section Shunt sections The image impedances of the shunt section are given by and is the same as that of the constant k section As with the k-type section, the image impedance of the m-type low-pass section is purely real below the cut-off frequency and purely imaginary above it. From the chart it can be seen that in the passband the closest impedance match to a constant pure resistance termination occurs at approximately m = 0.6. Transmission parameters For an m-derived section in general the transmission parameters for a half-section are given by and for n half-sections For the particular example of the low-pass L section, the transmission parameters solve differently in three frequency bands. For the transmission is lossless: For the transmission parameters are For the transmission parameters are Prototype transformations The plots shown of image impedance, attenuation and phase change are the plots of a low-pass prototype filter section. The prototype has a cut-off frequency of ωc = 1 rad/s and a nominal impedance R0 = 1 Ω. This is produced by a filter half-section where L = 1 henry and C = 1 farad. This prototype can be impedance scaled and frequency scaled to the desired values. The low-pass prototype can also be transformed into high-pass, band-pass or band-stop types by application of suitable frequency transformations. Cascading sections Several L half-sections may be cascaded to form a composite filter. Like impedance must always face like in these combinations. There are therefore two circuits that can be formed with two identical L half-sections. Where ZiT faces ZiT, the section is called a Π section. Where ZiΠ faces ZiΠ the section formed is a T section. Further additions of half-sections to either of these forms a ladder network which may start and end with series or shunt elements. It should be born in mind that the characteristics of the filter predicted by the image method are only accurate if the section is terminated with its image impedance. This is usually not true of the sections at either end which are usually terminated with a fixed resistance. The further the section is from the end of the filter, the more accurate the prediction will become since the effects of the terminating impedances are masked by the intervening sections. It is usual to provide half half-sections at the ends of the filter with m = 0.6 as this value gives the