共查询到18条相似文献,搜索用时 156 毫秒
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基于射线追踪法开发的静区电平仿真软件应用于AFA型吸波材料(难燃型吸波材料)铺设的微波暗室静区性能仿真。软件以国内暗室性能检测机构的喇叭天线数据为依据设定发射天线的辐射特性模拟函数,得到发射天线的直射波方向图。以AFA 型吸波材料的实测数据为依据设定吸波材料的吸波特性模拟函数,计算微波暗室各面墙壁反射电场在静区内叠加后的总反射电场值,并据此得到静区内的反射电平分布。仿真与实测结果表明,1 GHz 以下静区反射电平仿真结果下限值与测试结果偏差相对较大;1 GHz 以上两者偏差小于1 dB,吻合较好。验证了该仿真软件能够快速并较准确地用于微波暗室吸波工程的设计与评估。 相似文献
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为提升暗室吸波工程的设计能力,运用镜像射线跟踪法对10 m 法电波暗室进行仿真设计,通过合理布置吸波材料,考虑一次反射和二次反射对静区的影响,计算了不同极化方式下静区的反射电平、归一化场地衰减和场均匀性。结果表明垂直极化和水平极化时,场地电压驻波比仿真与测试偏差小于2.3 dB;归一化场地衰减仿真与测试误差小于3 dB,场均匀性误差小于2 dB。仿真与测试结果吻合较好,各项指标均满足设计要求,验证了吸波材料布局的合理性及算法的可靠性。该仿真方法可应用于暗室静区性能评估,优化吸波材料布局,进而有效缩短设计周期。 相似文献
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介绍AXB型吸波材料的性能.用AXB型吸波材料建造的天线近、远场测量微波暗室,10m半电波暗室和RCS测量微波暗室的技术指标都符合相关标准的要求. 相似文献
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详细介绍了电波暗室用吸波材料的种类、制造工艺,以及电波暗室用吸波材料的反射率、阻燃性、耐功率等性能指标,为暗室建造企业在选择吸波材料时提供参考. 相似文献
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0引言:为什么要测量微波暗室的剩余互调
微波暗室分为全电波暗室和半电波暗室.全电波暗室定义为六面装有吸波材料的屏蔽室,用于模拟自由空间;半电波暗室则是五面装有吸波材料,地面为反射面,用于模拟开阔场.常见的微波暗室的墙体由铁氧体材料加微波吸波材料组成.和其他无源器件一样,微波暗室也遵循互调产生的机理.在大功率多载频的作用... 相似文献
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双喇叭微波暗室不但包含有锥形暗室和矩形暗室的特征和优点,而且建造这样的暗室能减少吸波材料和暗室建筑费用15%。柱型暗室具有独特的用途,对称性好,电磁静区的性能也比矩型暗室优良。 相似文献
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微波暗室为电磁波的定性分析或定量测试提供一个近似无反射的环境,当微波暗室内存在的反射不能忽略时,暗室墙面反射引起的多路径传输就会影响对测试结果的评定。在阐述比幅单脉冲测向原理的基础上,研究了由于暗室静区反射电平对雷达告警系统测向精确度的影响,建立了暗室静区反射电平与雷达告警接收机测向误差的关系模型,并且结合四元阵、八元阵、十六元阵说明了静区反射电平、来波方向与测向误差范围的关系。 相似文献
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暗室为卫星导航接收机抗干扰测试提供了全面有效的测试环境,极大地提高了抗干扰性能定量测试与评估能力。但暗室的静区性能、结构尺寸、天线布局等因素会对抗干扰性能测试结果产生影响。基于多径信号天线接收模型、阵列波程差等效模型和信号来向天线映射模型,通过仿真量化分析了干扰多径信号、有限距离下近场效应和来波方向误差对抗干扰测试结果的影响。结果表明,暗室静区性能的提升可降低干扰多径信号对零陷位置的拉偏;不同暗室尺寸对应不同的零陷深度测试,需根据测试需求折中选择;布设暗室天线应依据预设的被测阵列天线和测试场景。结果可为暗室设计、抗干扰测试方案选定和测试结果分析提供参考,提升抗干扰测试的可信度。 相似文献
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An electromagnetic anechoic chamber has been constructed at the Multimedia University. It is designed to operate over a very wide frequency range from 30 MHz through 18 GHz. It can be used for electromagnetic compatibility (EMC) tests, antenna measurements, radar cross section (RCS) measurements, testing RF transceivers, calibration of scatterometers, and other electromagnetic research experiments. The geometry of the chamber is asymmetrical, consisting of a combination of rectangular and tapered volumes. The size of the chamber is about 64 ft /spl times/ 32 ft /spl times/ 24 ft high. Ease of construction and ease of lining of the absorbers were preserved so that the actual quietness is comparable to the theoretical simulation result. The transmitting source is placed at one end of the chamber, and the receiving antenna or object under test is placed in a designated quiet zone at the other end. The walls and ceilings are configured such that no first-order and or second-order reflections (except those reflected from the floor) propagate into the quiet zone. Hence, less-expensive absorbers can be used to achieve the required wideband performance. Reflection from the floor is required by the international EMC standards for radiated electromagnetic interference (EMI) emission tests; therefore, the chamber is designed for this capability. However, absorbing material can be placed on the floor to convert a semi-anechoic chamber into a fully anechoic chamber for radar and antenna measurements. 相似文献
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Dau-Chyrh Chang Chao-Hsiang Liao Chih-Chun Wu 《Antennas and Propagation Magazine, IEEE》2004,46(4):27-37
There are several types of CATRs (compact antenna test ranges) used in antenna-pattern measurements. An offset reflector is generally used to generate the quiet zone of a CATR. Serrated edges, rolled edges, or R-cards are generally chosen along the reflector's edge to reduce the edge-diffraction field inside the quiet zone of the CATR. In order to reduce stray signals from the environment, a high-quality RF anechoic chamber is required for a CATR. In this paper, a new type of CATR, without either a reflector edge treatment or an RF anechoic chamber, is developed. A commercially available DBS (direct-broadcast satellite) reflector antenna, without edge treatment, is used as the reflector antenna of the CATR to generate the quiet zone of the antenna test range. In order to improve the quiet zone's performance, the fields due to feed spillover, edge diffractions, and other stray signals are gated out by the ITDAMS (impulse time-domain antenna measurement system). The RF interference in the environment can also be reduced by time synchronization and pulse integration of the impulse time-domain antenna measurement system. In order to verify the capabilities of the proposed CATR, three kinds of antennas (a low-directivity horn antenna, a high-directivity 60 cm direct-broadcast satellite reflector antenna, and a 25 cm Ka-band Cassegrain LMDS - local microwave distribution system - antenna) were measured by the proposed CATR. The antenna-pattern results agreed quite well with those of a near-field range and a far-field range. 相似文献