粗糙面下方金属目标复合电磁散射的快速算法

为快速有效计算粗糙面下金属目标的复合电磁散射,提出了一种基于前后向迭代算法(FBM)和共轭梯度(CG)法的快速互耦迭代算(CCIA).首先建立目标与粗糙面的耦合积分方程组,并采用矩量法将其离散为矩阵方程.其次针对得到的耦合积分方程,用FBM求解粗糙面表面电流分布,用CG法求解目标表面电流分布,目标和粗糙面的相互作用通过更新两方程的激励项完成.最后,计算了高斯粗糙面下方无限长金属圆柱目标的复合电磁散射系数,当目标尺寸趋于零或目标深度趋于无穷时的结果与单独介质粗糙面相一致,验证了该数值方法的正确性;同时,讨论了不同粗糙面情况下该方法的收敛性,并分析了不同粗糙面媒质、目标尺寸和目标位置对双站散射系数的影响.     

分析电大开口腔体电磁散射的快速混合算法-IPO+FMM

电大尺寸开口腔体结构的高频电磁散射分析是复杂目标RCS分析预测中一项很有意义和难度的工作,提出 一种混合算法-IPO+FMM,将迭代物理光学法与快速多极子方法相结合,对电大尺寸开口腔体进行电磁散射分析,文中对 IPO+FMM混合算法进行理论分析与公式推导,希望在保证分析精度的同时减小计算量,提高计算速度。     

复杂目标双站图形电磁计算

应用物理光学法（ＰＯ）与等效电磁流法（ＥＣＭ）分别计算了复杂目标双站散射中面元与棱边的散射场。在ＷＩＮＤＯＷＳ ＮＴ／９８微机平台上利用软件图形标准接口Ｏｐｅｎ ＧＬ和硬件图形加速卡对目标和背景像素进行实时显示和自动消隐,通过对各像素点的散射场计算和要位综合求得总散射场,从而将ＧＲＥＣＯ扩展为双站图形电磁学。数学模型和实例说明了本方法的正确性,对＊＊战斗机双站ＲＣＳ进行计算,对将来虚拟现实系统环境     

海面上电大尺寸目标电磁散射特性研究

基于几何光学法(GO)、物理光学法(PO)、射线弹跳法(SBR)和等效电流法(MEC),提出了一种快速计算金属海面上电大尺寸目标电磁散射的解析算法。该算法考虑了阴影效应,运用GO/PO+SBR计算了目标与海面的镜面反射以及它们之间的多次相互作用,并运用MEC计算了目标的棱边绕射以改进计算结果。应用该算法计算了平板上方规则金属目标的双站雷达散射截面(RCS),并与传统矩量法(MoM)进行比较,验证了算法的有效性。最后,计算了PM(Pierson-Moskowitz)海浪谱的随机海洋粗糙面上舰船模型目标的散射特性,并对计算结果进行了分析,讨论了海洋面以及入射波参数对散射结果的影响。     

复杂目标电磁散射混合算法

分析了复杂目标高频散射雷达截面(RCS)计算理论,提出了一种有效的混合算法.改进了等效电磁流方法(IMEC),推导了几何光学/物理光学区域投影算法(GO/PO).IMEC能有效地消除反射边界和阴影边界的奇异性,GO/PO法用于计算多重散射.通过AutoCAD软件,使用三角面元法构建目标三维模型.目标的高频雷达散射截面通过几何光学、物理光学、改进的等效电磁流和几何光学/物理光学区域投影等混合方法计算获得.同时,计算了某型号导弹的RCS,理论值同测量结果基本一致,说明该方法能满足复杂目标电磁散射分析的需要.     

基于三角网格的凸导体目标SB-ILDC算法

阴影边界增量长度绕射系数(SB-ILDC)可以用于计算电大尺寸目标在阴影边界处由不一致电流产生的表面绕射场,其在双站散射计算中对物理光学法(PO)有显著的修正作用。本文提出了一种基于三角网格模型的目标阴影边界寻迹算法,并将SB-ILDC拓展应用于三角网格模型光滑凸表面目标的宽带双站散射和高分辨率一维距离像的计算。通过典型目标计算结果同Mie级数解的对比,证明该方法对于凸导体目标PO散射场的修正是快速、显著的。     

分层粗糙面下方介质目标散射的快速算法

为快速获取分层粗糙面与下方介质目标的复合电磁散射特性,提出了一种基于前后向迭代算法(FBM)和双共轭梯度法(Bi-CG)的快速互耦迭代算法。推导了一维分层粗糙面与下方介质目标(二维散射问题)的耦合边界积分方程组,用FBM求解分层粗糙面的表面积分方程,而用Bi-CG求解目标的表面积分方程,目标和粗糙面的相互耦合作用通过更新两方程的激励项来迭代求解。应用该算法计算了下方存在介质目标时双层介质粗糙面的双站散射系数,与传统矩量法得到的结果相吻合,验证了该算法的正确性;分析了不同极化波入射时该算法的收敛性,讨论了目标尺寸和位置变化对双站散射系数的影响。     

一维微粗糙面与其上方金属平板的复合电磁散射研究

研究了一维导体随机粗糙面与其上方金属平板的复合电磁散射。应用互易性原理使求解复合目标的二次散射场简化为求解包含平板上的极化电流和微粗糙面散射场的积分方程。利用物理光学近似和粗糙面微扰法分别计算了平板上的感应电流和粗糙面的电磁散射场,导出了复合散射模型单、双站散射的计算公式并给出了单站数值计算结果,讨论了后向复合散射截面随入射频率及平板尺寸、位置的变化关系。     

IPO-MoM混合法分析开槽电大目标的电磁散射

本文利用迭代物理光学法（ＩＰＯ）与数值方法相结合的混合方法计算二维开槽民大目标的电磁散射,首先根据等效原理将散射场进行分解,分别采用ＩＰＯ法和矩量法（ＭｏＭ）计算槽缝填充的电大目标和槽缝的散射,并在口径处应用广义网络原理处理耦合问题,数据结果表明本文方法是准确和高效的。     

IPO—MoM混合法分析开槽电大目标的电磁散射

本文利用迭代物理光学法（ＩＰＯ）与数值方法相结合的混合方法计算二维开槽民大目标的电磁散射,首先根据等效原理将散射场进行分解,分别采用ＩＰＯ法和矩量法（ＭｏＭ）计算槽缝填充的电大目标和槽缝的散射,并在口径处应用广义网络原理处理耦合问题,数据结果表明本文方法是准确和高效的。     

涂层目标散射的双站物理光学公式及其散射矩阵

本文从物理光学基本假设与阻抗边界条件出发，建立了涂覆雷达吸波材料（ＲＡＭ）的任意三维光滑凸型导电物体散射的基本双站公式。公式是从Ｆｒｅｓｎｅｌ反射系统及阻抗边界条件推导的。本文同时得到了涂层物体表面入射场及其同几何结构导体表面入射场之间的关系与电、磁流比系数关系。文末给出了用基本双站公式计算电大物体双站散射矩阵与双站散射截面的计算方法与计算实例。     

Polarization correction and extension of the Kennaugh-Cosgrifftarget-ramp response equation to the bistatic case and applications toelectromagnetic inverse scattering

An analytical time-domain expression derived by Kennaugh (1967) for the early time impulse response for smooth, convex, perfectly conducting scatterers under the physical optics approximation for the bistatic case is reinterpreted. The physical optics bistatic early time impulse responses can be interpreted as cross-sectional areas of the scatterer. A crude polarization correction to the leading edge of the physical optics impulse response is obtained for the bistatic case, leading to a simple asymptotic relation between the specular principal curvature difference and certain co-polarized phase terms in the bistatic scattering matrix. Applications to direct scattering are discussed. Profile reconstruction from bistatic data with a priori knowledge of the validity range of physical optics in the time domain is proposed and tested with the sphere     

Plane wave scattering from 2-D perfectly conducting superquadriccylinders

The plane-wave scattering from perfectly conducting two-dimensional cylinders of arbitrary squareness parameter is investigated. A uniform geometrical optics (UGO) solution valid across the smooth caustics generated by the surface poles or zero curvature (inflection) points is developed based on physical optics (PO). The classical geometrical optics solution is modified using a multiplicative transition function that compensates for the caustic singularities and accounts for the complex ray contributions emanating from nonspecular scattering centers located near the surface poles. The transition function is heuristically derived on the basis of the PO radiation integral and involves a generalized (higher-order) form of Airy functions. The resulting UGO solution for the scattered field is simple, easy to apply, and computationally efficient for electrically large cylinders. It compares well with physical optics (numerical integration) and moment-method solutions for both backscatter and limited bistatic configurations     

Synthesis of tapered resistive strips

A technique for synthesizing a resistive taper that generates desired bistatic scattering and backscattering patterns from a strip is outlined. Antenna synthesis techniques relate the scattered field to the induced surface current density. Physical optics approximations then relate the induced current to the resistivity. The taper is checked by computing the surface current density and scattered fields of the tapered resistive strip using the integral equation formulation and comparing with the physical optics results.     

A fast physical optics (FPO) algorithm for double-bounce scattering

The fast physical optics (FPO) method for computing back-scattered fields over ranges of aspect angles and frequencies is extended to encompass double-bounce scattering. Computations are performed within the framework of the physical optics approximation appropriate in the high-frequency regime. The proposed algorithm is directly applicable to fixed angle bistatic configurations and a variety of double scattering settings. The method comprises two steps: 1) decomposition of the scatterer into subscatterers and computation of the scattering amplitudes of all pairs of subscatterers and 2) interpolation, phase correction, and aggregation of the scattering amplitude patterns of all subscatterer pairs into the pattern of the entire scatterer. The proposed method is especially suited for generating synthetic data for radar imaging simulations.     

Scattering by a ferrite-coated conducting sphere

The theory for scattering by a perfectly conducting sphere with a coating of lossy, homogeneous, isotropic ferrite material is presented. In addition to the rigorous eigenfunction formulation, the physical optics (PO) and geometrical optics (GO) approximations are also included. Numerical results are shown in graphical form to illustrate the backscatter echo area versus the radius of the sphere, as well as the bistatic scattering patterns.     

A Study of an AIEM Model for Bistatic Scattering From Randomly Rough Surfaces

In this paper, we study the bistatic scattering using an advanced integral equation model (AIEM). By keeping all the surface current terms in the Kirchhoff surface fields, the bistatic scattering coefficients are obtained. For simplification, the complete Kirchhoff field did not cast into the derivation of the complementary field. We compare varied updated versions of IEM-based models with the small perturbation model, geometrical optics model, and Kirchhoff approximation standard models at respective regions of validity. The results indicate that the new AIEM provides much more accurate predictions for bistatic scattering.      

On scatterer reconstruction from far-field data

The reconstruction problem of perfectly conducting bodies from far-field scattering data is discussed within the context of physical optics. The general bistatic scattering configuration, discussed in this investigation, adds inherent complexity to the problem but also introduces possibilities not present in the backscatter limit.     

A fast physical optics (FPO) algorithm for high frequency scattering

A novel algorithm referred as the fast physical optics (FPO) for computing the back-scattered field over a range of aspect angles and frequencies is presented. The computation is performed in the framework of the conventional physical optics approximation appropriate for the high frequency scattering regime. The proposed algorithm is, also, directly applicable to fixed angle bistatic configurations and a variety of single scattering formulations. The method comprises two steps. First, a decomposition of the scatterer into subdomains and computation of the pertinent scattering characteristics of each subdomain. Second, interpolation, phase-correction and aggregation of the scattering patterns of the subdomains into the final pattern of the whole body. A multilevel algorithm is formulated via a recursive application of the domain decomposition and aggregation steps. The computational structure of the multilevel algorithm resembles that of the FFT. The proposed method is especially suited for generation of synthetic data for radar imaging simulation.