共查询到18条相似文献,搜索用时 218 毫秒
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复杂目标后向激光雷达散射截面计算与缩比模型测量比较 总被引:10,自引:2,他引:10
研究了复杂目标激光雷达散射截面(LRCS)与电磁波段雷达散射截面的差异,提出使用可视化技术计算复杂目标后向激光雷达散射截面的流程框图,并使用该技术对某飞机全尺寸模型进行了计算。将计算结果按缩比关系换算,得到了1:8缩比模型的散射截面。利用标准板定标法,在外场环境对1:8缩比模型进行了实际测量,获得了缩比模型散射截面的实验数据。对计算数据与测量数据进行了对比分析,结果表明,在目标主要散射方位,理论计算和测量结果一致;通过缩比模型的测量可以获取全尺寸目标的激光散射特性。 相似文献
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首先,对雷达目标电磁散射特性的重要性做了简单介绍,对获取雷达目标电磁散射特性数据的方法进行了分类;然后,详细回顾了电磁仿真与测量的主要方法的基本原理、发展过程与适用范围;最后,阐述了国内在雷达目标电磁散射特性研究方面取得的进展与基本情况,对电磁仿真与测量的技术发展趋势进行了总结。 相似文献
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全尺寸目标激光脉冲后向散射回波功率测定和建模 总被引:7,自引:1,他引:7
运用粗糙面散射、激光脉冲散射理论,结合复杂目标粗糙表面相关建模参数,建立用于计算全尺寸复杂目标激光脉冲后向散射功率的理论模型.实验测量一种空中缩比目标模型后向散射激光脉冲回波功率,获取该缩比目标激光脉冲后向散射功率随接受天顶角的变化曲线.比较理论建模与实验测量数据,分析实验误差,证明了该理论模型的正确性.将建立的理论模型进一步应用于计算非合作空间全尺寸目标的激光脉冲回波功率.计算结果能够预估空间目标的激光散射特征,解决一些关于空间目标激光脉冲光学特征工程的应用问题. 相似文献
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提取系统的冲击响应函数(impulse response function,IRF)是测量雷达系统性能指标的前提,IRF来自理想点目标的雷达图像。对于低频超宽带合成孔径雷达(ultra wide band synthetic aperture radar,UWB SAR),参考点目标的电磁散射特性是频率和方位角的函数,不满足理想点目标的散射特性要求。本文从IRF的定义出发,结合低频UWBSAR系统处理模型,利用二维数字聚焦方法消除杂波的影响,同时利用低频电磁散射数值建模的方法计算参考点目标的电磁散射特性,最后给出了计算系统IRF的方法。 相似文献
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全尺寸目标的电磁散射特性测试,需要足够大的测试距离或紧缩场系统,但是建设满足远场条件的室外静态场与室内紧缩场需要巨大的经费投入和很高的技术条件,更无法对飞行器进行现场成像与雷达散射截面(Radar Cross Section,RCS)诊断.针对近距离测试检定飞行器隐身性能的需求,提出了基于散射分布函数模型的近远场变换算法.建立三维散射分布函数模型,采用三维扫描方式记录近场数据,将球面波函数分别在柱坐标系、三维直角坐标系与球坐标系下展开,变换得到目标的远场数据,通过三维逆傅里叶变换与插值算法给出目标的三维重建图像与远场RCS.仿真分析与实验表明,算法准确有效. 相似文献
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本文提出了三个对有耗介质目标进行散射缩比测量时,所应遵循的相似法则。只要满足其中一个相似法则,就可以把所测的模型雷达散射截面(RCS)变换为原型的RCS。文中给出了三个相似法则的使用范围,相似条件及RCS诱导相似比。对第一相似律进行了实验验证,结果表明:原型的实测结果与由模型测量结果所变换的原型结果吻合很好,变换误差为1~2dB。同时,用电磁介质涂敷金属球的精确解,对三个相似律进行了验证,结果表明,第二、第三相似律可适用于全频段,变换误差小于1dB。第一相似律只适用于光学区,在Rayleign区和谐振区有较大误差。 相似文献
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提出一种基于电磁等效原理的一组积分方程,应用变分方法和傅立叶变换理论,得到了时域散射场与目标电磁参数之间非线性关系的频域表示式,即反演自由空间中二维电磁目标的时域非线性迭代方法的反演方程。列举了一些典型的数值反演实例,对反演性能进行了多方面的考察,指出本法是一种具有良好反演性能的时域非线性反演方法。 相似文献
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The millimeter-wave polarimeter (MMP), a scatterometer system uses the HP 8510A vector network analyzer for coherent processing of the received signal, provides the polarization and phase measurement capability needed to measure the complete scattering matrix of a given target. A calibration and measurement technique that was used with the MMP at 35 GHz to measure the scattering matrix for both distributed and point targets is described. The measurement accuracy was analyzed by comparing theoretical and measured values for a set of conducting spheres and finite-length conducting cylinders. As an extension of the analysis to natural targets, the scattering matrix was measured for a series of twigs and various smooth and rough surfaces 相似文献
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Ultra-wideband impulse scattering measurements 总被引:3,自引:0,他引:3
A recently upgraded laboratory is described for measurement of ultra-wideband (1-20 GHz) impulse scattering responses from scale model radar targets. A linear systems model is introduced, leading to new measurement concepts and signal processing algorithms for estimating the target's scattering response to a user-defined impulse waveform. The experimental and processing procedures serve to eliminate clutter and antenna coupling, while compensating for antenna characteristics in the system. Experimental validations are examined and planned enhancements are discussed 相似文献
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Tzong-Jyh Chen Tah-Hsiung Chu 《Antennas and Propagation, IEEE Transactions on》1997,45(7):1080-1085
The principle of operation, calibration procedure, and experimental results of a wideband six-port polarimetric measurement system are described in this paper. This measurement system can measure the polarization states of incoming waves and the polarimetric scattering matrices of scattering targets from the wideband power data. The imbalances and coupling between antenna polarization channels and the characteristics of microwave components used in the measurement system are calibrated using three partly unknown scattering calibrators that are illuminated by four unknown-polarized calibrating waves 相似文献
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Sullivan A. Damarla R. Geng N. Yanting Dong Carin L. 《Antennas and Propagation, IEEE Transactions on》2000,48(9):1306-1315
Electromagnetic (EM) scattering from subsurface unexploded ordnance (UXO) is investigated both theoretically and experimentally. Three EM models are considered: the multilevel fast multipole algorithm (MLFMA), the method of moments (MoM), and physical optics (PO). The relative accuracy of these models is compared for several scattering scenarios. Moreover, the model results are compared to data measured by an experimental synthetic aperture radar (SAR) system, SAR images have been generated for subsurface UXO targets, in particular 155-mm shells. We compare SAR images from the measured data with theoretical images produced by the MoM and PO simulations, using a standard back-projection imaging technique. In addition to such comparisons with measurement, we consider additional buried-UXO scattering scenarios to better understand the underlying wave phenomenology 相似文献
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Nashashibi A. Sarabandi K. Ulaby F.T. 《Antennas and Propagation, IEEE Transactions on》1995,43(4):396-404
A new technique for calibrating a coherent-on-receive polarimetric radar system is proposed. A coherent-on-receive polarimetric radar is capable of measuring the Mueller matrix of point or distributed targets directly by transmitting at least four independent polarizations and measuring the vertical and horizontal components of the backscatter signal simultaneously. The technique requires the use of two calibration targets, a target with known scattering matrix (such as a metallic sphere or a trihedral corner reflector) and any depolarizing target (for which knowledge of its scattering matrix is not required) to determine the system distortion parameters. The system distortion parameters, which include the channel imbalances, the cross-talk factors of both the transmit and the receive antennas, and the phase shifts and amplitude variations of the transmitter polarizers, are determined by measuring the calibration targets for four different transmit polarizations. The validity of the new calibration technique is examined by measuring the scattering matrices of spheres and cylinders as test targets using a coherent-on-receive radar operating at 34.5 GHz. Excellent agreement between the theoretical and the measured scattering matrices for the test targets are obtained 相似文献