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本程序为星载降水雷达卫星测量地面降雨时,回波的归一化雷达散射截面图。
主程序为FiSAR,其他两个程序为嵌套的函数。-This procedure for the spaceborne precipitation radar satellite measurements of rainfall on the ground, the echoes of the normalized radar cross section diagram. The main program for the Fi
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目标的雷达散射截面(RCS)包含了丰富的目标类别信息,如何有效利用目标RCS特征对空间目标的雷
达识别具有重要意义. 文中提取中心矩作为特征向量,采用主分量分析( PCA)进一步进行特征压缩,利用支撑矢
量-Target radar cross section (RCS) contains a wealth of objective categories of information, how the effective use of target RCS characteristi
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用c++语言,编写了基于FDTD的三维散射体雷达散射截面的计算程序。程序注释清楚。稍微改动必要的数据就可以直接使用。已经多次验证了程序的正确性。-Using c++ language, compiled based on three-dimensional FDTD radar cross section scattering calculation program. Program notes clearly. Slightly change the necessary data can be
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Radar Cross Section book by "Eugene F. Knott, John F. Shaeffer, Michael T. Tuley
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天线耦合仿真算例,大型舰船模型,雷达反射截面积-Antenna coupling simulation example, a large ship models, radar cross section
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用c++语言,编写了基于FDTD的三维散射体雷达散射截面的计算程序。程序注释清楚。稍微改动必要的数据就可以直接使用。已经多次验证了程序的正确性。-Using c++ language, compiled based on three-dimensional FDTD radar cross section scattering calculation program. Program notes clearly. Slightly change the necessary data can be
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本程序是用来计算导体球的电磁散射的雷达截面问题的,使用的是由MATLAB编写的-This procedure is used to calculate the electromagnetic scattering problem of radar cross section of the conductor ball, the use of MATLAB
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这是一个早期预警雷达的模拟。模拟生成随机目标(坐标、速度、加速度和雷达散射截面(RCS))。(It is a simulation of an early warning radar. The simulation generates random targets (coordinates, velocity, acceleration & Radar Cross Section (RCS)).)
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TE波照射无限长导体柱求雷达散射截面、TM波照射无限长导体柱求雷达散射截面(TE wave is used to irradiate an infinite conductor cylinder, radar cross section and TM wave are used to obtain the radar cross section of an infinite conductor cylinder)
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用comsol来求解雷达散射截面,麦克斯韦方程的重要应用(Using comsol to solve the radar cross section, the important application of Maxwell's equation)
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使用Mie系列解决方案计算给定直径的完美球体的精确RCS
使用Mie系列解决方案计算给定直径的完美球体的精确RCS(SPHERE_RCS calculates the exact RCS for a perfect sphere of given diameter, using the Mie series solution, given by equations 4-19, 4-16, and 4-17 in section 4.2 of "Radar Cross Section,
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