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反场构形的传输过程

李璐璐 张华 杨显俊

反场构形的传输过程

李璐璐, 张华, 杨显俊
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导出引用
  • 介于惯性约束聚变与磁约束聚变之间的磁化靶聚变技术, 可能是一种实现纯聚变更低廉更有效的途径. 磁化靶聚变一般分为三个过程: 形成过程、传输过程和内爆压缩过程. 利用二维磁流体力学模拟程序MPF-2D, 对反场构形的传输过程进行了理论研究. 结果显示, 反场构形在传输过程中必须外加适当的磁场, 使得其内外磁压平衡, 才能维持其拓扑结构并进行稳定的传输. 还对初始磁压、传输磁场以及线圈间隙对反场构形传输过程的影响进行了详细的分析.
    • 基金项目: 国家自然科学基金(批准号:11105005,11175026,11175028)资助的课题.
    [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

  • [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

  • 引用本文:
    Citation:
计量
  • 文章访问数:  1453
  • PDF下载量:  137
  • 被引次数: 0
出版历程
  • 收稿日期:  2014-11-15
  • 修回日期:  2014-12-29
  • 刊出日期:  2015-06-05

反场构形的传输过程

  • 1. 北京应用物理与计算数学研究所, 北京 100094
    基金项目: 

    国家自然科学基金(批准号:11105005,11175026,11175028)资助的课题.

摘要: 介于惯性约束聚变与磁约束聚变之间的磁化靶聚变技术, 可能是一种实现纯聚变更低廉更有效的途径. 磁化靶聚变一般分为三个过程: 形成过程、传输过程和内爆压缩过程. 利用二维磁流体力学模拟程序MPF-2D, 对反场构形的传输过程进行了理论研究. 结果显示, 反场构形在传输过程中必须外加适当的磁场, 使得其内外磁压平衡, 才能维持其拓扑结构并进行稳定的传输. 还对初始磁压、传输磁场以及线圈间隙对反场构形传输过程的影响进行了详细的分析.

English Abstract

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