Effect of aperture field distribution on the maximum radiated power at atmospheric pressure
The air breakdown in the high-power antenna near-field region limits the enhancement of the radiated power. A model coupling the field equivalent principle and the electron number density equation is presented to study the breakdown process in the near-field region of the circular aperture antenna a...
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Published in | Chinese physics B Vol. 26; no. 11; pp. 324 - 328 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
01.11.2017
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Online Access | Get full text |
ISSN | 1674-1056 2058-3834 |
DOI | 10.1088/1674-1056/26/11/115101 |
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Abstract | The air breakdown in the high-power antenna near-field region limits the enhancement of the radiated power. A model coupling the field equivalent principle and the electron number density equation is presented to study the breakdown process in the near-field region of the circular aperture antenna at atmospheric pressure. Simulation results show that, although the electric field in the near-field region is nonuniform, the electron diffusion has small influence on the breakdown process when the initial electron number density is uniform in space. The field magnitude distribution on the aperture plays an important role in the maximum radiated power above which the air breakdown occurs. The maximum radiated power also depends on the phase difference of the fields at the center and edge of the aperture, especially for the uniform field magnitude distribution. |
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AbstractList | The air breakdown in the high-power antenna near-field region limits the enhancement of the radiated power. A model coupling the field equivalent principle and the electron number density equation is presented to study the breakdown process in the near-field region of the circular aperture antenna at atmospheric pressure. Simulation results show that, although the electric field in the near-field region is nonuniform, the electron diffusion has small influence on the breakdown process when the initial electron number density is uniform in space. The field magnitude distribution on the aperture plays an important role in the maximum radiated power above which the air breakdown occurs. The maximum radiated power also depends on the phase difference of the fields at the center and edge of the aperture, especially for the uniform field magnitude distribution. |
Author | 赵朋程;郭立新 |
AuthorAffiliation | School of Physics and Optoelectronic Engineering, Xidian University, Xi' an 710071, China |
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Cites_doi | 10.1063/1.4736863 10.1109/TEMC.2011.2112366 10.1063/1.2403782 10.1063/1.4768220 10.1063/1.3462320 10.1103/PhysRevLett.104.015002 10.1109/TDEI.2016.006047 10.1103/PhysRevLett.100.035003 10.1109/27.84292 |
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Notes | Pengcheng Zhao, Lixin Guo(School of Physics and Optoelectronic Engineering, Xidian University, Xi' an 710071, China) field equivalent principle aperture antenna air breakdown maximum radiated power 11-5639/O4 The air breakdown in the high-power antenna near-field region limits the enhancement of the radiated power. A model coupling the field equivalent principle and the electron number density equation is presented to study the breakdown process in the near-field region of the circular aperture antenna at atmospheric pressure. Simulation results show that, although the electric field in the near-field region is nonuniform, the electron diffusion has small influence on the breakdown process when the initial electron number density is uniform in space. The field magnitude distribution on the aperture plays an important role in the maximum radiated power above which the air breakdown occurs. The maximum radiated power also depends on the phase difference of the fields at the center and edge of the aperture, especially for the uniform field magnitude distribution. |
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References | Zhao P (7) 2015; 24 13 14 Zhu G Q (12) 2011; 20 Zhao P (8) 2017; 26 1 2 3 4 5 Zhao P (10) 2015; 24 6 Stutzman W L (11) 1998 9 |
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SubjectTerms | 击穿过程 场分布 大气压 孔径 环形天线 电子数密度 空气击穿 辐射功率 |
Title | Effect of aperture field distribution on the maximum radiated power at atmospheric pressure |
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