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RF Electronics: Design and Simulation

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RF Electronics Chapter 7: RF Filters Page 249 2022, C. J. Kikkert, James Cook University, ISBN 978-0-6486803-9-0. resonator fp = 0.5559*70 MHz = 38.9 MHz. The coupling gap is re-tuned to obtain a difference of 38.9 MHz between the peaks. This corresponds to a coupling gap of 2.5 mm. This procedure is then repeated for all the remaining coupling gaps for the filter using the respective coupling coefficients from tables or equations 4 and 5. Figure 7.62. Circuit for the interdigital filter using calculated loading and coupling values. Simulating this circuit of figure 7.62 gives a filter with a response close to the desired value, as shown in figure 7.63. To obtain the precise desired specification, the filter needs to be optimised. For a lossless Butterworth filter, the coupling gaps are symmetrical. However, for lossy filters or different filter types, asymmetrical coupling gaps result. For a practical Butterworth Bandpass filter, the design procedure can assume a lossless filter. Subsequent optimisation for the desired filter performance, accommodates the losses by; allowing changes in resonator lengths, coupling points and coupling gaps. Note that after optimisation, the resonators in this design are not of equal length and the filter is no longer RF Electronics: Design and Simulation 249 www.cadence.com/go/awr

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