V.2 No 1 |
21 |
Homogeneous 1d resistant line | |
3. Analysis of excitation transmission process in a resistant elastic line The parameters R and 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 2r. 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 variation: |
(25) |
In accordance with (11) and (17), both parameters, r and , depend on frequency nonlinearly. At r 0 we have r , R 1 and Gr 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 2r() and R2(), shown in Fig. 1 and Fig. 2 corroborate it.
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Fig. 1. Delay phase, caused by a member of an elastic line, against the frequency
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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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