SELF

40

S.B. Karavashkin and O.N. Karavashkina

The input impedance of the filter for which, in case of the load absence at its end, we will write oc is equal:

at the pass band, el <1

(13)

at the stop band, el >1   

(14)

and at the cutoff frequency, el =1

(15)

At the pass band, dependently on 1 and 2 , the impedance Roc can be active, inductive or capacitive. But the main, in any case its amplitude-frequency characteristic will have also n resonances. At the stop band with the frequency growth the input impedance monotonously tends to zero proportionally to ~ 1/el+. And only at the cutoff frequency and at large n the input impedance is approximately equal in its amplitude to the impedance (- 12)1/2. It essentially differs from the results obtained by the two-port method (see, e.g., [4, p. 606]. One more important feature of the presented solutions is that the vibration amplitude of the last filter section (i = n) is not maximal, as we used to think by the analogy with electrical distributed transmission lines. According to (9), it differs by the multiplier  cos el  and diminishes to zero with the vibration frequency approaching to that critical  ( el arrow.gif (839 bytes)picut.gif (836 bytes)/ 2).

 

fig3.gif (5607 bytes)

Fig. 3. The schematic diagram of a finite mechanical elastic line with fixed end (a) and of corresponding ladder filter with shorted output (b)

 

For a ladder filter with the shorted output the situation will be similar. In Fig. 3a we show the model of a finite mechanical line whose nth element is fixed, and in Fig. 3b – the corresponding diagram of an electric ladder filter with the shortened output. Noting [11] and relations (8), we can describe the process in the studied filter by the following system of expressions:

at the pass band of the filter, el <1

(16)

at the stop band, el >1

(17)

at the pass band of the filter, el =1

(18)

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