V.2 No 1 |
29 |
Homogeneous 1d resistant line | |
?We can trace the same property in the phase velocity dependence on frequency. To find it, substitute (34) into (27). We will yield |
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(40) |
At
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Fig. 6. Phase velocity of wave propagation in a distributed elastic line against the frequency
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Thus, we see that in (40) the main regularities of
resistance affection on vibration process have retained. At the same time, the
regularities describing the main parameters |
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