SELF |
40 |
S.B. Karavashkin and O.N. Karavashkina |
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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 / 2).
|
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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