A Complete Set Of Passband Tapped Circuits And Practical Application Range

A. Podcameni, M.S. Cordeiro de Mello
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Abstract

Tapped resonant LC circuits are investigated here in order to determine, in both qualitative and quantitative ways, how they deviate from previously proposed models. Mismatch, frequency shift and bandwidth shrinkage are observed. Limits for practical use suggested. Moreover, two additional tapped individuals are offered and modeled for the benefit of complex load matching applications. Introduction: The tapped capacitor and tapped inductor circuits, shown in Fig. l(a) and (c), respectively, have the same kind of transfer function. They are sometimes called as capacitor or inductor transformers [l], or parallel transformerlike network [2]. Their advantage is to provide the selectivity of a passband LC circuit combined with the effect of a physical transformer. Clarke and Hess [2] have mentioned the two above circuits and it was shown that, if some conditions are met, the equivalent circuits may be those of Fig. l(b) and (d), respectively. The correspondence between the circuit elements and the models is provided in Table 1. The equivalent circuits possess a shunt LC and an ideal transformer. The presence of the transfoFmer opens up the possibility of matching a step impedance: n = R / R This is a substantial improvement over the single passband LC circuit, where, for maximum power transfer condition one must always have: RG=RL. G L' Furthermore, in Fig. l(b) and (d), it is immaterial which side of the circuit the generator is placed at; these circuits may then perform a step-up or a step-down impedance transformation. While not mentioned previously, both Fig. l(a) and (c) circuits are in a Pi-configuration. It follows that for each of these circuits a correspondent Tee-configuration may now be introduced, This is shown in Fig l(e) and (9). The new proposed models are those in Fig. l(f) and (h), respectively: a series LC and an ideal transformer. Again, equivalence between circuits and models may be seen in Table 1. All four options are capable of matching an impedance step and presenting a bandpass shape equivalent to that of an LC. This four topologies set may be extremely useful when matching a complex load [3]. By selecting the right circuit, one is able to look into either port and see any of the four basic elements: shunt C, series C, shunt L or series L. The best configuration for absorbing an specific existent parasitic reactance may then be elected. The matching of microwave transistors, antennas, optical devices -lasers or photodetectorsis a suggested utilization.
一套完整的通带抽头电路及实际应用范围
本文研究了抽头谐振LC电路,以定性和定量的方式确定它们如何偏离先前提出的模型。观察到失配、频移和带宽收缩。建议的实际使用限制。此外,还提供了两个额外的抽头个体,并对其进行了建模,以方便复杂的负载匹配应用。图1 (a)和图1 (c)所示的抽头电容和抽头电感电路具有相同的传递函数。它们有时被称为电容器或电感变压器[1],或并联变压器网络[2]。它们的优点是提供了通带LC电路的选择性,结合了物理变压器的效果。Clarke和Hess[2]提到了上述两种电路,并表明,如果满足某些条件,等效电路可能分别为图1 (b)和图1 (d)。电路元件与模型之间的对应关系见表1。等效电路具有并联LC和理想变压器。传输器的存在开启了匹配阶跃阻抗的可能性:n =R / R这是对单通带LC电路的重大改进,其中,对于最大功率传输条件,必须始终具有:RG=RL。此外,在图1 (b)和(d)中,发电机位于电路的哪一侧无关紧要;然后这些电路可以进行升压或降压阻抗变换。虽然前面没有提到,但图1 (a)和(c)电路都是pi配置。因此,对于这些电路中的每一个,现在可以引入相应的tee配置,如图1 (e)和(9)所示。新提出的模型分别是图1 (f)和(h)中的模型:串联LC和理想变压器。同样,电路和模型之间的等效性可以在表1中看到。所有四个选项都能够匹配阻抗阶跃并呈现与LC等效的带通形状。在匹配复杂的负载[3]时,这四个拓扑集可能非常有用。通过选择正确的电路,可以查看任意一个端口,并看到四种基本元素中的任何一种:分流C,串联C,分流L或串联L。然后可以选择吸收特定存在的寄生电抗的最佳配置。微波晶体管、天线、光学器件-激光或光电探测器的匹配是一个建议的应用。
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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