针对卫星通信工作频率越来越高的应用需求,设计了一种工作在极高频(Extremely High Frequency,EHF)的接收模块,实现极高频射频信号的接收及下变频功能。模块内部集成波导-微带探针过渡、低噪声放大器、微带滤波器、本振电路、混频器及...针对卫星通信工作频率越来越高的应用需求,设计了一种工作在极高频(Extremely High Frequency,EHF)的接收模块,实现极高频射频信号的接收及下变频功能。模块内部集成波导-微带探针过渡、低噪声放大器、微带滤波器、本振电路、混频器及供电电路,具有低噪声系数、高增益、高带外抑制的优点。采用单片微波集成电路(Monolithic Microwave Integrated Circuit,MMIC)混合多功能集成技术实现了模块的小型化、通用化,可适应多种场景下的极高频收发前端应用,具有广阔的应用前景。展开更多
The expression of mutual impedance between two probes in a circular waveguide is derived by means of a vector potential function, reaction concept and reciprocity theorem. The waveguide is semi-infinite, and one end o...The expression of mutual impedance between two probes in a circular waveguide is derived by means of a vector potential function, reaction concept and reciprocity theorem. The waveguide is semi-infinite, and one end of the waveguide is terminated to a load with a reflection coefficient. The contribution to the mutual resistance is found to come from the dominant mode, while the contribution to the mutual reactance comes from the dominant mode and the higher order modes. The major contribution to the mutual reactance is from the dominant mode, since the higher modes decay rapidly with the increasing the probes’ of separation distance. However, as the separation distance approaches zero, the higher modes become dominant, which results in a large value of the mutual reactance. The mutual impedance is dependent on the location and height of the probes, their separation distance and the location of the terminal plane.展开更多
基金Biographies: The National Natural Science Foundation of China(29776012).
文摘The expression of mutual impedance between two probes in a circular waveguide is derived by means of a vector potential function, reaction concept and reciprocity theorem. The waveguide is semi-infinite, and one end of the waveguide is terminated to a load with a reflection coefficient. The contribution to the mutual resistance is found to come from the dominant mode, while the contribution to the mutual reactance comes from the dominant mode and the higher order modes. The major contribution to the mutual reactance is from the dominant mode, since the higher modes decay rapidly with the increasing the probes’ of separation distance. However, as the separation distance approaches zero, the higher modes become dominant, which results in a large value of the mutual reactance. The mutual impedance is dependent on the location and height of the probes, their separation distance and the location of the terminal plane.
