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纳秒脉冲等离子体气动激励数值仿真

李凡玉 李军 吴云 刘东健

李凡玉, 李军, 吴云, 刘东健. 纳秒脉冲等离子体气动激励数值仿真[J]. 航空动力学报, 2015, 30(3): 537-545. doi: 10.13224/j.cnki.jasp.2015.03.003
引用本文: 李凡玉, 李军, 吴云, 刘东健. 纳秒脉冲等离子体气动激励数值仿真[J]. 航空动力学报, 2015, 30(3): 537-545. doi: 10.13224/j.cnki.jasp.2015.03.003
LI Fan-yu, LI Jun, WU Yun, LIU Dong-jian. Numerical simulation of nanosecond pulse plasma aerodynamic actuation[J]. Journal of Aerospace Power, 2015, 30(3): 537-545. doi: 10.13224/j.cnki.jasp.2015.03.003
Citation: LI Fan-yu, LI Jun, WU Yun, LIU Dong-jian. Numerical simulation of nanosecond pulse plasma aerodynamic actuation[J]. Journal of Aerospace Power, 2015, 30(3): 537-545. doi: 10.13224/j.cnki.jasp.2015.03.003

纳秒脉冲等离子体气动激励数值仿真

doi: 10.13224/j.cnki.jasp.2015.03.003
基金项目: 

国家自然科学基金(51276197,51336011)

详细信息
    作者简介:

    李凡玉(1988-),男,山东济宁人,博士生,主要从事等离子体改善动力效能技术研究.

  • 中图分类号: V211

Numerical simulation of nanosecond pulse plasma aerodynamic actuation

  • 摘要: 从纳秒脉冲等离子体气动激励对流场的作用机理出发,将其对流场的作用等效为热源对流场的快速加热,建立了纳秒脉冲等离子体气动激励的空气动力学模型.应用模型计算了单次纳秒脉冲等离子体气动激励下静止流场的响应,计算结果表明:纳秒脉冲等离子体气动激励可在静止流场中形成一个高温升压升区(716K,225.95kPa)和一个低温升压升区(380K,131.7kPa),分别可诱导一强一弱两道压缩波,压缩波后各有一道稀疏波.压缩波与稀疏波同速向外传播,传播速度开始较大(大于400m/s),随着逐渐向外传播,其传播速度逐渐减小(357m/s).压缩波经过的区域可诱导局部速度,初期诱导的局部速度较大,在激励器切向和法向可诱导60m/s以上的局部速度,随着压缩波的衰减,诱导局部速度的能力减弱,最大可诱导10m/s左右的局部速度.

     

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出版历程
  • 收稿日期:  2013-11-06
  • 刊出日期:  2015-03-28

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