无限衰减固定频率带通滤波器的计算

E. N. Chervinskiy
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To develop of a method for calculating band-pass filters with fixed attenuation poles.Materials and methods. Odd-order filters with an additional capacitor in the transverse branch of the П-link and an inductance in the longitudinal branch of the Т-link were used as low-frequency prototypes of the BPF with attenuation poles. Approximation of the frequency response of a low-frequency prototype (inverse or quasi-elliptical LPF) was performed by methods based on solving systems of nonlinear equations.Results. A realizable transfer function (TF) of an n-th order LPF with attenuation poles was written as the ratio of the product of binomials and a polynomial of power n with real coefficients. Systems of equations were derived to determine amplitude-frequency response coefficients with a given frequency of maximum attenuation interference for both types of filters. 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引用次数: 1

摘要

介绍。在用变频法计算无限衰减频率的带通滤波器时,根据传统公式将原型滤波器的参数重新计算为带通滤波器的参数。使用所选的低通滤波器截止频率和带通滤波器的q因子,可以随意选择一个无限衰减频率(衰减极点)。为了抑制衰减带内的一对具体频率,BPF的合成应首先固定最大衰减频率和滤波器的中心频率。利用变频公式对低频样机的频响参数进行了反向转换。建立一种固定衰减极点带通滤波器的计算方法。材料和方法。在П-link的横向支路上附加电容和Т-link的纵向支路上附加电感的奇阶滤波器被用作带衰减极点的BPF的低频原型。基于非线性方程组的求解方法,对低频原型(逆或准椭圆LPF)的频率响应进行了近似。将具有衰减极点的n阶LPF的可实现传递函数(TF)写成二项与实系数n次多项式的乘积之比。推导了两种滤波器在给定频率下最大衰减干扰的幅频响应系数的方程组。通过调整到中心频率和抑制频率的BPF电路的电容,记录了低频原型的3阶和5阶TF的解析表达式,从而可以直接计算所需的电容。BPF的电感由表示BPF中心频率与电路参数的关系的公式确定,并考虑到文中给出的关系。给出了一个计算10阶拟椭圆型BPF的实例。该方法可直接确定BPF参数,无需中间计算和LPF原型参数的后续转换。给出了第6阶和第10阶П-和Т-shaped bpf频率响应的解析表达式,当用标准值代替计算的电容值时,可以验证所执行的计算并使用电感校正频率响应。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Calculation of Band-Pass Filters with Fixed Frequencies of Infinite Attenuation
Introduction. When calculating band-pass filters (BPF) with infinite attenuation frequencies using the frequency conversion method, the parameters of the prototype – an inverse or quasi-elliptic low-pass filter (LPF) – are recalculated into BPF parameters according to conventional formulas. Using the selected low-pass filter cutoff frequency and the Q-factor of the band-pass filter, one can select at their discretion only one infinite attenuation frequency (attenuation pole). In order to suppress a pair of concrete frequencies in the attenuation band, the synthesis of BPF should initially fix the frequencies of maximum attenuation and the central frequency of the filter. The reverse transition toward the frequency response parameters of a low-frequency prototype is carried out using frequency conversion formulas.Aim. To develop of a method for calculating band-pass filters with fixed attenuation poles.Materials and methods. Odd-order filters with an additional capacitor in the transverse branch of the П-link and an inductance in the longitudinal branch of the Т-link were used as low-frequency prototypes of the BPF with attenuation poles. Approximation of the frequency response of a low-frequency prototype (inverse or quasi-elliptical LPF) was performed by methods based on solving systems of nonlinear equations.Results. A realizable transfer function (TF) of an n-th order LPF with attenuation poles was written as the ratio of the product of binomials and a polynomial of power n with real coefficients. Systems of equations were derived to determine amplitude-frequency response coefficients with a given frequency of maximum attenuation interference for both types of filters. Analytical expressions for the TF of the low frequency prototypes of 3th and 5th orders were recorded through the capacitances of the BPF circuits tuned to the central and suppressed frequencies, thus allowing the desired capacitances to be directly calculated. The BPF inductances were determined by formulas expressing the dependences of the BPF central frequency on the circuits parameters, taking into account the relationships given in the article. An example of calculating a 10th order quasi-elliptic BPF was provided.Conclusion. The proposed method can be used to determine the BPF parameters directly, without an intermediate calculation and subsequent transformation of the LPF prototype parameters. The given analytical expressions for the frequency response of the П- and Т-shaped BPFs of the 6th and 10th orders make it possible to verify the performed calculations and to correct the frequency response using inductances, when replacing the calculated capacitance values with their standard values.
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