma Sci. 33 152
[13] Sun Q Z, Fang D F, Liu W, Qin W D, Jia Y S, Zhao X M, Han W H 2013 Acta Phys. Sin. 62 078407 (in Chinese) [孙奇志, 方东凡, 刘伟, 秦卫东, 贾月松, 赵小明, 韩文辉 2013 物理学报 62 078407]
[14] Armstrong W T, Cochrane J C, Commisso R J, Lipson J, Tuszewski M 1981 Appl. Phys. Lett. 38 680
[15] Sgro A G, Armstrong W T, Lipson J, Tuszewski M G, Cochrane J C 1982 Phys. Rev. A 26 3564
[16] Soběhart J R 1990 Phys. Fluids B 2 2268
[17] Li L L, Zhang H, Yang X J 2014 Acta Phys. Sin. 63 165202 (in Chinese) [李璐璐, 张华, 杨显俊 2014 物理学报 63 165202]
[18] Kershaw D S 1981 J. Comput. Phys. 39 375
[19] Winslow A W 1963 Equipotential Zoning of Two-Dimensional Meshes (Livermore: Lawrence Livermore National Laboratory) UCRL-7312
[20] Winslow A W 1981 Adaptive Mesh Zoning by Equipotential Method (Livermore: Lawrence Livermore National Laboratory) UCID-19062
[21] Margolin L G, Shashkov M 2002 Second-Order Sign-Preserving Remapping on General Grids (Los Alamos: Los Alamos National Scientific Laboratory) LA-UR-02-525
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[1] Hurricane O A, Callahan D A, Casey D T, Celliers P M, Cerjan C, Dewald E L, Dittrich T R, Doppner T, Hinkel D E, Berzak Hopkins L F, Kline J L, Pape S L, Ma T, MacPhee A G, Milovich J L, Pak A, Park H S, Patel P K, Remington B A, Salmonson J D, Springer P T, Tommasini R 2014 Nature 506 343
[2] Zaripov M M, Khaybullin I B, Shtyrkov E I 1976 Sov. Phys. Usp. 19 1032
[3] Lindemuth I R, Kirkpatrick R C 1983 Nucl. Fusion 23 263
[4] Taccetti J M, Intrator T P, Wurden G A, Zhang S Y, Aragonez R, Assmus P N, Bass C M, Carey C, deVries S A, Fienup W J, Furno I, Hsu S C, Kozar M P, Langner M C, Liang J, Maqueda R J, Martinez R A, Sanchez P G, Schoenberg K F, Scott K J, Siemon R E, Tejero E M, Trask E H, Tuszewski M, Waganaar W J 2003 Rev. Sci. Instrum. 74 4314
[5] Intrator T P, Siemon R E, Sieck P E 2008 Phys. Plasmas 15 042505
[6] Green T S 1960 Phys. Rev. Lett. 5 297
[7] Wright J K, Phillips N J 1960 J. Nucl. Energy Part C 1 240
[8] Binderbauer M W, Guo H Y, Tuszewski M, et al. 2010 Phys. Rev. Lett. 105 045003
[9] Yamada M, Ono Y, Hayakawa A, Katsurai M 1990 Phys. Rev. Lett. 65 721
[10] Slough J T, Miller K E 2000 Phys. Rev. Lett. 85 1444
[11] Armstrong W T, Linford R K, Lipson J, Platts D A, Sherwood E G 1981 Phys. Fluids 24 2068
[12] Intrator T P, Park J Y, Degnan J H, Furno S I, Grabowski C, Hsu S C, Ruden E L, Sanchez P G, Taccetti J M, Tuszewski M, Waganaar W J, Wurden G A, Zhang S Y, Wang Z 2004 IEEE Trans. Plasma Sci. 33 152
[13] Sun Q Z, Fang D F, Liu W, Qin W D, Jia Y S, Zhao X M, Han W H 2013 Acta Phys. Sin. 62 078407 (in Chinese) [孙奇志, 方东凡, 刘伟, 秦卫东, 贾月松, 赵小明, 韩文辉 2013 物理学报 62 078407]
[14] Armstrong W T, Cochrane J C, Commisso R J, Lipson J, Tuszewski M 1981 Appl. Phys. Lett. 38 680
[15] Sgro A G, Armstrong W T, Lipson J, Tuszewski M G, Cochrane J C 1982 Phys. Rev. A 26 3564
[16] Soběhart J R 1990 Phys. Fluids B 2 2268
[17] Li L L, Zhang H, Yang X J 2014 Acta Phys. Sin. 63 165202 (in Chinese) [李璐璐, 张华, 杨显俊 2014 物理学报 63 165202]
[18] Kershaw D S 1981 J. Comput. Phys. 39 375
[19] Winslow A W 1963 Equipotential Zoning of Two-Dimensional Meshes (Livermore: Lawrence Livermore National Laboratory) UCRL-7312
[20] Winslow A W 1981 Adaptive Mesh Zoning by Equipotential Method (Livermore: Lawrence Livermore National Laboratory) UCID-19062
[21] Margolin L G, Shashkov M 2002 Second-Order Sign-Preserving Remapping on General Grids (Los Alamos: Los Alamos National Scientific Laboratory) LA-UR-02-525
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