V.2 No 1

21

Homogeneous 1d resistant line

3. Analysis of excitation transmission process in a resistant elastic line

The parameters R and ficut.gif (844 bytes)r have the main effect on the resistant elastic line vibrations. To analyse them, conveniently use the transfer function of a link Gr by the analogy with electric filters:

(24)

where Gr is the transfer function for resistant elastic lines.

According to (24), the transmission coefficient of each link is proportional to R2 and the delay caused by each link – to 2ficut.gif (844 bytes)r. This process is inherent in the whole frequency range from zero to infinity. At the same time, according to (7)–(9), the transfer function of a link G0 for an ideal line is different in all three bands of betacut.gif (852 bytes)  variation:

(25)

In accordance with (11) and (17), both parameters, ficut.gif (844 bytes)r and taucut.gif (827 bytes), depend on frequency nonlinearly. At r arrow.gif (839 bytes)0 we have ficut.gif (844 bytes)r arrow.gif (839 bytes)taucut.gif (827 bytes), R arrow.gif (839 bytes)1 and Gr arrow.gif (839 bytes)G0. It means that an ideal line reflects the processes occurring in real lines as some approximate model, despite in the general solutions three frequency bands appear. The plots 2ficut.gif (844 bytes)r(omegacut.gif (838 bytes))  and R2(omegacut.gif (838 bytes)), shown in Fig. 1 and Fig. 2 corroborate it.

 

fig1.gif (5833 bytes)

Fig. 1. Delay phase, caused by a member of an elastic line, against the frequency

 

fig2.gif (4598 bytes)

Fig. 2. Attenuation degree R2 caused by a member of line, against the frequency of external affection f , at different resistances r

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