南京大学学报(自然科学版) ›› 2013, Vol. 49 ›› Issue (1): 95–100.

• • 上一篇    下一篇

 太赫兹高斯脉冲球体雷达散射截面研究*

 赵帅**
  

  • 出版日期:2015-09-24 发布日期:2015-09-24
  • 作者简介: (南京大学物理学院,南京,210093)
  • 基金资助:
     国家"883”计划(2006AA03Z458),国家自然科学基金(60977042, 10904-061)

 Scattering of sphere by Terahertz Gaussian pulse

Zhan Shuai   

  • Online:2015-09-24 Published:2015-09-24
  • About author: (Department of Physics,Nanjing University,Nanjing,210093,China)

摘要:  选择作为表征散射体对入射波散射能力重要参数的需达散射截而(RCS)为研究对象,应用时
域有限差分法(FDTD)仿真计算了太赫兹高斯脉冲波对亚mm至?m量级尺度的金属铜和三聚氰胺甲
醛树脂(MF)微粒的电磁散射.散射目标尺寸取为300 ?m至3 ?m,该尺寸与太赫兹波长范围3 mm至
30 ?m大致重叠.由于太赫兹带宽很大,该量级大小的微粒散射区间很大部分处在瑞利散射向Mie散射
的过渡区,解析解会受到应用范围的限制,所以选择数值计算方法FDTD.即把入射平面波设为宽频带
脉冲,其频带宽度覆盖了求解的频率范围,计算散射体对脉冲波的响应并进行傅里叶变换就可以得到散
射体的宽频响应.通过选取不同尺寸大小(半径300 ?m至3 ?m)、材质(金属铜和三聚氰胺甲醛树脂)、
几何构成(实心、空心、双层),对散射目标进行分类和对比,得出了球形微粒的太赫兹波需达散射截面特
性.由于目标的宽频带特性中包含了大量信息,其低频区包含了目标的体积信息,谐振区包含了目标的
轮廓信息,为该量级尺寸微粒的检测识别以及太赫兹波段屏蔽材料的选择提供了依据.

Abstract:  The radar cross section(RCS)is an important parameter of the scattering ability of incident wave, this pa-
per choose it as the research object,using the finite difference time domain method(FDTD)to simulate the progress
of terahertz Gaussian pulse scattering by particles making of copper and melamine formaldehyde resin(MF).The in-
cident plane wave is set as Gaussian pulse,the band width of which coverage for a range of frequencies to be calculat-
ed and the frequency response to scattering spheres can be get from Fouricr transform. In this paper, numerical cal-
culation of RCS has the following characteristic;the size of scattering target range from 300? m to 3? m,and tcra-
hertz wavelength range from 3 mm to 30? m,they are broadly overlapping. As a result of terahertz bandwidth, the
size range of the scattering particles is in the transition zone from Raylcigh scattering to Mie scattering, the use of
analytical solution is limited by the range of application, In this situation, numerical computational method FDTD is
selected to classify and compare scattering targets in different sizes(range from 300 ?m to 3? m),matcrials(copper
and MF)and gcometrics(solid sphere, hollow sphere,two layers sphere). With the increase of diameters,electromag-
netic scattering intensity of metal and MF spheres radius of which are from 3? m to 300? m increase. At the same
time,the distribution of scattering intensity gradually focus to back. For the symmetry of forward and backward
scattering,MF spheres radius of which arc from 3 ?m to 30 ?m arc better than that of the metal spheres. Forward
and backward RCS of MF sphere radius of which is 3 um consistently increase with the frequency increase. On the
other hand,with the increase of particles size, oscillation of frequency response curves exacerbate,especially for the
backward scattering. When the particle size is increased by one order of ma}nitudc,the forward scattering intensity
of electric field is increased by 2 to 3 orders of magnitude.The numerical size difference of electric field scattering in-
tensity between forward scattering and backward scattering of MF spheres radius of which arc from 3 ? m to 300? m
gradually increase from the almost identical to 3 orders of magnitude. At last,for the hollow MF sphere radius of
which is 30 ?m,duc to the formation of a resonant cavity and small volume which takes part in forced vibration,
merge a number of distinct minima,and at the same time its RCS is significantly smaller than that of the solid MF
sphere.
The broadband characteristics of target contains a lot of information,thc low frequency region contains volume
information of the target,the resonant region contains contour information of the target.The research of RCS pro-
vides the basis for target detection and materials selection of terahertz band shielding.

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