Characteristics of pulsed plasma synthetic jet and its control effect on supersonic flow
The plasma synthetic jet is a novel flow control approach which is currently being studied. In this paper its characteristic and control effect on supersonic flow is investigated both experimentally and numerically. In the experiment, the formation of plasma synthetic jet and its propagation velocit...
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Published in | Chinese journal of aeronautics Vol. 28; no. 1; pp. 66 - 76 |
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Main Authors | , , , , , , |
Format | Journal Article |
Language | English |
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01.02.2015
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Abstract | The plasma synthetic jet is a novel flow control approach which is currently being studied. In this paper its characteristic and control effect on supersonic flow is investigated both experimentally and numerically. In the experiment, the formation of plasma synthetic jet and its propagation velocity in quiescent air are recorded and calculated with time resolved schlieren method. The jet velocity is up to 100 m/s and no remarkable difference has been found after changing discharge parameters. When applied in Mach 2 supersonic flow, an obvious shockwave can be observed. In the modeling of electrical heating, the arc domain is not defined as an initial condition with fixed temperature or pressure, but a source term with time-varying input power density, which is expected to better describe the influence of heating process. Velocity variation with different heating efficiencies is presented and discussed and a peak velocity of 850 m/s is achieved in still air with heating power density of 5.0 · 1012W/m3. For more details on the interaction between plasma synthetic jet and supersonic flow, the plasma synthetic jet induced shockwave and the disturbances in the boundary layer are numerically researched. All the results have demonstrated the control authority of plasma synthetic jet onto supersonic flow. |
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AbstractList | The plasma synthetic jet is a novel flow control approach which is currently being studied. In this paper its characteristic and control effect on supersonic flow is investigated both experimentally and numerically. In the experiment, the formation of plasma synthetic jet and its propagation velocity in quiescent air are recorded and calculated with time resolved schlieren method. The jet velocity is up to 100m/s and no remarkable difference has been found after changing discharge parameters. When applied in Mach 2 supersonic flow, an obvious shockwave can be observed. In the modeling of electrical heating, the arc domain is not defined as an initial condition with fixed temperature or pressure, but a source term with time-varying input power density, which is expected to better describe the influence of heating process. Velocity variation with different heating efficiencies is presented and discussed and a peak velocity of 850m/s is achieved in still air with heating power density of 5.0×1012W/m3. For more details on the interaction between plasma synthetic jet and supersonic flow, the plasma synthetic jet induced shockwave and the disturbances in the boundary layer are numerically researched. All the results have demonstrated the control authority of plasma synthetic jet onto supersonic flow. The plasma synthetic jet is a novel flow control approach which is currently being studied. In this paper its characteristic and control effect on supersonic flow is investigated both experimentally and numerically. In the experiment, the formation of plasma synthetic jet and its propagation velocity in quiescent air are recorded and calculated with time resolved schlieren method. The jet velocity is up to 100 m/s and no remarkable difference has been found after changing discharge parameters. When applied in Mach 2 supersonic flow, an obvious shockwave can be observed. In the modeling of electrical heating, the are domain is not defined as an initial condition with fixed temperature or pressure, but a source term with time-varying input power density, which is expected to better describe the influence of heating process. Velocity variation with different heating efficiencies is presented and discussed and a peak velocity of 850 m/s is achieved in still air with heating power density of 5.0 x 10 super(12) W/m super(3). For more details on the interaction between plasma synthetic jet and supersonic flow, the plasma synthetic jet induced shockwave and the disturbances in the boundary layer are numerically researched. All the results have demonstrated the control authority of plasma synthetic jet onto supersonic flow. The plasma synthetic jet is a novel flow control approach which is currently being studied. In this paper its characteristic and control effect on supersonic flow is investigated both experimentally and numerically. In the experiment, the formation of plasma synthetic jet and its propagation velocity in quiescent air are recorded and calculated with time resolved schlieren method. The jet velocity is up to 100 m/s and no remarkable difference has been found after changing discharge parameters. When applied in Mach 2 supersonic flow, an obvious shockwave can be observed. In the modeling of electrical heating, the arc domain is not defined as an initial condition with fixed temperature or pressure, but a source term with time-varying input power density, which is expected to better describe the influence of heating process. Velocity variation with different heating efficiencies is presented and discussed and a peak velocity of 850 m/s is achieved in still air with heating power density of 5.0 · 1012W/m3. For more details on the interaction between plasma synthetic jet and supersonic flow, the plasma synthetic jet induced shockwave and the disturbances in the boundary layer are numerically researched. All the results have demonstrated the control authority of plasma synthetic jet onto supersonic flow. |
Author | Jin Di Cui Wei Li Yinghong Li Fanyu Jia Min Sun Quan Zhang Bailing |
AuthorAffiliation | Science and Technology on Plasma Dynamics Laboratory, Air Force Engineering University, Xi'an 710038, China School of Aerospace Engineering, Tsinghua University, Beijing 100084, China |
Author_xml | – sequence: 1 givenname: Di surname: Jin fullname: Jin, Di email: james.8653@gmail.com organization: Science and Technology on Plasma Dynamics Laboratory, Air Force Engineering University, Xi’an 710038, China – sequence: 2 givenname: Wei surname: Cui fullname: Cui, Wei email: cw14@mails.tsinghua.edu.cn organization: School of Aerospace Engineering, Tsinghua University, Beijing 100084, China – sequence: 3 givenname: Yinghong surname: Li fullname: Li, Yinghong organization: Science and Technology on Plasma Dynamics Laboratory, Air Force Engineering University, Xi’an 710038, China – sequence: 4 givenname: Fanyu surname: Li fullname: Li, Fanyu organization: Science and Technology on Plasma Dynamics Laboratory, Air Force Engineering University, Xi’an 710038, China – sequence: 5 givenname: Min surname: Jia fullname: Jia, Min organization: Science and Technology on Plasma Dynamics Laboratory, Air Force Engineering University, Xi’an 710038, China – sequence: 6 givenname: Quan surname: Sun fullname: Sun, Quan organization: Science and Technology on Plasma Dynamics Laboratory, Air Force Engineering University, Xi’an 710038, China – sequence: 7 givenname: Bailing surname: Zhang fullname: Zhang, Bailing organization: Science and Technology on Plasma Dynamics Laboratory, Air Force Engineering University, Xi’an 710038, China |
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Keywords | Supersonic flow Shockwave Plasma aerodynamic actuation Synthetic jet Pulsed direct current (DC) discharge |
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Notes | supersonic heating shockwave authority actuator details currently pulsed numerically remarkable The plasma synthetic jet is a novel flow control approach which is currently being studied. In this paper its characteristic and control effect on supersonic flow is investigated both experimentally and numerically. In the experiment, the formation of plasma synthetic jet and its propagation velocity in quiescent air are recorded and calculated with time resolved schlieren method. The jet velocity is up to 100 m/s and no remarkable difference has been found after changing discharge parameters. When applied in Mach 2 supersonic flow, an obvious shockwave can be observed. In the modeling of electrical heating, the arc domain is not defined as an initial condition with fixed temperature or pressure, but a source term with time-varying input power density, which is expected to better describe the influence of heating process. Velocity variation with different heating efficiencies is presented and discussed and a peak velocity of 850 m/s is achieved in still air with heating power density of 5.0 · 1012W/m3. For more details on the interaction between plasma synthetic jet and supersonic flow, the plasma synthetic jet induced shockwave and the disturbances in the boundary layer are numerically researched. All the results have demonstrated the control authority of plasma synthetic jet onto supersonic flow. 11-1732/V ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
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SubjectTerms | Density Disturbances Electric power generation Heating Mathematical models Plasma aerodynamic actuation Pulsed direct current (DC) discharge Shock waves Shockwave Supersonic aircraft Supersonic flow Synthetic jet 传播速度 功率密度 合成射流 控制效果 数值研究 时间分辨 脉冲等离子体 超音速流动 |
Title | Characteristics of pulsed plasma synthetic jet and its control effect on supersonic flow |
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