V.2 No 1

97

Bend effect on vibration pattern

fig11a.gif (6828 bytes)

fig11b.gif (6992 bytes)

fig11c.gif (6980 bytes)

fig11d.gif (6919 bytes)

Fig. 11. The typical diagrams of vibrations in a homogeneous elastic 1D lumped system with respect to the external force momentary phase tetabigcut4cut.gif (853 bytes) and external force inclination angle psi.gif (848 bytes) to the axis x, with the bend angle alphacut.gif (839 bytes) equal to 60° and -60° and with the ratio of transverse stiffness to that longitudinal equal to 2,5

 

In Fig. 11 one of typical patterns of vibration process is shown for the positive and negative bend angles alphacut.gif (839 bytes) dependently on the direction of external force affection. It is visual that with quite small before-the-bend vibration amplitudes, in the bend region there forms a complicated vibration process with the inflections (Fig. 11 b, c), with breaking of the wave process continuity being generally different for the positive and negative bend angles and relating geologically to the charriages, and when excess of the rock strength – to the faults. The wave process amplitude depends essentially on the external excitation frequency and the bend angle. Particularly, in complete correspondence to Haug’s description given in the introduction, the steeper the mountain range inflects and the closer to the normal the front of coming seismic wave is, the faster amplitude grows when passing through the bend.

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