共查询到20条相似文献,搜索用时 62 毫秒
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提出了一种开敞式脊加载折叠波导慢波结构.通过除去直波导段周围的金属边界,形成一种开敞式结构以减弱色散,同时在直波导段加脊以提高耦合阻抗.研究表明,和传统结构相比,新型结构在不影响带宽的前提下,有效提高了耦合阻抗,尤其在大功率设计情况下,耦合阻抗的提高接近1倍. 相似文献
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提出了一种新型的微带线慢波结构。与传统的N型微带线慢波结构相比,新型结构具有相速值较小、工作电压低、功率大、耦合阻抗高等特点。利用HFSS和CST分别对此结构在V波段进行高频特性、传输特性和注-波互作用仿真,得出在60GHz频点耦合阻抗大于20Ω,在55~63GHz频段内VSWR<1.5;当输入功率为100mW时,并且带状电子注的电流和电压分别工作在100mA和5kV的条件下,该行波管慢波结构的最大输出功率为115W,平均互作用效率为14.6%,瞬时3dB带宽为5GHz(56~61GHz)。 相似文献
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采用理论分析和粒子模拟方法研究同轴内盘荷慢波结构注波互作用的物理机理。采用场匹配理论得到色散方程,通过数值计算得到了准TEM模的色散曲线及不同电子注电压下注波互作用的增长率;采用粒子模拟技术研究了注波互作用的物理过程。结果表明,随着电子注电压的不断增加,器件的工作状态由返波振荡转换到行波振荡;通过对辐射谱特性进行分析表明粒子模拟结果与理论计算结果基本一致。 相似文献
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A slow wave structure named Π — line is analysed in this paper. This circuit propagates slow waves in symmetrical and antisymmetrical mode. The dispersion relations of both symmetrical and antisymmetrical modes are derived here, by means of the field matching method. Numerical results are also given in this paper. The Π — line slow wave structure is of large diameter, and its radial supported stubs provide good heat conduction paths. These properties make this circuit well suited for use in high power, millimeter wave traveling wave tubes. 相似文献
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Quasi elliptic filters are of great demand in the present day communication systems. Coupling matrix analysis of pseudo-elliptic low pass filter using conventional microstrip line is presented in this paper. The conventional microstrip line has no non-zero cut off frequency. The conventional microstrip line is transformed into a pseudo-elliptic low-pass filter using the concept of slow wave. The slow wave microstrip line exhibits pseudo-elliptic low-pass behavior with transmission zeros at finite frequencies unlike the conventional Butterworth and Chebyshev filters. The coupling matrix of the slow wave microstrip line is arrived at by using the generalized Chebyshev functions. The coupling matrix of the slow wave line is validated using the MATLAB tool box. Finally, the prototype is fabricated and the performance is measured. 相似文献
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使用一种显式方法对0.14 THz折叠波导行波管慢波结构进行了快速设计,并通过解析模型、等效电路模型以及电磁场仿真软件(CST MWS)对结构的色散关系和耦合阻抗进行了计算。计算结果表明,0.14 THz附近的色散较为平坦,耦合阻抗在1Ω左右。为了满足大功率输出需求,对初始结构尺寸进行了部分调整。CST PS互作用模拟结果表明,在0.14 THz附近,输出功率大于1 W。用微电火花(EDM)和微铣削方法分别进行了加工实验,结果表明,两种方法在尺寸精确度上均能满足指标要求,微铣削加工能获得更平整、表面粗糙度更好的槽底。 相似文献
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在0.14 THz,0.22 THz和0.34 THz折叠波导行波管研制的基础上,讨论了0.41 THz折叠波导行波管慢波结构设计与加工的可行性,分析研究了折叠波导慢波结构弯曲处直角弯曲与半圈弯曲、方形电子注通道与圆形电子注通道对色散特性、耦合阻抗、带宽、冷损耗和增益的影响。考虑了慢波结构中增加理想衰减器对该行波管带宽和增益的影响,得到了0.41 THz折叠波导行波管慢波结构的初步设计方案,为太赫兹折叠波导行波管的继续发展打下了一定基础。 相似文献
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《Solid-state electronics》1987,30(5):497-502
The use of MeV ion-implantation for realization of a GaAs monolithically compatible device is demonstrated. Ion implants up to 6 MeV in energy are used employing Si and S atoms. The fabricated device is an electromagnetic slow wave microstrip-like structure designed for performance into the millimeter wave regime. Phase shift θ and insertion loss L measurements are performed for frequencies 2–18 GHz at room temperature. Comparison of the experimental ion-implanted device results to epitaxial device results indicates comparable electrical performance, with no more than a 30% reduction in θ but with an improvement in loss behavior, namely a L reduction up to 40%. These θ and L differences between the ion-implanted and epitaxial devices are attributed to differences in doping profiles. Theoretical modelling of θ characteristics produces agreement with experimental data to within a few percent. 相似文献
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对W波段三槽梯形线耦合腔慢波结构(包括大功率输入输出耦合器和射频窗)的加工和冷测进行了研究。此慢波结构由一个矩形波导耦合器馈电,该耦合器由放置在输入腔短边上的三阶阶梯变换矩形波导组成。首先,利用仿真方法研究了慢波结构的色散、互作用阻抗、传输特性和注-波互作用。结果表明,采用三槽梯形线耦合腔慢波结构的行波管能够在91~96 GHz的频率范围内提供大于1000 W的饱和输出功率,并且在94 GHz频点,饱和输出功率最大,可以达到1125 W。其次,采用高精度数控铣床加工出三槽梯形线慢波结构,并将其固定在非磁性不锈钢外壳中。文中给出了带有耦合器和射频窗的三槽梯形线慢波系统的测试结果,表明在90 GHz到100 GHz的频率范围内,S11<-10 dB。因此,三槽梯形线慢波结构在W波段大功率行波管方面具有应用前景。 相似文献
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The capability of heat conduction of the slow wave structure is one of the main obstacles to the development of the high-frequency
high-power helix TWTs. A simple but reliable technological method for obtaining high heat conduction capability and low rf
loss is suggested. The method of measurement of the heat conduction capability and the results of this measurement are also
given. 相似文献