Investigation of Millimeter-Wave Band Magnetron Dispersion Characteristics

M. Volovenko, O. Nikitenko
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Abstract

Considered in this paper is the influence of electrode temperature on dispersion characteristics of millimeter-wave band magnetron. Cavity resonators without straps were used in millimeter-wave band magnetrons. In this case such systems have resonance equation as, Yr + Yn = 0, where Yr-cavity impedance, Yn -interaction space impedance. The impedance of both interaction space and cavity has been defined. Dispersion characteristics of millimeter-wave band magnetron have been investigated. Calculation results are shown. The electrodes investigation devices have changed geometrical dimensions for anode, high and width slot cavity and for secondary cathode. Rz=Rz(1+Deltat) (2) RK=RKldr(l + Deltat)/pi where Delta-temperature expansion factor. This factor is different to anode and cathode. They have been determined separately. Dispersion characteristics of millimeter-wave band magnetron are presented for the case when temperature of both electrodes' is equal ~27degC, for the case when cathode and anode temperature is increased up to ~100degC and for the case when anode temperature is increased up to ~100degC, and cathode temperature is increased up to ~600degC. Using this method calculated accuracy has been achieved no more 5 % compared with experimental results. Separation of magnetron oscillation were changed from 5 to 14 % for different millimeter-wave band devices when the secondary cathode temperature has been changed from 27degC to 250deg C.
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毫米波磁控管色散特性研究
本文研究了电极温度对毫米波磁控管色散特性的影响。毫米波磁控管采用无带腔谐振器。在这种情况下,这种系统的共振方程为,Yr + Yn = 0,其中,Yr-腔阻抗,Yn -相互作用空间阻抗。定义了相互作用空间和腔体的阻抗。研究了毫米波磁控管的色散特性。计算结果如下所示。电极探测装置改变了阳极、高、宽槽腔和二次阴极的几何尺寸。Rz=Rz(1+ δ) (2) RK=RKldr(1+ δ)/其中δ是温度膨胀因子。这个因素对阳极和阴极是不同的。它们是分开确定的。给出了两电极温度等于~27℃、阴极和阳极温度升高到~100℃、阳极温度升高到~100℃、阴极温度升高到~600℃时毫米波磁控管的色散特性。与实验结果相比,该方法的计算精度不超过5%。当二次阴极温度从27℃变化到250℃时,不同毫米波器件的磁控管振荡分离率从5%变化到14%。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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