基于Fokker-Planck-Landau碰撞模型的非均匀尘埃等离子体目标散射特性

陈伟; 黄海; 杨利霞; 薄勇; 黄志祥

doi:10.7498/aps.72.20222113

摘要

从玻尔兹曼方程出发, 推导了全电离非均匀尘埃等离子体的Fokker-Planck-Landau碰撞模型下时域有限差分的迭代表达式. 结合尘埃等离子体的碰撞效应和充电效应, 得到了Fokker-Planck-Landau碰撞模型下全电离尘埃等离子体的电导率表达式. 利用Z变换时域有限差分(Z-FDTD)法计算了二维情况下尘埃等离子体涂覆金属钝头锥的雷达散射截面. 分析了尘埃粒子密度、尘埃粒子半径、电子密度与尘埃粒子密度比值、尘埃粒子充电频率以及电磁波的入射角对钝头锥散射特性的影响. 结果表明, 在全电离空间非均匀尘埃等离子体中, 随着尘埃粒子半径的增大会削弱德拜屏蔽效应, 导致雷达散射截面增大; 此外, 受到尘埃等离子体的碰撞效应和充电效应产生影响, 会对目标的雷达散射截面有较大的影响. 这些结果对研究空间非均匀尘埃等离子体的电磁波散射特性以及近地空间的通信问题提供了理论依据.

关键词:

Abstract

Dusty plasma is a multi-particle system of dust particles suspended in plasma, which is generally composed of free electrons, ions, and dust particles. It is widely found in natural space and aerospace equipment, such as the Earth’s ionosphere, rocket tail flame, and sheath of the hypersonic vehicle. The dust particles will interact with free electrons and ions in the plasma so that the dust particles are charged. They also significantly change the characteristics of dusty plasma, showing some phenomena different from those in ordinary plasma, such as dust acoustic solitary waves and dust void. Electromagnetic (EM) waves will interact with dusty plasma, which results in the attenuation of EM wave signal and the change of phase and other serious effects, and the phenomenon of “blackout” appears. This is very unfavorable for the guidance and control system of the vehicle. The generation of “blackout” is related to the dynamics of dusty plasma and the analysis and research of EM characteristics, so studying the scattering characteristics of dusty plasma is of great significance. First, starting from the Boltzmann equation, the iterative expression of finite-difference time-domain under the Fokker-Planck-Landau (FPL) collision model of fully ionized non-uniform dusty plasma is derived. The expression of the conductivity of the fully ionized dusty plasma under the FPL collision model is obtained by combining the collision effect and charging effect of the dusty plasma. By using the Z-transform finite-difference time-domain method, the radar cross section (RCS) of the dusty plasma coated metal blunt cone in two dimensions is calculated. The effects of dust particle density, dust particle radius, ratio of electron density to dust particle density, dust particle charging frequency, and EM wave incident angle on the scattering characteristics of the mental blunt cone are analyzed. The results show that the Debye shielding effect is weakened and RCS is increased with the increase of the radius of dust particles in the fully ionized non-uniform dusty plasma. In addition, it is affected by the collision effect and charging effect of dusty plasma, which will have a great influence on the RCS of the target. These results provide a theoretical basis for studying the EM waves scattering problem of fully ionized non-uniform dusty plasma and the communication problems in near space.

Keywords:

Boltzmann equation /
dusty plasma /
Z-transform finite-difference time-domain method /
radar cross section

作者及机构信息

1.
安徽大学电子信息工程学院, 合肥　230601

2.
先进激光技术安徽省实验室, 合肥　230037

通信作者: 杨利霞, lixiayang@yeah.net

基金项目: 国家自然科学基金 (批准号: U21A20457, 61901004, 61871457, 62071003, 62071353)、先进激光技术安徽省实验室 (批准号: AHL2021KF04)、目标探测与特征提取安徽省重点实验室 (批准号: TRFE2021A001)和安徽省高校协同创新项目(批准号: GXXT-2020-050, GXXT-2021-028)资助的课题.

Authors and contacts

1.
School of Electronic and Information Engineering, Anhui University, Hefei 230601, China

2.
Advanced Laser Technology Laboratory of Anhui Province, Hefei 230037, China

Corresponding author: Yang Li-Xia, lixiayang@yeah.net

Funds: Project supported by the National Natural Science Foundation of China (Grant Nos. U21A20457, 61901004, 61871457, 62071003, 62071353), the Open Research Fund of Advanced Laser Technology Laboratory of Anhui Province, China (Grant No. AHL2021KF04), the Open Research Fund of Anhui Province Key Laboratory of Target Recognition and Feature Extraction, China (Grant No. TRFE2021A001), and the University Synergy Innovation of Program of Anhui Province, China (Grant Nos. GXXT-2020-050, GXXT-2021-028).

文章全文 : translate this paragraph

参考文献

[1]	孙俊国, 张宗国, 董焕河, 杨红卫 2019 物理学报 68 210201 Google Scholar Sun J G, Zhang Z G, Dong H H, Yang H W 2019 Acta Phys. Sin. 68 210201 Google Scholar
[2]	Wang Z Y, Guo L X, Li J T 2021 Chin. Phys. B 30 045203 Google Scholar
[3]	Yan J, Feng F, Liu F C, Dong L F, He Y F 2016 Chin. Phys. B 25 095202 Google Scholar
[4]	林麦麦, 付颖捷, 宋秋影, 于腾萱, 文惠珊, 蒋蕾 2022 物理学报 71 095203 Google Scholar Lin M M, Fu Y J, Song Q Y, Yu T X, Wen H S, Jiang L 2022 Acta Phys. Sin. 71 095203 Google Scholar
[5]	黄峰, 叶茂福, 王龙 2004 科学通报 49 2150 Google Scholar Huang F, Ye M F, Wang L 2004 Chin. Sci. Bull. 49 2150 Google Scholar
[6]	崔平远, 窦强, 高艾 2014 宇航学报 35 1 Google Scholar Cui P Y, Dou Q, Gao A 2014 J. Astr. 35 1 Google Scholar
[7]	Tsytovich V N 2015 Contrib. Plasma Phys. 55 664 Google Scholar
[8]	Sotnikov V I, Leboeuf J N, Mudaliar S 2010 IEEE Trans. Plasma Sci. 38 2208 Google Scholar
[9]	Motie I, Bokaeeyan M 2015 Phys. Plasmas 22 023707 Google Scholar
[10]	金铭, 韦笑, 吴洋, 张羽淮, 余西龙 2015 物理学报 64 205205 Google Scholar Jin M, Wei X, Wu Y, Zhang Y H, Yu X L 2015 Acta Phys. Sin. 64 205205 Google Scholar
[11]	Guo L X, Chen W, LI J T, Ren Y, Liu S H 2018 Phys. Plasmas 25 053707 Google Scholar
[12]	Dan L, Guo L X, Li J T 2018 Phys. Plasmas 25 013707 Google Scholar
[13]	Dan L, Gou L X, Li J T, Chen W, Yan X, Huang Q Q 2017 Phys. Plasmas 24 093703 Google Scholar
[14]	Mousseau V A, Knoll D A 1997 J. Comput. Phys. 136 308 Google Scholar
[15]	Li H, Wu J, Zhou Z, Yuan C 2016 Phys. Plasmas 23 073702 Google Scholar
[16]	Bendib A, Bendib-Kalache K, Cros B, Maynard G 2016 Phys. Rev. E 93 043208 Google Scholar
[17]	Bendib A, Bendib K, Sid A 1997 Phys. Rev. E 55 7522 Google Scholar
[18]	Jia J S, Yuan C X, Liu S, Yue F, Gao R L, Wang Y, Zhou Z X, Wu J, Li H 2016 Phys. Plasmas 23 043302 Google Scholar
[19]	葛德彪, 闫玉波 2011 电磁波时域有限差分方法 (第三版) (西安: 西安电子科技大学出版社) 第259页 Ge D B, Yan Y B 2011 Finite-Difference Time-Domain Method for Electromagnetic Waves (3rd Ed.) (Xi’an: Xidian University Press) p259 (in Chinese)
[20]	魏兵, 葛德彪, 王飞 2008 物理学报 57 6290 Google Scholar Wei B, Ge D B, Wang F 2008 Acta Phys. Sin. 57 6290 Google Scholar
[21]	Ren Y, Guo L X, Chen W, Liu S H 2018 Phys. Plasmas 25 093515 Google Scholar
[22]	王飞, 魏兵 2013 物理学报 62 084106 Google Scholar Wang F, Wei B 2013 Acta Phys. Sin. 62 084106 Google Scholar
[23]	Demarest K, Huang Z B, Plumb R 1996 IEEE Trans. Antennas Propag. 44 1150 Google Scholar
[24]	Britt C L 1989 IEEE Trans. Antennas Propag. 37 1181 Google Scholar
[25]	Zhang H F, Li J T, Bian Z, Guo L X 2022 IEEE Trans. Plasma Sci. 50 3200 Google Scholar
[26]	Liu S H, Zhu C K, Guo L X, Li J T, Dan L, Wang Z Y 2020 Phys. Plasmas 27 023701 Google Scholar

施引文献

图 1 RAM-C钝头锥飞行器模型图

Fig. 1. Model of RAM-C blunt cone vehicle.

下载: 全尺寸图片幻灯片

图 2 空间中电子密度分布

Fig. 2. Electron density distribution in space.

下载: 全尺寸图片幻灯片

图 3 未涂覆等离子体、等离子体涂覆以及尘埃等离子体涂覆的RCS

Fig. 3. RCS for without the plasma, coated with the plasma, and coated with the dusty plasma.

下载: 全尺寸图片幻灯片

图 4 不同尘埃粒子密度下的RCS

Fig. 4. RCS at different dust particle densities.

下载: 全尺寸图片幻灯片

图 5 不同尘埃粒子半径下的RCS

Fig. 5. RCS at different dust particle radii.

下载: 全尺寸图片幻灯片

图 6 不同电子密度与尘埃粒子密度比值下的RCS

Fig. 6. RCS at different ratios of electron density to dust particle density.

下载: 全尺寸图片幻灯片

图 7 不同充电频率的RCS

Fig. 7. RCS at different charging frequencies.

下载: 全尺寸图片幻灯片

图 8 不同电磁波入射角度下的RCS

Fig. 8. RCS at different incidence angles of EM waves.

下载: 全尺寸图片幻灯片

表 1 等离子体与尘埃等离子体相关参数

Table 1. Related parameters of plasma and dusty plasma.

参数等离子体尘埃等离子体

$n_{\text{d}}/(10^{12}~\text{m}^{-3})$ 0 1
$r_{\text{d}} /{\text{μ}{\rm m}}$ 0 5
$T_{\rm e}/(10^{4}~\text{K})$ 1 1
${\varphi /{\left( {^\circ } \right)} }$ 0 0

下载: 导出CSV

表 2 全电离尘埃等离子体的计算参数

Table 2. Calculated parameters of fully ionized dusty plasma.

n_d/(10¹² m^–3) r_d/μm n_e·n_d^–1/10⁴ v_ch/(10⁹ rad·s^–1)

图4 1, 2, 3 5 10 5
图5 1 3, 4, 5 10 5
图6 1 5 5.0, 7.5, 10.0 5
图7 1 5 10 5, 10, 15

下载: 导出CSV

[1]	孙俊国, 张宗国, 董焕河, 杨红卫 2019 物理学报 68 210201 Google Scholar Sun J G, Zhang Z G, Dong H H, Yang H W 2019 Acta Phys. Sin. 68 210201 Google Scholar
[2]	Wang Z Y, Guo L X, Li J T 2021 Chin. Phys. B 30 045203 Google Scholar
[3]	Yan J, Feng F, Liu F C, Dong L F, He Y F 2016 Chin. Phys. B 25 095202 Google Scholar
[4]	林麦麦, 付颖捷, 宋秋影, 于腾萱, 文惠珊, 蒋蕾 2022 物理学报 71 095203 Google Scholar Lin M M, Fu Y J, Song Q Y, Yu T X, Wen H S, Jiang L 2022 Acta Phys. Sin. 71 095203 Google Scholar
[5]	黄峰, 叶茂福, 王龙 2004 科学通报 49 2150 Google Scholar Huang F, Ye M F, Wang L 2004 Chin. Sci. Bull. 49 2150 Google Scholar
[6]	崔平远, 窦强, 高艾 2014 宇航学报 35 1 Google Scholar Cui P Y, Dou Q, Gao A 2014 J. Astr. 35 1 Google Scholar
[7]	Tsytovich V N 2015 Contrib. Plasma Phys. 55 664 Google Scholar
[8]	Sotnikov V I, Leboeuf J N, Mudaliar S 2010 IEEE Trans. Plasma Sci. 38 2208 Google Scholar
[9]	Motie I, Bokaeeyan M 2015 Phys. Plasmas 22 023707 Google Scholar
[10]	金铭, 韦笑, 吴洋, 张羽淮, 余西龙 2015 物理学报 64 205205 Google Scholar Jin M, Wei X, Wu Y, Zhang Y H, Yu X L 2015 Acta Phys. Sin. 64 205205 Google Scholar
[11]	Guo L X, Chen W, LI J T, Ren Y, Liu S H 2018 Phys. Plasmas 25 053707 Google Scholar
[12]	Dan L, Guo L X, Li J T 2018 Phys. Plasmas 25 013707 Google Scholar
[13]	Dan L, Gou L X, Li J T, Chen W, Yan X, Huang Q Q 2017 Phys. Plasmas 24 093703 Google Scholar
[14]	Mousseau V A, Knoll D A 1997 J. Comput. Phys. 136 308 Google Scholar
[15]	Li H, Wu J, Zhou Z, Yuan C 2016 Phys. Plasmas 23 073702 Google Scholar
[16]	Bendib A, Bendib-Kalache K, Cros B, Maynard G 2016 Phys. Rev. E 93 043208 Google Scholar
[17]	Bendib A, Bendib K, Sid A 1997 Phys. Rev. E 55 7522 Google Scholar
[18]	Jia J S, Yuan C X, Liu S, Yue F, Gao R L, Wang Y, Zhou Z X, Wu J, Li H 2016 Phys. Plasmas 23 043302 Google Scholar
[19]	葛德彪, 闫玉波 2011 电磁波时域有限差分方法 (第三版) (西安: 西安电子科技大学出版社) 第259页 Ge D B, Yan Y B 2011 Finite-Difference Time-Domain Method for Electromagnetic Waves (3rd Ed.) (Xi’an: Xidian University Press) p259 (in Chinese)
[20]	魏兵, 葛德彪, 王飞 2008 物理学报 57 6290 Google Scholar Wei B, Ge D B, Wang F 2008 Acta Phys. Sin. 57 6290 Google Scholar
[21]	Ren Y, Guo L X, Chen W, Liu S H 2018 Phys. Plasmas 25 093515 Google Scholar
[22]	王飞, 魏兵 2013 物理学报 62 084106 Google Scholar Wang F, Wei B 2013 Acta Phys. Sin. 62 084106 Google Scholar
[23]	Demarest K, Huang Z B, Plumb R 1996 IEEE Trans. Antennas Propag. 44 1150 Google Scholar
[24]	Britt C L 1989 IEEE Trans. Antennas Propag. 37 1181 Google Scholar
[25]	Zhang H F, Li J T, Bian Z, Guo L X 2022 IEEE Trans. Plasma Sci. 50 3200 Google Scholar
[26]	Liu S H, Zhu C K, Guo L X, Li J T, Dan L, Wang Z Y 2020 Phys. Plasmas 27 023701 Google Scholar

[1]	杨建荣, 毛杰键, 吴奇成, 刘萍, 黄立. 强碰撞磁化尘埃等离子体中的漂移波. 物理学报, 2020, 69(17): 175201. doi: 10.7498/aps.69.20200468
[2]	孙俊超, 张宗国, 董焕河, 杨红卫. 尘埃等离子体中的分数阶模型及其Lump解. 物理学报, 2019, 68(21): 210201. doi: 10.7498/aps.68.20191045
[3]	张旭涛, 阙肖峰, 蔡禾, 孙金海, 张景, 李粮生, 刘永强. 太赫兹雷达散射截面的仿真与时域光谱测量. 物理学报, 2019, 68(16): 168701. doi: 10.7498/aps.68.20190552
[4]	徐彬, 李辉, 王占阁, 许正文, 吴健. 高密度尘埃等离子体的非相干散射理论研究. 物理学报, 2017, 66(4): 049401. doi: 10.7498/aps.66.049401
[5]	闫昕, 梁兰菊, 张雅婷, 丁欣, 姚建铨. 基于编码超表面的太赫兹宽频段雷达散射截面缩减的研究. 物理学报, 2015, 64(15): 158101. doi: 10.7498/aps.64.158101
[6]	李文强, 曹祥玉, 高军, 赵一, 杨欢欢, 刘涛. 基于超材料吸波体的低雷达散射截面波导缝隙阵列天线. 物理学报, 2015, 64(9): 094102. doi: 10.7498/aps.64.094102
[7]	李学良, 石雁祥. 双麦克斯韦分布尘埃等离子体中尘埃粒子的充电研究. 物理学报, 2014, 63(21): 215201. doi: 10.7498/aps.63.215201
[8]	李勇峰, 张介秋, 屈绍波, 王甲富, 陈红雅, 徐卓, 张安学. 宽频带雷达散射截面缩减相位梯度超表面的设计及实验验证. 物理学报, 2014, 63(8): 084103. doi: 10.7498/aps.63.084103
[9]	李文强, 高军, 曹祥玉, 杨群, 赵一, 张昭, 张呈辉. 一种具有吸波和相位相消特性的共享孔径雷达吸波材料. 物理学报, 2014, 63(12): 124101. doi: 10.7498/aps.63.124101
[10]	梁达川, 魏明贵, 谷建强, 尹治平, 欧阳春梅, 田震, 何明霞, 韩家广, 张伟力. 缩比模型的宽频时域太赫兹雷达散射截面(RCS)研究. 物理学报, 2014, 63(21): 214102. doi: 10.7498/aps.63.214102
[11]	李思佳, 曹祥玉, 高军, 郑秋容, 赵一, 杨群. 低雷达散射截面的超薄宽带完美吸波屏设计研究. 物理学报, 2013, 62(19): 194101. doi: 10.7498/aps.62.194101
[12]	周前红, 董志伟. 弱电离大气等离子体电子能量分布函数的理论研究. 物理学报, 2013, 62(1): 015201. doi: 10.7498/aps.62.015201
[13]	杨利霞, 沈丹华, 施卫东. 三维时变等离子体目标的电磁散射特性研究. 物理学报, 2013, 62(10): 104101. doi: 10.7498/aps.62.104101
[14]	杨欢欢, 曹祥玉, 高军, 刘涛, 李思佳, 赵一, 袁子东, 张浩. 基于电磁谐振分离的宽带低雷达截面超材料吸波体. 物理学报, 2013, 62(21): 214101. doi: 10.7498/aps.62.214101
[15]	李思佳, 曹祥玉, 高军, 刘涛, 杨欢欢, 李文强. 宽带超薄完美吸波体设计及在圆极化倾斜波束天线雷达散射截面缩减中的应用研究. 物理学报, 2013, 62(12): 124101. doi: 10.7498/aps.62.124101
[16]	杨欢欢, 曹祥玉, 高军, 刘涛, 马嘉俊, 姚旭, 李文强. 基于超材料吸波体的低雷达散射截面微带天线设计. 物理学报, 2013, 62(6): 064103. doi: 10.7498/aps.62.064103
[17]	李民权, 陶小俊, 赵瑾, 吴先良. 基于辛Runge-Kutta-Nystrom方法的雷达散射截面计算. 物理学报, 2007, 56(4): 2115-2118. doi: 10.7498/aps.56.2115
[18]	石雁祥, 葛德彪, 吴健. 尘埃粒子充放电过程对尘埃等离子体电导率的影响. 物理学报, 2006, 55(10): 5318-5324. doi: 10.7498/aps.55.5318
[19]	刘少斌, 张光甫, 袁乃昌. 等离子体覆盖立方散射体目标雷达散射截面的时域有限差分法分析. 物理学报, 2004, 53(8): 2633-2637. doi: 10.7498/aps.53.2633
[20]	洪学仁, 段文山, 孙建安, 石玉仁, 吕克璞. 非均匀尘埃等离子体中孤子的传播. 物理学报, 2003, 52(11): 2671-2677. doi: 10.7498/aps.52.2671

计量

文章访问数: 4046
PDF下载量: 79
被引次数: 0

姓名
邮箱
手机号码
标题
留言内容
验证码

搜索

留言板

基于Fokker-Planck-Landau碰撞模型的非均匀尘埃等离子体目标散射特性